Set up and interpret each of ThermalOne’s 54 calculations.
Choose a calculation from the sidebar. On a narrow window, use the navigation control to return to the list. Select a process or model before filling its active fields: a disabled field is derived or is not used by that choice.
Results update from the current inputs. Read the fluid, phase and model together with the number. A warning can describe an approximation; an invalid or unresolved calculation instead needs corrected inputs before its result can be used. Defaults are a starting case, not a recommendation for a real machine.
Settings offers SI and US customary units and three to six significant figures. Follow the unit beside each field; changing units converts the number as well as its label. Absolute temperature and a temperature difference are different quantities. Do not enter a Celsius value in a field labelled K.
The significant-figure preference controls reported precision, not solver precision. Slider endpoints are convenient exploration intervals; the property's actual validity domain comes from the selected model and the explanation beside an invalid input.
Export Readings saves the published readings as CSV, including each quantity's unit. Copy Readings supplies tab-separated text for pasting into a spreadsheet. These contain the displayed, rounded values rather than every internal solver value. The Settings option Include the inputs in exported readings controls whether the published input rows are included.
A graph's Export graph menu offers PNG image, PDF document, SVG vector and Copy graph. PNG and the copied graph are raster images; PDF and SVG retain vector paths and text. Export uses the plotted model, axes, units, curves and annotations. A graph is not a replacement for the accompanying assumptions or case record.
On macOS choose a destination in the save panel. On iPadOS use the system share sheet, including Save to Files where available. The app exports calculations; it does not import CSV cases or open document files.
Help contains this Usage Manual and the Theory Manual. Choose a book, use its contents or search for the calculation name. Both books are bundled for offline reading. Settings remembers which book Help opens first.
This book explains tasks and active choices. The Theory Manual explains equations, assumptions, numerical methods and model limits. The symbol tables below are reference fields from the specification; a selected task may replace a generic field with a fluid-state pair, a derived value or a model-specific control.
On macOS, use File > Export Readings and Edit > Copy Readings. On iPadOS, the More menu offers export, copy, both manuals and Settings.
The state table gives pressure, temperature, density, specific volume, internal energy, enthalpy and entropy. Quality appears where it is meaningful. The dome diagram places the selected state in its phase region.
Pressure and temperature on saturation do not determine quality. Choose an independent pair. This entry is water-only, and the IF97 phase and critical-region guards remain applicable.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | Water in 1.0; refrigerants arrive with PE-12. |
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | 273.15 <= T <= 1073.15Regions 1–4; Region 5 remains outside the current water solver. |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | 0.000611657 <= p <= 100.0 |
v | Specific volume: the space one kilogram of the substance occupies. The reciprocal of density, and the property that makes a gas different from a liquid. | m^3/kg | v > 0 |
u | Specific internal energy: the energy stored in one kilogram of a substance by the motion and arrangement of its molecules, with no reference to where the substance is or how fast it is moving. | kJ/kg | — |
h | Specific enthalpy: internal energy plus pressure times specific volume. It exists because that combination appears every time a substance flows across a boundary, so it is a bookkeeping convenience that behaves like a property. | kJ/kg | — |
s | Specific entropy: the property that counts how much of a system's energy is no longer available to do work. It increases in every real process and stays put only in an ideal one. | kJ/(kg K) | — |
x | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | - | 0 <= x <= 1 |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | from the chosen pair |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
v | Specific volume: the space one kilogram of the substance occupies. The reciprocal of density, and the property that makes a gas different from a liquid. | m^3/kg | — |
rho | Density: mass per unit volume, the reciprocal of specific volume. | kg/m^3 | ρ = 1/v |
u | Specific internal energy: the energy stored in one kilogram of a substance by the motion and arrangement of its molecules, with no reference to where the substance is or how fast it is moving. | kJ/kg | — |
h | Specific enthalpy: internal energy plus pressure times specific volume. It exists because that combination appears every time a substance flows across a boundary, so it is a bookkeeping convenience that behaves like a property. | kJ/kg | h = u + pv |
s | Specific entropy: the property that counts how much of a system's energy is no longer available to do work. It increases in every real process and stays put only in an ideal one. | kJ/(kg K) | — |
x | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | - | x=(v-v_f)/v_fg Reported only when strictly between 0 and 1. |
phase | Which region of the phase diagram the state falls in: compressed liquid, saturated mixture, saturated vapour, superheated vapour, or supercritical. | — | One of the five region labels. |
Read the selected model's cp, cv, heat-capacity ratio, energy and entropy properties, then compare the other models at the same state. The two-state entropy result includes both thermal and pressure effects.
Model changes are physical approximations, not unit switches. Reference enthalpies need not match a printed table with another zero. All comparisons stay within the source temperature range.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | Air and the species set carried by the polynomial data. |
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | within the selected species source temperature range |
basis | Whether specific quantities are reported per kilogram or per kilomole. It changes every number on the screen at once. | — | Mass or molar. |
T_cp_evaluation | Temperature at which a constant specific heat is evaluated. | K | Active only for the constant-cp model; within the selected species source range. |
gas_cp_model | Specific-heat law used consistently in the ideal-gas state and inverse calculations. | — | one declared caloric modelVariable cp, constant cp at an evaluation temperature, or cold-air standard (air only). |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | within selected source rangeFirst temperature for entropy change and cp-plot interval. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0First pressure for entropy change. |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | within selected source rangeSecond temperature for entropy change and cp-plot interval. |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0Second pressure for entropy change. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
R | Specific gas constant: the universal gas constant divided by the molar mass of this particular gas. | kJ/(kg K) | R=R̄/M Core value is mass specific; molar basis uses ui.gas_properties_view.value and changes kg to kmol in the unit. |
M | Molar mass: the mass of one kilomole of the substance. For a mixture, the mole-fraction-weighted average. | kg/kmol | — |
cp | Specific heat at constant pressure: how much energy raises one kilogram by one degree while the pressure is held fixed. | kJ/(kg K) | c̄ₚ(T)=R̄(a₁T⁻²+a₂T⁻¹+a₃+a₄T+a₅T²+a₆T³+a₇T⁴) Core value is mass specific; molar basis uses ui.gas_properties_view.value and changes kg to kmol in the unit. |
cv | Specific heat at constant volume: the same question with the volume held fixed instead, which is a smaller number because none of the energy goes into pushing the surroundings back. | kJ/(kg K) | cᵥ=cₚ-R Core value is mass specific; molar basis uses ui.gas_properties_view.value and changes kg to kmol in the unit. |
k | Specific heat ratio: cp divided by cv. It governs how steeply temperature changes when a gas is compressed without heat transfer. | - | k=cₚ/cᵥ |
h | Specific enthalpy: internal energy plus pressure times specific volume. It exists because that combination appears every time a substance flows across a boundary, so it is a bookkeeping convenience that behaves like a property. | kJ/kg | h(T)=∫ cₚ dT Core value is mass specific; molar basis uses ui.gas_properties_view.value and changes kg to kmol in the unit. |
u | Specific internal energy: the energy stored in one kilogram of a substance by the motion and arrangement of its molecules, with no reference to where the substance is or how fast it is moving. | kJ/kg | u=h-RT Core value is mass specific; molar basis uses ui.gas_properties_view.value and changes kg to kmol in the unit. |
s0 | The standard-state entropy function: the part of an ideal gas's entropy that depends only on temperature, with the pressure dependence stripped out and handled separately. | kJ/(kg K) | s°(T)=∫ cₚ/T dT Core value is mass specific; molar basis uses ui.gas_properties_view.value and changes kg to kmol in the unit. |
pr | Relative pressure: a tabulated function of temperature alone whose ratio between two states equals the pressure ratio of an isentropic process between them. A device for avoiding an integral, not a physical pressure. | - | p_r(T)= exp ((s°(T)-s°(T_ref))/R) Normalised to 1 at the reference temperature. Defined only up to a multiplicative constant; every use is a ratio. |
vr | Relative volume: the companion to relative pressure, whose ratio gives the volume ratio of an isentropic process. | - | v_r(T)=(T/T_ref)/(p_r(T)) Same normalisation, same reason. |
specific_entropy_change | Entropy change per unit mass, or per unit amount when molar basis is selected. | kJ/(kg K) | Δ s=s⁰(T₂)-s⁰(T₁)-R ln (p₂/p₁) Specific entropy change, not total entropy. Molar basis multiplies the mass-specific value by molar mass and displays kJ/(kmol K). Core value is mass specific; molar basis uses ui.gas_properties_view.value and changes kg to kmol in the unit. |
Read the IF97 phase, molar volume, reduced coordinates and each available model. Molar volumes use m³/kmol; the table difference is a fraction, while the difference graph uses percent. Each model reports its own root count and resolved stable branch. Unavailable models carry a reason. The logarithmic-pressure graph marks the current IF97 state when it falls inside the interval; PNG, PDF and SVG retain gaps and model colours.
A root choice is not a saturation calculation. Multiple roots can be metastable, and a comparison across unlike phases is not a same-phase accuracy test. Low pressure does not guarantee an ideal gas. The water reference covers 273.15–1073.15 K, excluding Region 5. Branch verification may remain unresolved near critical conditions; no curve is drawn through that gap.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
p_plot_min | Lower pressure of the displayed isotherm interval. | MPa | 0.000611213 <= p_plot_min < p_plot_max <= 100Lower pressure of the displayed isotherm interval. |
p_plot_max | Upper pressure of the displayed isotherm interval. | MPa | 0.000611213 <= p_plot_min < p_plot_max <= 100Upper pressure of the displayed isotherm interval. |
root | Candidate outer branch selected independently for each EOS. | - | largest root: vapour, smallest root: liquidCandidate outer branch selected independently for each EOS. |
plot_quantity | Quantity on the common isotherm chart. | - | compressibility, relative volume differenceQuantity on the common isotherm chart. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Z | Compressibility factor: how far the substance departs from ideal-gas behaviour, expressed as the ratio of its actual specific volume to the ideal-gas value at the same temperature and pressure. | - | Z=pv/RT |
v | Specific volume: the space one kilogram of the substance occupies. The reciprocal of density, and the property that makes a gas different from a liquid. | m^3/kmol | Molar basis, matching the universal gas constant used by the cubic relations. |
TR | Reduced temperature: temperature as a fraction of the critical temperature. | - | T_R=T/T_c |
pR | Reduced pressure: pressure as a fraction of the critical pressure. | - | p_R=p/p_c |
vR_pseudo | Pseudo-reduced specific volume: a dimensionless volume built from the critical constants, used so a volume can be entered on a chart drawn in reduced coordinates. | - | v_R'=v p_c/(RT_c) |
error_vs_reference | How far the chosen model sits from the reference formulation at this state, so the model's accuracy is a number rather than a claim. | - | Relative molar-volume difference from IF97: table values are fractions; the relative-difference chart uses percent. |
phase | Which region of the phase diagram the state falls in: compressed liquid, saturated mixture, saturated vapour, superheated vapour, or supercritical. | - | IF97 reference phase. |
root_count | Per-model root counts or Lee–Kesler fitted-fluid crossing count; counts do not establish phase coexistence. | - | Per-model root counts or Lee–Kesler fitted-fluid crossing count; counts do not establish phase coexistence. |
branch_status | Resolved per-model candidate branch and reasons for unavailable comparisons. | - | Resolved per-model candidate branch and reasons for unavailable comparisons. |
Each endpoint has a departure correction and fugacity coefficient. The reported real-gas property change is the ideal-gas change plus outlet departure minus inlet departure.
The native entry uses the gas root. Departure corrections are state-property corrections; they do not determine heat or work without a process balance.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | Selected species supplies its critical constants and acentric factor; these are not editable inputs. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
model | Which equation of state the screen is evaluating. | — | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
dh_departure | How much the real enthalpy differs from the ideal-gas enthalpy at the same temperature. | kJ/kg | — |
ds_departure | How much the real entropy differs from the ideal-gas entropy at the same temperature and pressure. | kJ/(kg K) | — |
DeltaH | Change in total enthalpy between the two states. | kJ/kg | — |
DeltaS | Change in total entropy between the two states. | kJ/(kg K) | — |
phi_fug | Fugacity coefficient: the factor by which a real gas's escaping tendency differs from its pressure. One for an ideal gas. | - | ln φ=∫₀^p(Z-1)/p dp |
Depending on the selection, results compare Maxwell relations, cp−cv, expansion/compressibility, Joule–Thomson response, speed of sound or Clapeyron slopes and latent heat from two routes.
A derivative identity can be exact for an approximate equation of state. Near critical or phase boundaries, undefined derivatives and poorly conditioned differences must not be read as zero.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
relation | Which of the property relations the screen is evaluating. | — | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
beta_v | Volume expansivity: the fractional change in volume per degree of temperature rise at constant pressure. | 1/K | β=(1/v)(∂ v/(∂ T))ₚ |
kappa_T | Isothermal compressibility: the fractional reduction in volume per unit pressure rise at constant temperature. | 1/MPa | κ=-(1/v)(∂ v/(∂ p))_T |
cp_minus_cv | The gap between the two specific heats, which for a real substance depends on how much it expands when heated and how much it resists being squeezed. | kJ/(kg K) | cₚ-cᵥ=vTβ²/κ |
mu_JT | Joule-Thomson coefficient: how much the temperature changes per unit pressure drop in a throttling process. Its sign decides whether throttling cools or warms, and refrigeration only works where it is positive. | K/MPa | Kernel returns K/kPa; presentation multiplies by 1000. |
dpdT_sat | The slope of the saturation line on the pressure-temperature plane. | MPa/K | Kernel Clapeyron slope with kJ/kg is kPa/K; presentation divides by 1000. |
hfg | Latent enthalpy: the energy one kilogram absorbs turning from saturated liquid into saturated vapour at fixed temperature. | kJ/kg | h_fg=T v_fg(dp/(dT))_sat |
c_sound | Speed of sound in the substance at this state. | m/s | — |
Mixture properties include molecular mass, gas constant, cp, cv, heat-capacity ratio, fractions and partial pressures. Mixing adds outlet temperature and total entropy production split into thermal, composition and pressure contributions.
The mixer has no heat, shaft work or kinetic-energy change. Nonpositive/nonfinite pressure or a negative total entropy balance is refused. Positive entropy alone does not solve momentum or establish mixer geometry.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
composition1 | The make-up of the mixture, as fractions of its components. | - | First stream or property-state composition; proportional nonnegative amounts are normalised. |
composition2 | The make-up of the mixture, as fractions of its components. | - | Second stream composition in mixing mode. |
basis | Whether specific quantities are reported per kilogram or per kilomole. It changes every number on the screen at once. | - | mole fractions, mass fractionsControls composition fractions only; both entered stream flows remain molar. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | First stream or property-state temperature. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | First stream or property-state pressure. |
ndot1 | Molar flow: amount of substance passing a section per unit time. | kmol/s | positive finiteFirst inlet molar flow; active in mixing mode. |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Second inlet temperature. |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Second inlet pressure. |
ndot2 | Molar flow: amount of substance passing a section per unit time. | kmol/s | positive finiteSecond inlet molar flow; active in mixing mode. |
p3 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Outlet mixing pressure; momentum is not solved. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
M | Molar mass: the mass of one kilomole of the substance. For a mixture, the mole-fraction-weighted average. | kg/kmol | M=Σ yᵢMᵢ |
R | Specific gas constant: the universal gas constant divided by the molar mass of this particular gas. | kJ/(kg K) | — |
cp | Specific heat at constant pressure: how much energy raises one kilogram by one degree while the pressure is held fixed. | kJ/(kg K) | — |
cv | Specific heat at constant volume: the same question with the volume held fixed instead, which is a smaller number because none of the energy goes into pushing the surroundings back. | kJ/(kg K) | — |
k | Specific heat ratio: cp divided by cv. It governs how steeply temperature changes when a gas is compressed without heat transfer. | - | — |
p_partial | Partial pressure: the pressure one component of a mixture would exert if it alone occupied the whole volume. | MPa | pᵢ=yᵢp Same pressure unit as the input, before the display-unit conversion. |
DeltaS_mixing | The entropy created purely by letting distinct species share a volume, with no temperature or pressure change involved. Forgetting it is the classic mixture error. | kJ/(kg K) | -(R̄/M)Σᵢ yᵢ ln yᵢ Displayed mass-specific entropy of mixing; the raw kernel identity is per kmol and is divided by apparent molar mass. |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
sigmadot | Rate of entropy production. | kW/K | Total = thermal + composition + pressure contributions, each in kW/K. Pressure changes can contribute negatively; the total must satisfy the second law. The mixer does not solve momentum. |
ndot | Molar flow: amount of substance passing a section per unit time. | kmol/s | Total outlet molar flow; sum of the inlet molar flows. |
sigma_thermal | Thermal contribution to the entropy-production rate. | kW/K | Thermal contribution to the entropy-production rate. |
sigma_composition | Composition contribution to the entropy-production rate. | kW/K | Composition contribution to the entropy-production rate. |
sigma_pressure | Pressure contribution to entropy rate; it may be negative while the total remains nonnegative. | kW/K | Pressure contribution to entropy rate; it may be negative while the total remains nonnegative. |
The account gives liquid yield, work per feed and liquid mass, recovered expander work, minimum work, figure of merit, heat rejection, entropy production and energy closures. Recuperator diagrams show sampled minimum approaches.
Nitrogen and methane use Helmholtz models at every station; CO2 retains its labelled cubic model. All states, including compressor discharge, must remain within the model range. The expander must stay dry. The PR inversion diagnostic is a separate model comparison for cryogenic cases.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | CO2, N2, CH4CO2 uses the cubic/NASA model; N2 and CH4 use their cryogenic Helmholtz models. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Fresh-feed and aftercooler temperature; actual compressor suction follows return mixing. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | 0 < p_low < p_highCommon low pressure of feed, separator and return. |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | 0 < p_low < p_highCompressor discharge and high-pressure heat-exchanger pressure; not station 2 pressure. |
eta_reg | Regenerator effectiveness: how much of the available temperature rise the regenerator actually delivers. | - | 0 < eta_reg <= 1Linde uses one recuperator; Claude adds a positive expander split and a second recuperator. Warm-end enthalpy approach applies to the entire Linde recuperator but only the warm Claude recuperator. At a fixed approach below one, zero split is not a continuous cross-arrangement limit. |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | 0 < eta_c <= 1Adiabatic isentropic efficiency from the actual mixed suction state; not the legacy ideal isothermal work estimate. |
alpha_split | Fraction of compressed feed sent through the work-producing expander. | - | 0 < alpha_split < 1 for Claude; zero for LindeFraction of feed through the expander. |
T_split | Temperature where the high-pressure flow divides between the expander and cold recuperator. | K | T_sat_low < T_split < T_supplyHigh-pressure split-point temperature for Claude. |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | 0 < eta_t <= 1Dry-expander isentropic efficiency. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
y_liquid | Liquid yield: the fraction of the gas processed that comes out as liquid. Small, and seeing how small is the point. | - | Liquid production divided by compressor circulation; the fresh make-up fraction equals this yield at steady state. Single-species molar and mass fractions agree. |
w_specific | Work required per unit mass of product, which for liquefaction is per kilogram of liquid actually made rather than per kilogram processed. | kJ/kg | Net input work per kg liquid product. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
w_min_liquid | Reversible minimum work per kg liquid product. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. | kJ/kg | Reversible minimum work per kg liquid product. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
beta | Coefficient of performance of a refrigerator: heat removed from the cold space divided by the work it cost. Routinely greater than one, which is why it is not called an efficiency. | - | Minimum work divided by actual net work on the same liquid basis. |
w_feed | Net input work per kg feed. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. | kJ/kg | Net input work per kg compressor circulation. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
w_compressor | Compressor work per kg feed. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. | kJ/kg | Compressor work per kg compressor circulation. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
w_expander | Recovered expander work per kg feed; the flow-split factor is already included. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. | kJ/kg | Recovered expander work per kg compressor circulation; the flow-split factor is already included. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
q_aftercooler | Aftercooler heat rejection per kg feed. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. | kJ/kg | Aftercooler heat rejection per kg compressor circulation. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
closure_feed | Whole-process energy residual per kg feed. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. | kJ/kg | Whole-process energy residual per kg compressor circulation. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
cold_box_closure | Cold-box energy residual per kg feed. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. | kJ/kg | Cold-box energy residual per kg compressor circulation. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
s_gen_feed | Whole-process entropy generation per kg feed and kelvin. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. | kJ/(kg K) | Whole-process entropy generation per kg compressor circulation and kelvin. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
s_mix_feed | Return-mixing entropy generation per kg feed and kelvin. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. | kJ/(kg K) | Return-mixing entropy generation per kg compressor circulation and kelvin. Raw result is molar; ui.liquefaction_view.per_mass divides by the selected molar mass before display. |
T_inversion | The temperature above which throttling warms the gas instead of cooling it, so simple liquefaction stops working. | K | Independent warm-gas Peng–Robinson/NASA diagnostic; not the N2/CH4 Helmholtz cycle inversion locus. |
flow_fraction | Each station flow divided by fresh compressor-feed basis. | - | Each station flow divided by compressor circulation (station 2 flow = 1); fresh make-up at station 1 equals liquid yield, not unity. |
sampled_approach | Minimum computed temperature difference at sampled heat fractions. | K | Minimum of 65 recuperator heat-load samples; temperature difference, not absolute temperature or a continuous certificate. |
Cascade results retain separate loop flows, powers, diagrams and exchanger entropy generation. Flash staging reports high/low-stage flows and powers, flash fraction, staged versus single-stage COP and energy closure.
The cascade exchanger couples loop heat duties but does not mix their fluids. Intermediate temperature and intermediate pressure belong to different arrangements and are not interchangeable controls.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
pi | Intermediate pressure between two stages. | MPa | Intermediate pressure. |
DeltaT_cascade | The temperature overlap in the exchanger that couples two refrigeration loops. | K | Temperature overlap in the cascade exchanger. |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | — |
Qdot_L | Rate of heat removed from the cold side, which is the useful output of a refrigerator. | kW | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
beta | Coefficient of performance of a refrigerator: heat removed from the cold space divided by the work it cost. Routinely greater than one, which is why it is not called an efficiency. | - | — |
Wdot | Rate of work transfer, that is, power. | kW | — |
pi_opt | The intermediate pressure that minimises total work, which for two ideal stages is the geometric mean of the end pressures. | MPa | Flash staging optimises intermediate pressure. The separate-loop route instead optimises the exchanger midpoint temperature, with the chosen temperature approach held fixed. |
mdot | Mass flow rate. | kg/s | Flash core flows are kmol/s and are multiplied by the selected molar mass at the display boundary. Separate-loop outputs are kg/s for each fluid independently. |
The balance reports theoretical and supplied oxygen, air/fuel ratios, reactant/product coefficients and atom/mass closure. Conventional and model-consistent mass air/fuel ratios are labelled separately.
Custom atom counts define stoichiometry, not an invented heating value for an unknown fuel. Complete oxidation refuses oxygen-deficient conditions; it does not add soot or dissociation automatically.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
fuel | Which fuel is being burned. | — | — |
a_C | Number of carbon atoms in one molecule of the fuel. | - | — |
b_H | Number of hydrogen atoms in one molecule of the fuel. | - | — |
c_O | Number of oxygen atoms already in one molecule of the fuel. | - | — |
d_N | Number of nitrogen atoms in one molecule of the fuel. | - | — |
e_S | Number of sulphur atoms in one molecule of the fuel. | - | — |
pct_theo_air | How much air was supplied as a percentage of exactly enough. A hundred per cent means exactly enough. | - | — |
phi_eq | Equivalence ratio: how much fuel is present relative to exactly enough. One means exactly enough, above one means rich. | - | 0 < phi_eq <= 1 |
AF | Air-fuel ratio on a mass basis: kilograms of air supplied per kilogram of fuel. | - | — |
omega | Humidity ratio: kilograms of water vapour carried per kilogram of dry air. The quantity that stays fixed when moist air is merely heated or cooled. | - | Humidity ratio of the combustion air, when moist air is used. |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | positive product pressurePressure for the product-water dew-point calculation; does not change stoichiometric coefficients. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
alpha_stoich | Moles of oxygen needed to burn one mole of the fuel completely with none left over. | - | — |
AF | Air-fuel ratio on a mass basis: kilograms of air supplied per kilogram of fuel. | - | AF=AF̄ M_air/M_fuel |
AF_molar | The same ratio counted in moles instead of kilograms. | - | — |
phi_eq | Equivalence ratio: how much fuel is present relative to exactly enough. One means exactly enough, above one means rich. | - | — |
pct_theo_air | How much air was supplied as a percentage of exactly enough. A hundred per cent means exactly enough. | - | — |
products | The species and amounts the reaction produces. | — | — |
Tdp | Dew point: the temperature at which the air being cooled would start to condense. | K | Below this the water in the exhaust condenses, which is what limits stack temperature in a real plant. |
The inversion recovers fuel carbon/hydrogen scale, air/fuel measures, water formed and oxygen residual. Condition measures identify which recovered quantity is most sensitive to the stated reading model.
The model is a carbon/hydrogen fuel with four dry species. Without a supplied molecular scale, C=1 is an empirical formula unit. Sensitivity is not a statistical confidence interval.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
y_CO2 | Mole fraction of carbon dioxide in the dry product gas. | - | 0 <= y_CO2 <= 1Mole-fraction mode requires sum 1 within 0.002. Relative amounts have a separate explicit input mode. Nitrogen may be the remainder only when the four dry species are exhaustive. |
y_CO | Mole fraction of carbon monoxide in the dry product gas, which is what incomplete combustion leaves behind. | - | 0 <= y_CO <= 1Mole-fraction mode requires sum 1 within 0.002. Relative amounts have a separate explicit input mode. Nitrogen may be the remainder only when the four dry species are exhaustive. |
y_O2 | Mole fraction of oxygen in the dry product gas, which is what excess air leaves behind. | - | 0 <= y_O2 <= 1Mole-fraction mode requires sum 1 within 0.002. Relative amounts have a separate explicit input mode. Nitrogen may be the remainder only when the four dry species are exhaustive. |
y_N2 | Mole fraction of nitrogen in the dry product gas. | - | 0 <= y_N2 <= 1Mole-fraction mode requires sum 1 within 0.002. Relative amounts have a separate explicit input mode. Nitrogen may be the remainder only when the four dry species are exhaustive. |
fuel | Which fuel is being burned. | — | — |
AF | Air-fuel ratio on a mass basis: kilograms of air supplied per kilogram of fuel. | - | AF > 0Known mode: molar dry-air amount per mole of fuel, not a mass ratio. |
a_C | Number of carbon atoms in one molecule of the fuel. | - | a_C > 0Known-fuel carbon count. |
b_H | Number of hydrogen atoms in one molecule of the fuel. | - | b_H >= 0Known-fuel hydrogen count. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
AF | Air-fuel ratio on a mass basis: kilograms of air supplied per kilogram of fuel. | - | — |
phi_eq | Equivalence ratio: how much fuel is present relative to exactly enough. One means exactly enough, above one means rich. | - | — |
a_C | Number of carbon atoms in one molecule of the fuel. | - | — |
b_H | Number of hydrogen atoms in one molecule of the fuel. | - | — |
pct_theo_air | How much air was supplied as a percentage of exactly enough. A hundred per cent means exactly enough. | - | — |
The account gives heat per fuel amount and per fuel mass, product-minus-reactant enthalpy/internal energy and a cancellation indicator. Standard HHV/LHV retain their declared reference-water convention.
Negative heat means heat released by the system. A selected liquid-water outlet is a specified separated phase, not an equilibrium condensate amount. Heating values are not the actual process duty at arbitrary temperatures.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
fuel | Which fuel is being burned. | — | — |
pct_theo_air | How much air was supplied as a percentage of exactly enough. A hundred per cent means exactly enough. | - | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Reactant temperature. |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Product temperature. |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
W | Work transferred across the boundary, taken as positive when it comes out of the system. | kJ/kmol | Positive work out per kmol of fuel; non-boundary work in a rigid vessel. |
T_liquid | Temperature of the specified separate liquid-water phase. | K | 273.15 <= T_liquid <= 623.15Liquid product-water model envelope. Also requires p >= psat(T), p <= 100 MPa. Gas properties remain ideal-gas NASA data. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Qdot_per_fuel | Heat transferred per kilomole of fuel burned. | kJ/kmol | — |
hRP | Enthalpy of combustion: the difference between product and reactant enthalpies at the same temperature and pressure. | kJ/kmol | h̄_RP=Σ_P n_eh̄_e-Σ_R n_ih̄_i Standard gas-phase reference, including water as vapor, independent of the selected product phase. |
HHV | Higher heating value: energy released per kilogram of fuel with the product water counted as liquid. | kJ/kg | Water in the products taken as liquid. |
LHV | Lower heating value: the same with the water counted as vapour. Smaller, and quoting the wrong one is a common way to overstate an efficiency. | kJ/kg | Water in the products taken as vapour. |
hf0 | Enthalpy of formation: the energy bookkeeping entry that lets substances of different chemical identity be added together. Zero by convention for a stable element in its reference form. | kJ/kmol | Standard gas-phase reference, including water as vapor, independent of the selected product phase. |
The entry reports selected adiabatic temperature, energy residual, frozen and two-dissociation temperatures and the associated product amounts. Their difference shows the energy absorbed by the modeled dissociation.
This entry's dissociation set includes CO2 and H2O reactions only. Use the separate equilibrium-flame task for the larger radical/NO libraries; neither model predicts finite-rate emissions.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
fuel | Which fuel is being burned. | — | — |
pct_theo_air | How much air was supplied as a percentage of exactly enough. A hundred per cent means exactly enough. | - | Native air input. Equivalence ratio is its reciprocal convention, 100 divided by this percentage; it is not a separate editable input. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Reactant temperature, including any preheat. |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
omega | Humidity ratio: kilograms of water vapour carried per kilogram of dry air. The quantity that stays fixed when moist air is merely heated or cooled. | - | Humidity of the combustion air. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
T_ad | Adiabatic flame temperature: how hot the products get when none of the released energy is allowed to leave. | K | — |
products | The species and amounts the reaction produces. | — | — |
residual | How far from zero the energy balance still is at the returned root. Reported rather than assumed, so convergence is visible. | kJ/kmol | The residual at the returned root, reported so convergence is visible rather than asserted. |
The selected system reports phase-equilibrium quantities, degrees of freedom and its phase diagram. Binary results show liquid/vapour composition under the stated ideal-solution approximation; osmosis shows the logarithmic solvent-activity result.
Binary equilibrium uses pure-component saturation plus Raoult/Dalton assumptions, not a general nonideal cubic-mixture flash. The dilute osmotic expression is a comparison, not the main formula at concentrated composition.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
components | Which species are present. | — | — |
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | T > 0 within the selected property modelBinary saturation uses mechanical PR roots, independent of caloric polynomial bounds. Pure water uses IF97; four refrigerants use Helmholtz; CO2 uses PR. |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0Pressure is input for binary bubble/dew modes; pure coexistence computes pressure from temperature. |
composition | The make-up of the mixture, as fractions of its components. | — | 0 <= composition <= 1First-component liquid mole fraction, or vapor fraction in dew mode. Pure endpoints ignore the absent component. |
nphase | How many phases coexist. | - | nphase = 2Two coexisting bulk phases in pure and binary modes; the membrane constraint is not counted by the free bulk phase rule. |
solvent_fraction | Mole fraction of solvent in the ideal solution. | — | 0 < solvent_fraction <= 1Solvent mole fraction in the ideal solution. |
solvent_molar_volume | Constant partial molar volume of solvent used to convert a chemical-potential difference to osmotic pressure. | m³/kmol | solvent_molar_volume > 0Constant solvent partial molar volume in the membrane model. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
F_dof | Degrees of freedom: how many properties can still be chosen freely once the phases and components are fixed. | - | F=2+N-P One for pure coexistence, two for a binary with two independent components; the freely exchanging bulk phase rule does not apply to the selective membrane. |
composition | The make-up of the mixture, as fractions of its components. | — | — |
T_bubble | The temperature at which the first bubble of vapour appears in a liquid mixture being heated. | K | — |
T_dew | The temperature at which the first drop of liquid appears in a vapour mixture being cooled. | K | — |
pi_osmotic | Osmotic pressure: the pressure that has to be applied to a solution to stop pure solvent flowing into it through a membrane. | MPa | — |
The coupled energy/equilibrium solution gives flame temperature, temperature reduction, product amounts and scaled residuals. The library comparison exposes the effect of adding radical species and NO.
The base library has six gases; expanded sets add radicals and then NO. The temperature and air-supply ranges remain explicit. Equilibrium NO is not a finite-residence-time emissions prediction.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
fuel | Which fuel is being burned. | — | — |
pct_theo_air | How much air was supplied as a percentage of exactly enough. A hundred per cent means exactly enough. | - | at least 100%; fuel-rich product chemistry is outside this libraryNative air input. Equivalence ratio is its reciprocal convention, 100 divided by this percentage; it is not a separate editable input. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0 |
species_set | Which dissociation products are being allowed into the equilibrium calculation. | — | Six molecular species; add H, O, OH and N; then add NO. Species with absent elements are deleted exactly. |
omega | Humidity ratio: kilograms of water vapour carried per kilogram of dry air. The quantity that stays fixed when moist air is merely heated or cooled. | - | finite omega >= 0Water mass per dry-air mass carried with the reactants; used by selected and comparison flame calculations. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
T_ad | Adiabatic flame temperature: how hot the products get when none of the released energy is allowed to leave. | K | — |
composition | The make-up of the mixture, as fractions of its components. | — | — |
T_gap | How much lower the flame temperature is once dissociation is accounted for. The whole point of running the equilibrium calculation. | ΔK | Difference from the complete-combustion answer. This is the number the screen exists to produce. |
residual | How far from zero the energy balance still is at the returned root. Reported rather than assumed, so convergence is visible. | kJ/kmol | — |
Results identify equilibrium amounts, gas fractions when gas exists, reaction extents or diagnostics, conservation residuals and phase status. Pressure exploration uses the same inventory and thermochemical assumptions as the selected state.
Enter ln K, not K, and retain the stated dimensionless pressure standard. Available thermochemical data constrain species and temperature. A zero gas amount or exhausted pure phase can require a different active phase set; an unsupported or unresolved system is refused.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
reaction | Which reaction the equilibrium is being computed for. | — | Choose a library or declare species and an arbitrary independent signed reaction matrix. Decimal/fraction coefficients are preserved exactly; every element and charge must balance. |
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | T>0 in given-lnK mode; thermochemical mode uses the valid ranges of participating records, including the pure-water IF97 pressure restriction. |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0; declared pure liquid water with nonzero inventory or participation also requires IF97 region 1 at T,pUser-defined pressure slider explores 0.001 to 10 MPa logarithmically. This is an exploration interval, not a validity limit; typed values remain subject to phase and model checks. |
n_initial | How much of each species is present before the reaction proceeds. | kmol | non-negative finite amounts with nonzero totalCO2, CO, H2O vapor, H2, O2, N2 and pure H2O liquid; omitted species mean zero. Atomic mode accepts H, N, O, Ar, Na, Cs with each singly charged ion and electrons; initial total charge must be zero. User-defined mode accepts declared species with explicit integer element counts, charge and phase; total initial charge must be zero. |
inert | Species present that take no part in the reaction but dilute the mixture, which shifts the equilibrium anyway. | — | Any species excluded from all supplied reactions remains chemically frozen, even if its elements occur in reactive species. |
lnK_given | User-supplied natural logarithm of the equilibrium constant at the current temperature and 1 atm standard state. | — | finite natural-log constants, one per active atom or written user-defined reactionGiven at the entered temperature and 1 atm standard state; does not specify reaction enthalpy or temperature dependence. |
nu_matrix | Exact signed reaction coefficients; zero entries exclude a species from a reaction. | — | explicit user-defined systemExact signed reaction coefficients; zero entries exclude a species from a reaction. |
species_atoms | Positive integer count of each declared element in one species. | — | explicit user-defined systemPositive integer count of each declared element in one species. |
species_charge | Signed integer electric charge of one species. | — | explicit user-defined systemSigned integer electric charge of one species. |
species_phase | Ideal gas or a separate pure condensed phase with unit activity. | — | explicit user-defined systemIdeal gas or a separate pure condensed phase with unit activity. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
lnK | The logarithm of the equilibrium constant. The app works in this throughout because the constant itself spans about forty decades. | - | ln K=-Δ G°/(R̄T) Gas standard-state K depends on T; effective condensation K includes actual-pressure liquid Gibbs and therefore depends on T and p. |
K_eq | Equilibrium constant: how far the reaction goes at this temperature. Shown for reading only, never used as an intermediate. | - | Display only; unavailable when exp(lnK) cannot retain six significant digits. Never used in the solver. |
epsilon_ext | Extent of reaction: how far the reaction has actually proceeded, from none of it to all of it. | kmol | Signed extent in each written reaction coordinate; inverse rows favor smaller inventory scales. An unresolved near-zero extent is unavailable, not a false exact zero. |
composition | The make-up of the mixture, as fractions of its components. | — | — |
dH_reaction | Energy absorbed or released by the reaction, which is what decides whether heating pushes it forwards or backwards. | kJ/kmol | Computed only from matching thermochemical records; given-lnK mode does not invent reaction heat. |
n_e | Amount of free electrons, included as a gas species in charge and mole balances. | kmol | Common electron inventory, included in total gas moles and partial pressures. |
z_ion | Fraction of a conserved atom inventory present as singly charged ions. | — | Ionized fraction for each conserved atom inventory. |
Electrical power and reaction-consumed fuel flow accompany heat transfer, reversible voltage and work. The detailed account separates energy, stream/heat exergy, incoming resources, destruction and closure.
A fuel cell is not bounded by a heat engine's efficiency alone. Operating voltage, reaction direction and heat sign must be consistent; current denotes reaction consumption in this model, not a separate utilization or stack-loss model.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
fuel | Which fuel is being burned. | — | Hydrogen for PEM; H2, CO or CH4 net-reaction bounds for solid oxide. Pure oxygen supply; no reforming or polarization model. |
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | 200 <= T <= 6000 for gas products; liquid-water model requires IF97 R1Mathematical property range, not an electrode or membrane operating specification. |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0Common pure fuel / pure oxygen / mixed-product stream pressure; liquid product feasibility checked with T. |
n_electrons | How many electrons move per mole of fuel in the cell reaction. | - | Derived from the selected oxidation reaction: 2 for H2/CO, 8 for CH4; displayed, not arbitrarily editable. |
V_operating | The voltage the cell is actually running at, which is always below the reversible value. | V | 0 <= V_operating <= EcellFour ULPs only accommodate representational roundoff at the reversible boundary. |
current | Current drawn from the cell. | A | current >= 0Total cell current. Unity fuel utilization and Faradaic efficiency; zero current returns zero power and consumed flow. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Ecell | Reversible cell voltage: the most a fuel cell can produce before any losses, set by the Gibbs function change and the charge moved. | V | E=-Δḡ/(nF) |
Wmax | The most work obtainable from a reaction, which is set by the Gibbs function change rather than by the energy released. | kJ/kmol | Wₘₐₓ=-Δḡ |
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | — |
epsilon | Exergetic efficiency: what the component actually delivered as a fraction of the exergy it was given. It asks a harder question than thermal efficiency and usually gets a worse answer. | - | Electrical work divided by all incoming exergy resources: positive fuel/oxygen/heat terms plus negative outlet-stream exergy. Distinct from voltage efficiency V/E. |
Qdot | Rate of heat transfer. | kW | Positive heat rejection; negative when heat is absorbed. Current converts per-fuel heat to a rate. |
The account separates inlet exergy, product-stream exergy and destruction, with heat, entropy production and rates. It also shows incoming-fuel exergy and the internally consistent alternative water reference.
All streams must use the same chemical reference. The unselected water-endpoint difference reflects reference-model consistency and printed conventions, not an additional recoverable energy term.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
fuel | Which fuel is being burned. | — | — |
pct_theo_air | How much air was supplied as a percentage of exactly enough. A hundred per cent means exactly enough. | - | — |
T0 | Dead-state temperature: the temperature of the environment the system is eventually going to equilibrate with. Exergy is meaningless without it. | K | 200 <= T0 <= 6000 in custom gas mode; standard models fix 298.15 KCustom liquid-water route additionally requires an IF97 R1 liquid state and non-condensing reference vapor. |
p0 | Dead-state pressure: the pressure of that same environment. | MPa | p0 > 0 for custom gas modeStandard Model I fixes 0.103250175 MPa; Model II fixes 0.101325 MPa. Fixed reference values are displayed, not silently overridden. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
environment_model | Which published reference environment the chemical exergies are computed against. Two are in common use and they do not agree. | — | Model I, Model II, or the explicitly separate fixed-composition custom gas environment. |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0Common fuel, air and product process pressure; independent of reference pressure. |
ndot | Molar flow: amount of substance passing a section per unit time. | kmol/s | ndot > 0Molar fuel flow; multiplies per-kmol entropy generation to obtain kW/K. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
sigmadot | Rate of entropy production. | kW/K | — |
sbar0 | Absolute entropy: entropy measured from the third-law zero rather than from an arbitrary datum, which is what reacting systems require. | kJ/(kmol K) | Absolute entropy of the pure fuel at its actual inlet T,p, per kmol. |
ech | Chemical exergy: the work still obtainable from a substance once it is at the environment's temperature and pressure but not yet at its composition. | kJ/kmol | — |
e_total | Total exergy of a substance, thermomechanical plus chemical. | kJ/kg | e=(u-u₀)+p₀(v-v₀)-T₀(s-s₀)+V²/2+gz+e^ch Pure incoming fuel at actual inlet T,p, per fuel mass, with zero kinetic and potential terms. |
ef_total | Total flow exergy, thermomechanical plus chemical. | kJ/kg | Pure incoming fuel at actual inlet T,p, per fuel mass, with zero kinetic and potential terms. |
epsilon | Exergetic efficiency: what the component actually delivered as a fraction of the exergy it was given. It asks a harder question than thermal efficiency and usually gets a worse answer. | - | All outlet-stream exergy / total fuel-plus-air inlet exergy. This is a retained-exergy ratio, not a definition of useful product efficiency. |
Ed | Exergy destroyed: work potential that was permanently lost, equal to the dead-state temperature times the entropy produced. | kJ/kmol | — |
The result includes final temperature/pressure, total and per-fuel heat, initial fuel amount/mass, mole ratio, temperature ratio and energy residual. The pressure change includes both temperature and reaction mole-count changes.
The vessel model keeps frozen gaseous products. Below the water dew point it is a hypothetical vapour reference, and at high temperature dissociation can change the actual pressure and temperature.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
fuel | Which fuel is being burned. | — | — |
pct_theo_air | How much air was supplied as a percentage of exactly enough. A hundred per cent means exactly enough. | - | — |
V | Volume: the space the whole system occupies, as opposed to the space one kilogram of it occupies. | m^3 | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
Q | Heat transferred across the boundary, taken as positive when it goes into the system. | kJ | Heat into the entire charge in specified-heat mode; zero is adiabatic. In specified-final-temperature mode heat is an output. |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | within selected product property rangeFinal temperature when the specified-final-state mode is selected; otherwise recovered from full-charge heat. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
Qv | Heat released by a reaction carried out at constant volume rather than constant pressure. | kJ/kmol | — |
uRP | The same quantity on an internal energy basis, which is what a constant-volume reaction needs. | kJ/kmol | — |
The complete charging account compares stored energy/exergy, incoming-stream exergy and entropy generation with capacity and duration constraints. Histories show charging evolution and the selected optimum.
Sensible storage begins at ambient temperature. Latent storage stays at the entered melting temperature and does not include a warm-up from ambient. Best time or temperature maximises stored exergy divided by incoming-stream exergy, not stored exergy alone. The entropy account distinguishes heat-exchanger production from disposal of the outlet stream. Latent operation is limited by finite capacity; inputs beyond exhaustion are refused.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | T > T0 > 0Source stream inlet. |
T0 | Dead-state temperature: the temperature of the environment the system is eventually going to equilibrate with. Exergy is meaningless without it. | K | 0 < T0 < T |
mdot | Mass flow rate. | kg/s | mdot > 0Mass flow of charging stream. |
cp | Specific heat at constant pressure: how much energy raises one kilogram by one degree while the pressure is held fixed. | kJ/(kg K) | cp > 0Constant specific heat of charging stream. |
UA_store | Conductance between the charging stream and the store. | kW/K | UA_store > 0 |
t_charge | How long the store is charged for. | s | t_charge > 0Finite entered charging duration; latent charge must fit the available latent heat. |
T_store | Temperature the store is held at. | K | T0 < T_store < TLatent melting temperature. Sensible store begins at ambient and its temperature evolves. |
storage_kind | Whether the store works by rising in temperature or by melting at a fixed one. | — | sensible or latent |
M_store | Sensible store total heat capacity. | kJ/K | M_store > 0Sensible store total heat capacity. |
Q_latent | Available latent heat; no warming outside the phase-change plateau is modeled. | kJ | Q_latent > 0Available latent heat; no warming outside the phase-change plateau is modeled. |
storage_flow | Latent stream transfer factor: 1-exp(-N) or N/(1+N). Sensible model uses plug flow. | — | plug flow or mixed flowLatent stream transfer factor: 1-exp(-N) or N/(1+N). Sensible model uses plug flow. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
sigma | Entropy production: entropy that was created inside the boundary rather than carried across it. Zero for an ideal process, positive for every real one, and never negative. | kJ/K | Integrated heat-exchanger entropy generation, excluding outlet disposal. |
Ed | Exergy destroyed: work potential that was permanently lost, equal to the dead-state temperature times the entropy produced. | kJ | Integrated heat-exchanger exergy destruction, T0*sigma. |
T_store_opt | The storage temperature that destroys the least exergy, which is neither the highest available nor the source temperature. | K | Capacity-constrained latent melting temperature maximizing captured exergy at fixed duration. |
eta_storage | How much of the exergy put into a store is still there to take out. | - | Stored / incoming exergy over the full duration. |
t_charge_opt | Sensible charging duration maximizing stored / incoming exergy. | s | Sensible charging duration maximizing stored / incoming exergy. |
Q_stored | Integrated stored heat. | kJ | Integrated stored heat. |
B_stored | Integrated captured exergy. | kJ | Integrated captured exergy. |
B_in | Incoming stream exergy over the entered time. | kJ | Incoming stream exergy over the entered time. |
B_out | Unused outgoing stream exergy over the entered time. | kJ | Unused outgoing stream exergy over the entered time. |
S_dump | Additional entropy if the outlet is discarded to ambient. | kJ/K | Additional entropy if the outlet is discarded to ambient. |
S_total | Heat-exchanger plus outlet-disposal entropy. | kJ/K | Heat-exchanger plus outlet-disposal entropy. |
T_final_store | Store temperature at the end of the charge. | K | Store temperature at the end of the charge. |
T_final_out | Final outlet temperature. | K | Final outlet temperature. |
The selected model reports available work or comparison rate, work per area and conversion factor. Collector mode also reports its optimum temperature, while the plot keeps the selected radiation model explicit.
Source radiation exergy, a Carnot factor and a collector's net useful output are different quantities. The collector model uses its stated radiation-loss assumptions and does not infer optical or convective losses.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | (0, infinity)Blackbody source temperature, at or above T0; collector requires strictly above. |
T0 | Dead-state temperature: the temperature of the environment the system is eventually going to equilibrate with. Exergy is meaningless without it. | K | 0 < T0 <= TEnvironment temperature bounded by the entered source; zero is an excluded endpoint. |
A | Cross-sectional area the stream passes through. | m^2 | (0, infinity)Emitting area in reference models, receiver area in collector model. |
flux | Radiant energy arriving per unit area per unit time. | kW/m^2 | (0, infinity)Incident irradiance before concentration; collector only. |
concentration | How many times the incoming radiation is concentrated before it reaches the collector. | - | (0, infinity)Collector irradiance multiplier; concentration*flux cannot exceed the source blackbody emissive power. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
psi_radiation | The fraction of a radiation stream's energy that is available as work. Lower than the reversible factor at the source temperature, and the two are routinely confused. | - | — |
E_radiation | Rate at which radiation delivers exergy. | kW | Total available/reference power includes area; density is separately labeled kW/m². The selected model defines the energy reference. |
eta_max | The largest thermal efficiency any device can have between the two given reservoir temperatures. | - | Shown beside it, since the two are routinely confused. |
T_opt | The collector temperature that maximises work output, balancing conversion quality against loss. | K | — |
Results report maximum power for the supplied constraints, efficiency and internal temperatures or stream endpoints. A conductance-allocation comparison reoptimizes each allocation under the same total budget.
Maximum power and reversible efficiency answer different questions. The finite-stream model assumes a constant heat capacity and an ideal cold reservoir; its internal-engine distribution is not a finite machine layout.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
TH | Temperature of the hot reservoir. | K | (0, infinity)Hot reservoir or hot-stream inlet, greater than TC. |
TC | Temperature of the cold reservoir. | K | (0, infinity)Cold reservoir, also the exergy reference temperature. |
UA_hot | Conductance between the hot reservoir and the engine. | kW/K | (0, infinity)Hot-side conductance; derived from total and fraction in fixed-reservoir mode. |
UA_cold | Conductance between the engine and the cold reservoir. | kW/K | (0, infinity)Derived in fixed-reservoir mode; does not apply to the ideal cold sink of the continuous hot-stream mode. |
mdot | Mass flow rate. | kg/s | (0, infinity)Hot-stream mass flow. |
cp | Specific heat at constant pressure: how much energy raises one kilogram by one degree while the pressure is held fixed. | kJ/(kg K) | (0, infinity)Constant stream specific heat. |
UA_total | The fixed sum of hot and cold exchanger conductances. | kW/K | (0, infinity)Fixed-reservoir total conductance budget. |
hot_conductance_fraction | The share of the fixed conductance budget assigned to the hot side. | - | (0, 1)Fraction of total conductance assigned to the hot exchanger; zero endpoints cannot run the engine. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta_maxpower | The efficiency a device actually runs at when it is producing as much power as it can, which is lower than the reversible bound and much closer to what real plants achieve. | - | η=1-√(T_C/T_H) Model-dependent result; see explicitly selected source constraint. |
Wdot_max | The largest power the arrangement can produce under the stated constraint, as opposed to the largest efficiency. | kW | Model-dependent result; see explicitly selected source constraint. |
eta_max | The largest thermal efficiency any device can have between the two given reservoir temperatures. | - | Shown beside it, for the comparison. Model-dependent result; see explicitly selected source constraint. |
T_internal | The internal working temperatures of an endoreversible engine, which sit between the reservoir temperatures because the heat has to flow across a finite gap. | K | Model-dependent result; see explicitly selected source constraint. |
The design reports total entropy generation and its thermal/friction parts, with the selected diameter or heat-transfer size parameter and feasibility diagnostics. The curve exposes the competing contributions.
These are constrained thermodynamic/correlation models, not universal equipment optimizers. Keep Reynolds, Prandtl, aspect-ratio and Biot restrictions; properties are not automatically updated with the calculated temperature field.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
geometry | Arrangement: heated duct, balanced counterflow exchanger, or fixed-length pin fin in crossflow. | — | one of three declared arrangementsArrangement: heated duct, balanced counterflow exchanger, or fixed-length pin fin in crossflow. |
temperature | Fluid temperature for duct and pin fin. | K | finite positive; active only in named arrangementFluid temperature for duct and pin fin. |
density | Constant fluid density for duct and pin fin. | kg/m^3 | finite positive; active only in named arrangementConstant fluid density for duct and pin fin. |
viscosity | Constant dynamic viscosity for duct and pin fin. | Pa s | finite positive; active only in named arrangementConstant dynamic viscosity for duct and pin fin. |
conductivity | Constant fluid thermal conductivity for duct and pin fin. | W/(m K) | finite positive; active only in named arrangementConstant fluid thermal conductivity for duct and pin fin. |
mass_flow | Duct fluid mass flow. | kg/s | finite positive; active only in named arrangementDuct fluid mass flow. |
heat_per_length | Heat transferred to the duct fluid per unit length. | W/m | finite positive; active only in named arrangementHeat transferred to the duct fluid per unit length. |
duct_length | Duct segment length over which heat and pressure losses are evaluated. | m | finite positive; active only in named arrangementDuct segment length over which heat and pressure losses are evaluated. |
cp | Specific heat at constant pressure: how much energy raises one kilogram by one degree while the pressure is held fixed. | kJ/(kg K) | finite positive; active only in named arrangementDuct mass-specific heat; the display adapter alone converts to J/(kg K) for the composition calculation. |
prandtl | Duct heat-transfer correlation Prandtl number. Pin-fin Prandtl number is fixed at 0.71, not this input. | - | 0.7 < prandtl < 160Duct heat-transfer correlation Prandtl number. Pin-fin Prandtl number is fixed at 0.71, not this input. |
hot | Balanced exchanger hot-side inlet temperature. | K | hot > cold > 0Balanced exchanger hot-side inlet temperature. |
cold | Balanced exchanger cold-side inlet temperature. | K | hot > cold > 0Balanced exchanger cold-side inlet temperature. |
capacity | Equal heat-capacity rate of either single side of the balanced exchanger; not the sum. | kW/K | finite positiveEqual heat-capacity rate of either single side of the balanced exchanger; not the sum. |
hot_drop | Hot fractional inlet-pressure loss per unit NTU. | - | non-negative; at least one loss slope positiveHot fractional inlet-pressure loss per unit NTU. |
cold_drop | Cold fractional inlet-pressure loss per unit NTU. | - | non-negative; at least one loss slope positiveCold fractional inlet-pressure loss per unit NTU. |
hot_ratio | Hot-side gas constant divided by specific heat. | - | 0 < hot_ratio < 1Hot-side gas constant divided by specific heat. |
cold_ratio | Cold-side gas constant divided by specific heat. | - | 0 < cold_ratio < 1Cold-side gas constant divided by specific heat. |
minimum_effectiveness | Minimum fraction of the balanced exchanger maximum heat duty required by the design task. | - | 0 < minimum_effectiveness < 1Useful-duty lower bound on balanced-exchanger effectiveness. |
maximum_drop | Upper bound on either side fractional pressure drop. | - | 0 < maximum_drop < 1Upper bound on either side fractional pressure drop. |
heat | Fixed pin-fin heat duty. | W | finite positive; pin-fin arrangementFixed pin-fin heat duty. |
speed | Fluid speed across the pin fin. | m/s | finite positive; pin-fin arrangementFluid speed across the pin fin. |
fin_length | Fixed pin-fin length; only diameter is optimized. | m | finite positive; pin-fin arrangementFixed pin-fin length; only diameter is optimized. |
fin_conductivity | Solid pin-fin thermal conductivity. | W/(m K) | finite positive; pin-fin arrangementSolid pin-fin thermal conductivity. |
reference_capacity | Fixed pin-fin reference capacity used solely to normalize the entropy-generation number. | kW/K | finite positive; pin-fin arrangementFixed pin-fin reference capacity used solely to normalize the entropy-generation number. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Ns | Entropy generation number: entropy produced, made dimensionless by the stream's capacity rate, so arrangements of different size can be compared. | - | Total entropy generation divided by duct mass-flow heat capacity, either balanced-exchanger side capacity, or fixed pin-fin reference capacity. |
sigmadot_dT | The share of entropy production caused by heat crossing a finite temperature difference. | kW/K | Thermal part at the selected constrained design. |
sigmadot_dp | The share caused by fluid friction. | kW/K | Fluid-friction part at the selected constrained design. |
D_opt | Duct or pin-fin diameter at the constrained minimum; only these two arrangements. | m | Duct or pin-fin diameter at the constrained minimum; only these two arrangements. |
NTU_opt | Balanced-exchanger NTU at the constrained minimum; only this arrangement. | - | Balanced-exchanger NTU at the constrained minimum; only this arrangement. |
design_boundary | Whether the selected minimum is on a constraint boundary or is an interior stationary point. | — | Whether the selected minimum is on a constraint boundary or is an interior stationary point. |
Re | Reynolds number: the ratio of inertial to viscous effects in the flow, which is what fixes the friction. | - | duct arrangement: metric named Reynolds number. Derived at the selected design, not a direct input. |
Nu | Nusselt number. | - | duct arrangement: metric named Nusselt number. Derived at the selected design, not a direct input. |
f_fanning | Fanning friction factor. | - | duct arrangement: metric named Fanning friction factor. Derived at the selected design, not a direct input. |
wall_bulk_difference | Wall minus bulk temperature. | ΔK | duct arrangement: metric named Wall minus bulk temperature. Derived at the selected design, not a direct input. |
segment_pressure_drop | Segment pressure drop. | MPa | duct arrangement: metric named Segment pressure drop. Derived at the selected design, not a direct input. |
bulk_rise_fraction | Bulk temperature rise fraction. | - | duct arrangement: metric named Bulk temperature rise fraction. Derived at the selected design, not a direct input. |
property_prandtl | Property-derived Prandtl number. | - | duct arrangement: metric named Property-derived Prandtl number. Derived at the selected design, not a direct input. |
epsilon | Exergetic efficiency: what the component actually delivered as a fraction of the exergy it was given. It asks a harder question than thermal efficiency and usually gets a worse answer. | - | balanced arrangement: metric named Effectiveness. Derived at the selected design, not a direct input. |
Qdot | Rate of heat transfer. | kW | balanced arrangement: metric named Heat transferred. Derived at the selected design, not a direct input. |
hot_outlet_temperature | Hot outlet temperature. | K | balanced arrangement: metric named Hot outlet temperature. Derived at the selected design, not a direct input. |
cold_outlet_temperature | Cold outlet temperature. | K | balanced arrangement: metric named Cold outlet temperature. Derived at the selected design, not a direct input. |
hot_drop_fraction | Hot pressure drop / inlet pressure. | - | balanced arrangement: metric named Hot pressure drop / inlet pressure. Derived at the selected design, not a direct input. |
cold_drop_fraction | Cold pressure drop / inlet pressure. | - | balanced arrangement: metric named Cold pressure drop / inlet pressure. Derived at the selected design, not a direct input. |
NTU_asymptotic | Asymptotic unconstrained NTU. | - | balanced arrangement: metric named Asymptotic unconstrained NTU. Derived at the selected design, not a direct input. |
thermal_asymptotic | Asymptotic thermal entropy at selected NTU. | kW/K | balanced arrangement: metric named Asymptotic thermal entropy at selected NTU. Derived at the selected design, not a direct input. |
friction_asymptotic | Asymptotic friction entropy at selected NTU. | kW/K | balanced arrangement: metric named Asymptotic friction entropy at selected NTU. Derived at the selected design, not a direct input. |
Re | Reynolds number: the ratio of inertial to viscous effects in the flow, which is what fixes the friction. | - | pin fin arrangement: metric named Reynolds number. Derived at the selected design, not a direct input. |
Nu | Nusselt number. | - | pin fin arrangement: metric named Nusselt number. Derived at the selected design, not a direct input. |
C_drag | Drag coefficient. | - | pin fin arrangement: metric named Drag coefficient. Derived at the selected design, not a direct input. |
fin_base_temperature | Fin base temperature. | K | pin fin arrangement: metric named Fin base temperature. Derived at the selected design, not a direct input. |
base_ambient_difference | Base minus ambient temperature. | ΔK | pin fin arrangement: metric named Base minus ambient temperature. Derived at the selected design, not a direct input. |
Bi_transverse | Transverse Biot number. | - | pin fin arrangement: metric named Transverse Biot number. Derived at the selected design, not a direct input. |
aspect | The geometric design variable being optimised over. | - | pin fin arrangement: metric named Length / diameter. Derived at the selected design, not a direct input. |
drag_force | Drag force. | N | pin fin arrangement: metric named Drag force. Derived at the selected design, not a direct input. |
fin_conductance | Fin thermal conductance. | kW/K | pin fin arrangement: metric named Fin thermal conductance. Derived at the selected design, not a direct input. |
The resolved state reports dry bulb, wet bulb, dew point, relative humidity, humidity ratio, enthalpy and volume. The psychrometric chart uses the same pressure as the calculation.
Moist-air enthalpy and volume are per dry-air mass. Supersaturated fog or ice is not silently inserted, and an altitude estimate is not a local weather pressure measurement.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Barometric pressure; altitude-corrected. |
Tdb | Dry-bulb temperature: what an ordinary thermometer in the air stream reads. | K | — |
Twb | Wet-bulb temperature: what a thermometer with a wet wick reads, which is lower because evaporation cools it. How much lower is a measure of how dry the air is. | K | — |
Tdp | Dew point: the temperature at which the air being cooled would start to condense. | K | — |
omega | Humidity ratio: kilograms of water vapour carried per kilogram of dry air. The quantity that stays fixed when moist air is merely heated or cooled. | - | — |
phi | Relative humidity: how much water vapour the air holds as a fraction of the most it could hold at that temperature. | - | 0 <= phi <= 1 |
h_da | Enthalpy of moist air per kilogram of dry air, rather than per kilogram of mixture, because the dry air is what stays constant through the processes. | kJ/kg | Enthalpy per unit mass of dry air. |
altitude | Height above sea level, used to correct the barometric pressure, which shifts the whole chart. | m | -500 <= altitude <= 11000 |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
omega | Humidity ratio: kilograms of water vapour carried per kilogram of dry air. The quantity that stays fixed when moist air is merely heated or cooled. | - | ω=0.622pᵥ/(p-pᵥ) |
phi | Relative humidity: how much water vapour the air holds as a fraction of the most it could hold at that temperature. | - | — |
Tdp | Dew point: the temperature at which the air being cooled would start to condense. | K | — |
Twb | Wet-bulb temperature: what a thermometer with a wet wick reads, which is lower because evaporation cools it. How much lower is a measure of how dry the air is. | K | — |
h_da | Enthalpy of moist air per kilogram of dry air, rather than per kilogram of mixture, because the dry air is what stays constant through the processes. | kJ/kg | h=h_a+ω h_g(T) |
v_da | Volume occupied per kilogram of dry air. | m^3/kg | — |
mu_sat | Degree of saturation: the humidity ratio as a fraction of the saturated value at the same temperature and pressure. | - | — |
p_partial | Partial pressure: the pressure one component of a mixture would exert if it alone occupied the whole volume. | MPa | — |
Heating, cooling, dehumidification/reheat, humidification and mixing retain their distinct balances. Net duty, moisture transfer and sensible heat ratio are reported where defined; the path shows the corresponding moist-air states.
A coil bypass factor interpolates temperature and humidity ratio and may be capped at saturation with a note. Two-stream mixing instead refuses a fog-forming gas-only outlet; it does not solve condensate jointly.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
process | Which of the available process paths the screen is applying. | — | — |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
mdot1 | Mass flow rate. | kg/s | Dry air flow. |
Tdb1 | Dry-bulb temperature: what an ordinary thermometer in the air stream reads. | K | — |
phi1 | Relative humidity: how much water vapour the air holds as a fraction of the most it could hold at that temperature. | - | — |
Tdb2 | Dry-bulb temperature: what an ordinary thermometer in the air stream reads. | K | Second inlet temperature/humidity for adiabatic mixing; target supply temperature is entered in the relevant sensible or reheat branch. |
phi2 | Relative humidity: how much water vapour the air holds as a fraction of the most it could hold at that temperature. | - | Second inlet temperature/humidity for adiabatic mixing; target supply temperature is entered in the relevant sensible or reheat branch. |
mdot_water | Rate at which liquid water is added to or removed from a moist air stream. | kg/s | Injected water for steam or spray humidification. Condensate removal is an output in cooling branches. |
T_coil | Coil dew-point temperature in dehumidifying branches. | K | branch-dependentCoil dew-point temperature in dehumidifying branches. |
T_supply | Specified final supply temperature for sensible heating/cooling or reheat. | K | branch-dependentSpecified final supply temperature for sensible heating/cooling or reheat. |
bypass | Optional coil bypass factor; zero when omitted. | - | branch-dependentOptional coil bypass factor; zero when omitted. |
T_water | Injected steam or spray-water temperature; interpretation follows process. | K | branch-dependentInjected steam or spray-water temperature; interpretation follows process. |
epsilon_evap | Evaporative-cooling effectiveness. | - | branch-dependentEvaporative-cooling effectiveness. |
mdot2 | Mass flow rate. | kg/s | finite positiveSecond inlet dry-air mass flow for adiabatic mixing. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Qdot | Rate of heat transfer. | kW | — |
mdot_water | Rate at which liquid water is added to or removed from a moist air stream. | kg/s | ṁ_w=ṁ_a(ω_2-ω_1) |
omega2 | Humidity ratio: kilograms of water vapour carried per kilogram of dry air. The quantity that stays fixed when moist air is merely heated or cooled. | - | — |
Tdb2 | Dry-bulb temperature: what an ordinary thermometer in the air stream reads. | K | — |
SHR | Sensible heat ratio: the share of the total cooling load that changes temperature rather than removing moisture. It is what sizes real equipment. | - | Sensible fraction of the total load, which is what sizes real equipment. |
The tower balance returns required dry-air flow, evaporative makeup, range, approach to entering wet bulb, rejected heat and entropy production. Both air states show how water evaporation changes the balance.
Makeup here covers evaporation, not drift or blowdown. A small positive approach can imply demanding equipment even when the balance is feasible; the calculation does not size packing or fan power.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
mdot1 | Mass flow rate. | kg/s | Water flow. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Warm water in. |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Cooled water out. |
Tdb3 | Dry-bulb temperature: what an ordinary thermometer in the air stream reads. | K | Air in. |
phi3 | Relative humidity: how much water vapour the air holds as a fraction of the most it could hold at that temperature. | - | — |
Tdb4 | Dry-bulb temperature: what an ordinary thermometer in the air stream reads. | K | Air out. |
phi4 | Relative humidity: how much water vapour the air holds as a fraction of the most it could hold at that temperature. | - | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
mdot_air | Dry air mass flow rate. | kg/s | — |
mdot_makeup | Rate at which water must be replaced to make up for what evaporated. | kg/s | — |
range | Cooling tower range: how far the water temperature falls across the tower. | ΔK | — |
approach | Cooling tower approach: how close the cooled water gets to the entering air's wet-bulb temperature. It can be made small but never zero, however large the tower. | ΔK | — |
sigmadot | Rate of entropy production. | kW/K | — |
Specific work, heat and changes in u, h and s are accompanied by total W, Q, delta U, delta H and delta S. Both diagrams use the same resolved path. Sampled p dv and T ds integrals and their differences from the reported transfers are shown separately.
Internally reversible closed-system paths with boundary work only are assumed. Water isotherms use the water equation of state, not the ideal-gas pv shortcut. T-s heat areas use absolute K or degR. Sampling and property-fit consistency affect integral differences. Unresolved branches, subresolution nonzero changes and unrepresentable totals refuse the whole path.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | declared ideal-gas species; water; or a user-given incompressible idealisation |
process | Which of the available process paths the screen is applying. | — | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | finite positive temperature inside the selected modelUsed only when active in the selected independent pair or endpoint control; otherwise derived. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | finite positive pressure inside the selected modelUsed only when active in the selected independent pair or endpoint control; otherwise derived. |
v1 | Specific volume: the space one kilogram of the substance occupies. The reciprocal of density, and the property that makes a gas different from a liquid. | m^3/kg | finite positive specific volumeUsed only when active in the selected independent pair or endpoint control; otherwise derived. |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | finite positive temperature inside the selected modelUsed only when active in the selected independent pair or endpoint control; otherwise derived. |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | finite positive pressure inside the selected modelUsed only when active in the selected independent pair or endpoint control; otherwise derived. |
v2 | Specific volume: the space one kilogram of the substance occupies. The reciprocal of density, and the property that makes a gas different from a liquid. | m^3/kg | finite positive specific volumeUsed only when active in the selected independent pair or endpoint control; otherwise derived. |
n | Polytropic exponent: the constant in a path where pressure times volume to this power stays fixed. Zero gives constant pressure, one gives constant temperature for an ideal gas, and the specific heat ratio gives an isentropic path. | - | -inf < n < infPolytropic exponent. |
m | Mass of the system or of the sample being considered. | kg | finite m > 0; all nonzero totals must remain representable |
process_model | Property model used for every state on the path. | — | ideal gas | water IF97 | incompressible (given c and v)Property model used for every state on the path. |
caloric_model | NASA polynomial, evaluated constant cp, or air-only cold-air standard. | — | one of the three declared gas caloric modelsNASA polynomial, evaluated constant cp, or air-only cold-air standard. |
evaluation_temperature | Temperature used to evaluate constant cp. | K | inside the selected gas polynomial intervalTemperature used to evaluate constant cp. |
inlet_pair | Water alone accepts quality; the given-c/v model uses p,T. | — | p,T | p,v | p,xWater alone accepts quality; the given-c/v model uses p,T. |
x | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | — | 0 <= x <= 1Active water quality for an initial p,x pair or isobaric endpoint. |
temperature_root | Visible water p,v temperature root; changing root counts on a polytrope are refused. | — | lower-temperature root | higher-temperature rootVisible water p,v temperature root; changing root counts on a polytrope are refused. |
heat_capacity | User-given incompressible constant c; no material database. | kJ/(kg K) | finite c > 0User-given incompressible constant c; no material database. |
fixed_volume | User-given incompressible constant specific volume. | m^3/kg | finite v > 0User-given incompressible constant specific volume. |
path_samples | Number of base nodes; water saturation breakpoints may add nodes. | — | integer 2 <= path_samples <= 401Number of base nodes; water saturation breakpoints may add nodes. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
W | Work transferred across the boundary, taken as positive when it comes out of the system. | kJ | W=∫₁² p dV Total for the stated mass; state changes and transfers are also shown per kg. |
Q | Heat transferred across the boundary, taken as positive when it goes into the system. | kJ | Q=Δ U+W Total for the stated mass; state changes and transfers are also shown per kg. |
DeltaU | Change in the total internal energy of the system between the two states. | kJ | Total for the stated mass; state changes and transfers are also shown per kg. |
DeltaH | Change in total enthalpy between the two states. | kJ | Total for the stated mass; state changes and transfers are also shown per kg. |
DeltaS | Change in total entropy between the two states. | kJ/K | Total for the stated mass; state changes and transfers are also shown per kg. |
specific_work | Boundary work leaving the closed system per unit mass. | kJ/kg | Boundary work leaving the closed system per unit mass. |
specific_heat | Heat entering the closed system per unit mass. | kJ/kg | Heat entering the closed system per unit mass. |
process_delta_u | Change in specific internal energy, final minus initial. | kJ/kg | Change in specific internal energy, final minus initial. |
process_delta_h | Change in specific enthalpy, final minus initial. | kJ/kg | Change in specific enthalpy, final minus initial. |
process_delta_s | Change in specific entropy, final minus initial. | kJ/(kg K) | Change in specific entropy, final minus initial. |
sampled_work | Trapezoidal integral of pressure with respect to specific volume. | kJ/kg | Trapezoidal integral of pressure with respect to specific volume. |
sampled_heat | Trapezoidal integral of absolute temperature with respect to specific entropy. | kJ/kg | Trapezoidal integral of absolute temperature with respect to specific entropy. |
work_difference | Sampled p dv minus reported boundary work; a diagnostic, not a certified error bound. | kJ/kg | Sampled p dv minus reported boundary work; a diagnostic, not a certified error bound. |
heat_difference | Sampled T ds minus reported heat; includes sampling and property-formulation consistency. | kJ/kg | Sampled T ds minus reported heat; includes sampling and property-formulation consistency. |
The balance reports total heat, work, internal-energy change, kinetic and potential terms and a residual. Final-state mode also reports the recovered water properties; the selected work mode shows its contribution explicitly.
Heat is positive in and work positive out. Specific energy and total energy are different bases. A first-law solution does not by itself certify the second law.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
m | Mass of the system or of the sample being considered. | kg | — |
Q | Heat transferred across the boundary, taken as positive when it goes into the system. | kJ | — |
W | Work transferred across the boundary, taken as positive when it comes out of the system. | kJ | — |
DeltaU | Change in the total internal energy of the system between the two states. | kJ | — |
vel1 | Velocity of the stream, which matters only when it is fast enough for its kinetic energy to compete with its enthalpy. | m/s | — |
vel2 | Velocity of the stream, which matters only when it is fast enough for its kinetic energy to compete with its enthalpy. | m/s | — |
z1 | Elevation above the chosen datum. | m | — |
z2 | Elevation above the chosen datum. | m | — |
Delta_u_specific | Change in internal energy per kilogram, specified independently when the total balance determines mass. | kJ/kg | finite, resolved net specific energyGiven for mass inverse; total energy outputs remain kJ. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | IF97 pressure rangeInitial state for final-state inverse |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | 273.15 <= T <= 1073.15, within supported regionInitial state for final-state inverse |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | IF97 pressure rangeFinal-pressure constraint |
v2 | Specific volume: the space one kilogram of the substance occupies. The reciprocal of density, and the property that makes a gas different from a liquid. | m^3/kg | v > 0, resolved inside supported formulationFinal specific-volume constraint; rigid volume uses initial v |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Q | Heat transferred across the boundary, taken as positive when it goes into the system. | kJ | Q=Δ U+Δ KE+Δ PE+W |
W | Work transferred across the boundary, taken as positive when it comes out of the system. | kJ | W=Q-Δ U-Δ KE-Δ PE |
DeltaU | Change in the total internal energy of the system between the two states. | kJ | — |
DeltaKE | Change in kinetic energy of the system as a whole. | kJ | Δ KE=(1/2)m(V₂²-V₁²) |
DeltaPE | Change in gravitational potential energy of the system as a whole. | kJ | Δ PE=mg(z₂-z₁) |
m | Mass of the system or of the sample being considered. | kg | m=(Q-W)/(Δ u+Δ ke+Δ pe) Positive resolved mass from independently specified specific energy change |
T | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Final water state; quality is defined only in the saturation domain |
p | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Final water state; quality is defined only in the saturation domain |
v | Specific volume: the space one kilogram of the substance occupies. The reciprocal of density, and the property that makes a gas different from a liquid. | m^3/kg | Final water state; quality is defined only in the saturation domain |
u | Specific internal energy: the energy stored in one kilogram of a substance by the motion and arrangement of its molecules, with no reference to where the substance is or how fast it is moving. | kJ/kg | Final water state; quality is defined only in the saturation domain |
h | Specific enthalpy: internal energy plus pressure times specific volume. It exists because that combination appears every time a substance flows across a boundary, so it is a bookkeeping convenience that behaves like a property. | kJ/kg | Final water state; quality is defined only in the saturation domain |
s | Specific entropy: the property that counts how much of a system's energy is no longer available to do work. It increases in every real process and stays put only in an ideal one. | kJ/(kg K) | Final water state; quality is defined only in the saturation domain |
x | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | — | Final water state; quality is defined only in the saturation domain |
Power mode reports signed work out and thermal efficiency. Reverse modes report negative work out, positive work input and both COPs, with heating COP equal to refrigeration COP plus one. The energy-flow figure supports the plot export controls.
A direction mismatch, negative entropy production or unresolved work difference replaces results with an explanation. These necessary balances do not reconstruct a machine or its component states.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
device | Which device the efficiency definition is being applied to. | — | power, refrigeration or heat pumpSelects the useful output and heat-transfer directions. |
Qin | Total heat supplied to a cycle over one complete circuit, counted as a positive quantity. | kJ | Positive heat absorbed: from TH in power mode, from TC in refrigeration/heat-pump mode. |
Qout | Total heat rejected by a cycle over one complete circuit, counted as a positive quantity. | kJ | Positive heat rejected: to TC in power mode, to TH in refrigeration/heat-pump mode. |
TH | Temperature of the hot reservoir. | K | — |
TC | Temperature of the cold reservoir. | K | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Wcycle | Net work produced or consumed over one complete circuit of a cycle. | kJ | W_cycle=Q_in-Q_out Signed work out. Refrigeration/heat-pump work input is its negative. |
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | η=W_cycle/Q_in Power mode only; positive work out divided by absorbed heat. |
beta | Coefficient of performance of a refrigerator: heat removed from the cold space divided by the work it cost. Routinely greater than one, which is why it is not called an efficiency. | - | β=Qᵢₙ/Wᵢₙ Refrigeration and heat-pump modes; Win=Qout−Qin>0. |
gamma | Coefficient of performance of a heat pump: heat delivered to the warm space divided by the work it cost. Always exactly one more than the refrigeration value for the same machine. | - | γ=Qₒᵤₜ/Wᵢₙ=β+1 Same refrigeration cycle, heating-output perspective. |
eta_C | Reversible heat-engine efficiency between the entered reservoirs. | - | Reversible heat-engine bound. |
beta_C | Reversible refrigeration coefficient of performance between the entered reservoirs. | - | Reversible refrigeration bound. |
gamma_C | Reversible heat-pump coefficient of performance between the entered reservoirs. | - | Reversible heat-pump bound. |
sigma_cycle | Entropy produced over one complete circuit, obtained from the cycle integral of heat over boundary temperature. | kJ/K | Entropy produced per cycle for the selected direction. |
r_energy | Signed residual of the stated energy balance; zero within numerical resolution for a closed balance. | kJ | Signed first-law residual. |
The energy columns show static enthalpy and kinetic energy on the same mass basis at both ends. Read exit speed, stagnation enthalpy, closure residual, entropy production and rate, areas and area ratio. The separate stated-area input reports mass flow or an explanation. The graph supports PNG/PDF/SVG export.
A wet state can have valid energy and area results without a defined acoustic result. This property-and-energy calculation does not design a choked duct or a nozzle contour.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
device | Which device the efficiency definition is being applied to. | — | nozzle or diffuserWater/steam, adiabatic, no shaft work. Exit state and areas are calculated from the selected device efficiency. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
vel1 | Velocity of the stream, which matters only when it is fast enough for its kinetic energy to compete with its enthalpy. | m/s | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
A2 | Cross-sectional area the stream passes through. | m^2 | Stated exit area for the separate mass-flow check. The primary calculation takes mass flow and reports its required inlet and exit areas. |
mdot | Mass flow rate. | kg/s | — |
eta_n | Isentropic nozzle efficiency: actual kinetic energy at the exit divided by what an ideal expansion would have produced. | — | 0 < efficiency <= 1Only the selected device efficiency is active: nozzle exit kinetic-energy ratio or diffuser ideal/actual enthalpy-rise ratio. |
eta_d | Diffuser efficiency: isentropic enthalpy rise divided by the actual kinetic-energy drop, equal to actual enthalpy rise for the adiabatic no-work model. | — | 0 < efficiency <= 1Only the selected device efficiency is active: nozzle exit kinetic-energy ratio or diffuser ideal/actual enthalpy-rise ratio. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
vel2 | Velocity of the stream, which matters only when it is fast enough for its kinetic energy to compete with its enthalpy. | m/s | V₂=√(2(h₁-h₂)+V₁²) |
A2 | Cross-sectional area the stream passes through. | m^2 | A=ṁv/V |
mdot | Mass flow rate. | kg/s | ṁ=AV/v Secondary stated-area check; primary flow is supplied independently. |
h2 | Specific enthalpy: internal energy plus pressure times specific volume. It exists because that combination appears every time a substance flows across a boundary, so it is a bookkeeping convenience that behaves like a property. | kJ/kg | — |
h0 | Stagnation enthalpy: the enthalpy a stream would have if it were brought to rest without loss. Conserved through an adiabatic duct with no work. | kJ/kg | Shared stagnation enthalpy; h + V²/2000 in the implementation units. |
e_kinetic1 | Kinetic energy carried by each unit of flowing mass. | kJ/kg | — |
e_kinetic2 | Kinetic energy carried by each unit of flowing mass. | kJ/kg | — |
A_ratio | Outlet area divided by inlet area, for the same steady mass flow. | — | — |
sigma | Entropy production: entropy that was created inside the boundary rather than carried across it. Zero for an ideal process, positive for every real one, and never negative. | kJ/(kg K) | Specific entropy produced across the device. |
sigmadot | Rate of entropy production. | kW/K | — |
r_energy | Signed residual of the stated energy balance; zero within numerical resolution for a closed balance. | kJ/kg | — |
A1 | Cross-sectional area the stream passes through. | m^2 | A₁=ṁ v₁/ V₁ Derived inlet area; a finite positive area requires a positive inlet speed. |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Derived actual water/steam exit temperature. |
Compare actual and isentropic outlet states, specific work and shaft power. With heat loss, the entry also reports heat into the turbine, entropy production and the enthalpy-drop ratio separately from the thermodynamic performance definition.
Outward heat loss is entered as a positive loss; the heat-into-system result is negative. A wet steam exit and its erosion warning need interpretation beyond a finite shaft-power result.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Active only when the selected inverse/supplied-state direction uses exit temperature; otherwise calculated. |
mdot | Mass flow rate. | kg/s | — |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | 0 < eta_t <= 1 |
h_exit_given | Measured turbine outlet enthalpy per unit mass. | kJ/kg | finite; applicable state/device domainActive only in the corresponding supplied-quantity direction. |
x_exit_given | Measured vapor mass fraction at the turbine outlet. | - | finite; applicable state/device domainActive only in the corresponding supplied-quantity direction. |
Wdot_given | Positive shaft power supplied to determine a turbine outlet. | kW | finite; applicable state/device domainActive only in the corresponding supplied-quantity direction. |
T_boundary | Temperature of the control surface where heat crosses the boundary. | K | finite and > 0Required for heat loss. |
heat_loss_rate | Non-negative thermal energy rate transferred out of the device. | kW | finite and >= 0Outward positive; heat into turbine is its negative. |
gas_cp_model | Specific-heat law used consistently in the ideal-gas state and inverse calculations. | — | one declared ideal-gas caloric modelActive for ideal gas. |
T_cp_evaluation | Temperature at which a constant specific heat is evaluated. | K | within source temperature rangeUsed by the constant-cp model. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Wdot | Rate of work transfer, that is, power. | kW | Ẇ=ṁ(h₁-h₂)+Q̇ Shaft power includes specified outward heat loss in the heat-loss model. |
h2 | Specific enthalpy: internal energy plus pressure times specific volume. It exists because that combination appears every time a substance flows across a boundary, so it is a bookkeeping convenience that behaves like a property. | kJ/kg | — |
x2 | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | - | — |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | ηₜ=(h₁-h₂)/(h₁-h₂ₛ) Adiabatic model only; a cooled-turbine enthalpy-drop ratio is reported separately and is not an efficiency. |
sigmadot | Rate of entropy production. | kW/K | σ̇=ṁ(s_2-s_1)-Q̇/T_b Includes thermal boundary entropy transfer. |
enthalpy_drop_ratio | Actual enthalpy decrease divided by the isentropic reference decrease; under heat loss this is not an adiabatic efficiency. | - | Displayed for heat-loss model; may exceed one. |
w_turbine | Work delivered by the turbine per kilogram of working fluid. | kJ/kg | Actual specific work out, including the selected heat-loss model. |
w_isentropic | Reversible adiabatic work per mass from the inlet and outlet enthalpy difference. | kJ/kg | Ideal isentropic specific work between the same inlet and exit pressure. |
q_specific | Signed heat into the turbine per unit mass; negative for outward loss. | kJ/kg | Signed heat into the turbine per unit mass; negative for outward loss. |
Qdot | Rate of heat transfer. | kW | Signed heat into the turbine; equals minus the entered outward heat-loss rate. |
sigma | Entropy production: entropy that was created inside the boundary rather than carried across it. Zero for an ideal process, positive for every real one, and never negative. | kJ/(kg K) | Specific entropy generated, including heat transfer at the supplied boundary temperature. |
The balance reports duty, all four terminal temperatures and recovered flows, entropy production and closure. Non-mixing mode plots constant-pressure temperatures against heat load and reports both terminal minimum approach and sampled internal minimum. Water phase-change breakpoints are included. Direct contact shows its three terminal temperatures schematically.
This is a thermodynamic balance, not exchanger sizing. The heat-load axis is not length. Internal temperature crossings are refused; a positive sampled minimum does not certify every unsampled state. Mixing requires one common fluid and pressure.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | Non-mixing: independent hot and cold fluid choices; mixing: both streams share the first selected fluid. |
mdot1 | Mass flow rate. | kg/s | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
mdot3 | Mass flow rate. | kg/s | — |
p3 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
T4 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Qdot | Rate of heat transfer. | kW | Q̇=ṁₕ(h₁-h₂) |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
T4 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
mdot | Mass flow rate. | kg/s | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Recovered or supplied inlet temperature. |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Recovered or supplied inlet temperature. |
approach_terminal | The smaller temperature gap at the two exchanger ends. | ΔK | Non-mixing only: smaller terminal temperature difference. |
approach_sampled | The smallest temperature gap among the evaluated exchanger points. | ΔK | Non-mixing only: minimum at the sampled heat-load points, not a continuous pinch guarantee. |
Q_at_minimum | Transferred heat rate at the smallest sampled temperature gap. | kW | Non-mixing only: heat-load coordinate of the sampled minimum. |
sigmadot | Rate of entropy production. | kW/K | Both streams together, or the mixing control volume. |
r_energy | Signed residual of the stated energy balance; zero within numerical resolution for a closed balance. | kW | Rate balance residual. |
Forward mode retains enthalpy and reports the outlet phase and entropy generation. Calorimetry recovers upstream quality when its assumptions hold. The inversion task shows zero-Joule–Thomson branches and the local cooling/heating response.
The sign of the local Joule–Thomson coefficient describes a differential pressure change, not an arbitrary finite throttle. A calorimeter measurement must resolve the downstream state rather than leave it on an ambiguous saturation pair.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
x1 | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | - | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Active only when the selected inverse/supplied-state direction uses exit temperature; otherwise calculated. |
mdot | Mass flow rate. | kg/s | finite and non-negativeMass-flow rating of the water or real-refrigerant forward process; entropy production is reported as a rate. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
h2 | Specific enthalpy: internal energy plus pressure times specific volume. It exists because that combination appears every time a substance flows across a boundary, so it is a bookkeeping convenience that behaves like a property. | kJ/kg | Exit enthalpy on a mass basis; water uses composition.throttle_operation.Operation.exit. |
x1 | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | - | The calorimeter reading: upstream quality from downstream temperature and pressure. |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Exit temperature from the selected real-fluid constant-enthalpy state; water uses composition.throttle_operation. |
mu_JT | Joule-Thomson coefficient: how much the temperature changes per unit pressure drop in a throttling process. Its sign decides whether throttling cools or warms, and refrigeration only works where it is positive. | K/MPa | μ_J=(1/c_p)[T(∂ v/(∂ T))_p-v] Local single-phase coefficient from the same EOS and cp. At saturation supply quality; no single-phase coefficient is assigned. |
sigmadot | Rate of entropy production. | kW/K | Mass-flow times mass-specific entropy increase; water uses composition.throttle_operation.Operation.entropy_rate. |
Read final temperature, pressure, mass, internal energy and quality when present. Positive mass transferred means admitted mass during charging and removed mass during discharge. Total stored, transported, heat and work energies share a kJ or Btu basis. The energy chart exports PNG/PDF/SVG; an evacuated adiabatic zero-work charge also compares u2 with supply enthalpy on a separate mass-specific chart. Discharge reports a 400-segment h dm diagnostic and its difference from the endpoint energy balance.
The remaining uniform contents of this particular adiabatic discharge have constant specific entropy; that does not imply a reversible external jet. No time or valve-flow model is supplied. Unresolved mass or energy differences are refused, and edits hide obsolete results while the new calculation runs.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
V | Volume: the space the whole system occupies, as opposed to the space one kilogram of it occupies. | m^3 | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Initial vessel state; omitted for initially evacuated charging. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Initial vessel state; omitted for initially evacuated charging. |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
p0 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Supply-line state. Supply state used only while charging. |
T0 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Supply state used only while charging. |
Qcv | Heat transferred into a control volume over the period being considered. | kJ | Charging only; total heat is positive into the vessel, total shaft/electrical work is positive out. Discharge fixes both to zero. |
Wcv | Work taken out of a control volume over the period being considered. | kJ | Charging only; total heat is positive into the vessel, total shaft/electrical work is positive out. Discharge fixes both to zero. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
m2 | Mass of the system or of the sample being considered. | kg | — |
u2 | Specific internal energy: the energy stored in one kilogram of a substance by the motion and arrangement of its molecules, with no reference to where the substance is or how fast it is moving. | kJ/kg | — |
mdot_total | Total mass transferred over the whole transient period, as opposed to the instantaneous rate. | kg | — |
U_vessel_initial | Initial total internal energy. | kJ | Initial total internal energy. |
U_vessel_final | Final total internal energy. | kJ | Final total internal energy. |
E_transport_net | Net transported energy signed into the vessel. | kJ | Net transported energy signed into the vessel. |
E_transport_sampled | Discharge diagnostic trapezoidal integral of h dm. | kJ | Discharge diagnostic trapezoidal integral of h dm. |
E_transport_delta | Sampled discharge transport minus the endpoint balance. | kJ | Sampled discharge transport minus the endpoint balance. |
E_vessel_residual | Final minus initial energy less heat minus work and net transport. | kJ | Final minus initial energy less heat minus work and net transport. |
The selected process reports work input and power, reference states and entropy production where defined. Pump results distinguish the state-based result from the inlet-volume approximation; gas results retain the selected caloric or real-fluid model.
Polytropic compression, isentropic-efficiency compression and isothermal compression are different processes. Do not transfer an exponent or an efficiency between them as if it were the same input.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0Exit pressure must exceed inlet pressure. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0Exit pressure must exceed inlet pressure. |
mdot | Mass flow rate. | kg/s | mdot >= 0 |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | 0 < eta_c <= 1 |
n | Polytropic exponent: the constant in a path where pressure times volume to this power stays fixed. Zero gives constant pressure, one gives constant temperature for an ideal gas, and the specific heat ratio gives an isentropic path. | - | n > 0Positive prescribed pv^n exponent. Only ideal gas n=1 implies isothermal. Real-fluid exit temperature is solved from the EOS; interstage heat may have either sign. |
nstage | How many compression stages are used. | - | integer 1 <= nstage <= 64At most 63 thermal resets; no final aftercooler. This ceiling bounds computation and chart size. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Wdot | Rate of work transfer, that is, power. | kW | Ẇᵢₙ=ṁ wᵢₙ Gas train total power; liquid pump uses composition.pump_operation.Result.power. |
h2 | Specific enthalpy: internal energy plus pressure times specific volume. It exists because that combination appears every time a substance flows across a boundary, so it is a bookkeeping convenience that behaves like a property. | kJ/kg | Every inlet and exit state, including final enthalpy; pump uses evaluation.exit. |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | η_c=(h_2s-h_1)/(h_2-h_1) |
pi_opt | The intermediate pressure that minimises total work, which for two ideal stages is the geometric mean of the end pressures. | MPa | pᵢ=p₁(p₂/p₁)^(i/N) Ideal-gas equal-ratio rule applies to its declared heat model. Real-fluid allocation is user-specified or a validated candidate from 32 logarithmic search intervals, not a global-optimum certificate. |
w_in | Total shaft energy input per kilogram through all stages. | kJ/kg | Total shaft energy input per kilogram through all stages. |
Q_compression | Net heat into all compressor stages per kilogram. | kJ/kg | Net heat into all compressor stages per kilogram. |
Q_interstage | Net heat rejected between stages per kilogram; negative means heating. | kJ/kg | Net heat rejected between stages per kilogram; negative means heating. |
sigma | Entropy production: entropy that was created inside the boundary rather than carried across it. Zero for an ideal process, positive for every real one, and never negative. | kJ/(kg K) | Entropy produced by compression and thermal resets per kilogram. |
The graph marks the current reversible bound and, for valid heat-engine inputs, the claimed efficiency and verdict. COP diverges as the temperatures converge; a ratio beyond the plotted interval is identified explicitly while the numeric bound remains available.
The supplied-heat verdict here is a heat-engine test: heat enters from the hot reservoir and leaves to the cold reservoir. Use Cycle Energy Accounting for an actual refrigerator or heat pump. The three reversible ratios remain available as bounds, not predictions of actual machine performance.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
TH | Temperature of the hot reservoir. | K | TH > TC |
TC | Temperature of the cold reservoir. | K | TC > 0 |
Qin | Total heat supplied to a cycle over one complete circuit, counted as a positive quantity. | kJ | — |
Qout | Total heat rejected by a cycle over one complete circuit, counted as a positive quantity. | kJ | — |
Wcycle | Net work produced or consumed over one complete circuit of a cycle. | kJ | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta_max | The largest thermal efficiency any device can have between the two given reservoir temperatures. | - | η_max=1-T_C/T_H |
beta_max | The largest refrigeration coefficient of performance possible between the two given temperatures. | - | β_max=T_C/(T_H-T_C) |
gamma_max | The largest heat pump coefficient of performance possible between the two given temperatures. | - | γ_max=T_H/(T_H-T_C) |
sigma_cycle | Entropy produced over one complete circuit, obtained from the cycle integral of heat over boundary temperature. | kJ/K | σ_cycle=-∮δ Q/T |
verdict | The screen's judgement on whether the described process is impossible, reversible, or irreversible. | — | impossible, reversible, or irreversible |
The balance separates stored or transported entropy from entropy carried by heat and entropy produced. Per-segment results include entropy transfer and the equivalent constant temperature, followed by a reversible/possible/impossible verdict.
For a steady control volume, a varying boundary temperature describes spatial heat exchange, not time accumulation. Heat must be signed into the system; absolute-temperature mistakes can reverse the verdict.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
s1 | Specific entropy: the property that counts how much of a system's energy is no longer available to do work. It increases in every real process and stays put only in an ideal one. | kJ/(kg K) | — |
s2 | Specific entropy: the property that counts how much of a system's energy is no longer available to do work. It increases in every real process and stays put only in an ideal one. | kJ/(kg K) | — |
m | Mass of the system or of the sample being considered. | kg | — |
mdot | Mass flow rate. | kg/s | — |
Qdot | Rate of heat transfer. | kW | — |
Tb | Temperature of the boundary where the heat crosses. Not the temperature of the system, and using the system's temperature instead is the standard error. | K | — |
Q | Heat transferred across the boundary, taken as positive when it goes into the system. | kJ | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
DeltaS | Change in total entropy between the two states. | kJ/K | — |
sigma | Entropy production: entropy that was created inside the boundary rather than carried across it. Zero for an ideal process, positive for every real one, and never negative. | kJ/K | σ=S_2-S_1-∫δ Q/T_b |
sigmadot | Rate of entropy production. | kW/K | — |
verdict | The screen's judgement on whether the described process is impossible, reversible, or irreversible. | — | impossible, reversible, or irreversible |
Read actual and isentropic reference states together. The performance section reports efficiency, speeds when relevant and entropy generation, preserving the different turbine, compressor and nozzle definitions.
Do not use a turbine enthalpy ratio as a compressor efficiency. A measured state inconsistent with the selected device direction is not repaired by forcing a plausible ratio.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
device | Which device the efficiency definition is being applied to. | — | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Active only when the selected inverse/supplied-state direction uses exit temperature; otherwise calculated. |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | 0 < eta_t <= 1 |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | 0 < eta_c <= 1 |
eta_n | Isentropic nozzle efficiency: actual kinetic energy at the exit divided by what an ideal expansion would have produced. | - | 0 < eta_n <= 1 |
h_exit_given | Measured turbine outlet enthalpy per unit mass. | kJ/kg | Measured exit enthalpy; optional alternative to T or x. |
x_exit_given | Measured vapor mass fraction at the turbine outlet. | - | Measured wet-water exit quality. |
x_inlet_given | Water inlet quality; zero for saturated-liquid pump inlet. | - | Water inlet quality; zero for saturated-liquid pump inlet. |
V_inlet_given | Nozzle inlet speed. | m/s | Nozzle inlet speed. |
V_exit_given | Measured nozzle exit speed. | m/s | Measured nozzle exit speed. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
h2 | Specific enthalpy: internal energy plus pressure times specific volume. It exists because that combination appears every time a substance flows across a boundary, so it is a bookkeeping convenience that behaves like a property. | kJ/kg | Actual exit station for h; isentropic exit station for h_2s, both rendered and plotted separately. |
h_2s | The exit enthalpy an ideal, entropy-preserving process would have reached at the actual exit pressure. The reference the real exit is measured against. | kJ/kg | s₂ₛ=s₁, p₂ₛ=p₂ Actual exit station for h; isentropic exit station for h_2s, both rendered and plotted separately. |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | — |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | — |
eta_n | Isentropic nozzle efficiency: actual kinetic energy at the exit divided by what an ideal expansion would have produced. | - | — |
x2 | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | - | — |
e_actual | Nozzle: actual exit kinetic energy. Other devices: magnitude of actual specific work. | kJ/kg | Nozzle: actual exit kinetic energy. Other devices: magnitude of actual specific work. |
e_isentropic | Nozzle: ideal exit kinetic energy. Other devices: magnitude of ideal specific work. | kJ/kg | Nozzle: ideal exit kinetic energy. Other devices: magnitude of ideal specific work. |
vel | Velocity of the stream, which matters only when it is fast enough for its kinetic energy to compete with its enthalpy. | m/s | Nozzle only: actual exit speed. |
vel_isentropic | Nozzle only: ideal exit speed. | m/s | Nozzle only: ideal exit speed. |
sigma | Entropy production: entropy that was created inside the boundary rather than carried across it. Zero for an ideal process, positive for every real one, and never negative. | kJ/(kg K) | Specific entropy increase across the adiabatic device. |
Read initial and final specific and total exergy, their total change, heat and work exergy, entropy production and its signed destruction diagnostic. Volume change is derived from the states and mass. Check the independent first-law residual, entropy-production assessment and exergy residual. The chart contains signed totals on the same mass basis and is available only when the physical checks pass. Export Readings keeps initial, final and environmental state groups distinct; graph export retains the signed bars and units.
A finite calculation may still be an impossible process. Negative entropy production is shown and does not become a physical negative loss bar. Very small nonzero state changes, near-dead water availability and near-cancelling heat-exergy contributions can be refused as unresolved; this does not mean zero exergy. Chemical exergy is excluded.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
model | Which equation of state the screen is evaluating. | — | water IF97; ideal gas; given constant c and vThe same model and substance resolve initial, final and environment states. |
substance | Which working fluid the screen is operating on. | — | declared gas species and mixturesWater is fixed in IF97 mode; no named-material database is assumed for given c and v. |
m | Mass of the system or of the sample being considered. | kg | finite and positiveThe same mass for both states and all totals. |
T0 | Dead-state temperature: the temperature of the environment the system is eventually going to equilibrate with. Exergy is meaningless without it. | K | finite and positive; inside the selected property domainEditable environment temperature. |
p0 | Dead-state pressure: the pressure of that same environment. | MPa | finite and positive; inside the selected property domainEditable environment pressure. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | selected property domainWater uses an explicit p,T or p,x pair; gas and given c/v use p,T. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | selected property domainWater uses an explicit p,T or p,x pair; gas and given c/v use p,T. |
x1 | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | — | selected property domainWater uses an explicit p,T or p,x pair; gas and given c/v use p,T. |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | selected property domainWater uses an explicit p,T or p,x pair; gas and given c/v use p,T. |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | selected property domainWater uses an explicit p,T or p,x pair; gas and given c/v use p,T. |
x2 | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | — | selected property domainWater uses an explicit p,T or p,x pair; gas and given c/v use p,T. |
Q | Heat transferred across the boundary, taken as positive when it goes into the system. | kJ | finite, signedTotal heat into contents. |
Tb | Temperature of the boundary where the heat crosses. Not the temperature of the system, and using the system's temperature instead is the standard error. | K | finite and positiveConstant boundary temperature or initial endpoint of a linear-in-heat law. |
Tb_end | The final absolute boundary temperature in a declared linear-in-transferred-heat path. | K | finite and positiveActive only for the linear-in-heat boundary temperature law. |
W | Work transferred across the boundary, taken as positive when it comes out of the system. | kJ | finite, signedTotal work out; derive from first law or check the entered value. |
velocity_in | The speed of the initial contents relative to the environment at rest. | m/s | finite and nonnegativeInitial speed; environment at rest. |
velocity_out | The final speed relative to the same environment. | m/s | finite and nonnegativeFinal speed. |
elevation_in | Initial height relative to the common environmental zero-height datum. | m | finite, signedInitial elevation relative to one common environmental datum. |
elevation_out | Final height relative to the same datum. | m | finite, signedFinal elevation relative to the same datum. |
c | The user-supplied constant specific heat capacity of the incompressible idealisation. | kJ/(kg K) | finite and positiveGiven heat capacity, only for the incompressible idealisation. |
v | Specific volume: the space one kilogram of the substance occupies. The reciprocal of density, and the property that makes a gas different from a liquid. | m^3/kg | finite and positiveGiven fixed specific volume, only for the incompressible idealisation. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
E1 | Exergy of a closed system: the most work its contents could still deliver as they come to equilibrium with the stated environment. | kJ | Total initial stored exergy. |
E2 | Exergy of a closed system: the most work its contents could still deliver as they come to equilibrium with the stated environment. | kJ | Total final stored exergy. |
e1 | Exergy per unit mass of a closed system. | kJ/kg | Specific initial stored exergy. |
e2 | Exergy per unit mass of a closed system. | kJ/kg | Specific final stored exergy. |
DeltaE | Change in exergy between the two states. | kJ | Δ E=E_q-E_w-E_d Evaluated from endpoint potentials; closure checked independently. |
Eq | Exergy that came along with a heat transfer, which is less than the heat itself by the reversible factor. | kJ | E_q=∫(1-T_0/T_b)δ Q Signed heat exergy; may be negative. |
Ew | Exergy that came along with a work transfer, less whatever was spent pushing the atmosphere aside. | kJ | E_w=W-p_0Δ V Signed work exergy out; volume is derived from the two states and mass. |
Ed | Exergy destroyed: work potential that was permanently lost, equal to the dead-state temperature times the entropy produced. | kJ | E_d=T_0σ A negative value is retained as an impossible-process diagnostic, never interpreted as physical destruction. |
sigma | Entropy production: entropy that was created inside the boundary rather than carried across it. Zero for an ideal process, positive for every real one, and never negative. | kJ/K | σ=Δ S-∫δ Q/T_b Independent entropy balance. |
DeltaV | Total final volume minus total initial volume for the same mass. | m^3 | Derived total volume change. |
DeltaS | Change in total entropy between the two states. | kJ/K | Total entropy change. |
energy_residual | Heat in minus work out minus the total energy change; a closed process requires zero within numerical resolution. | kJ | R_U=Q-W-Δ U-Δ KE-Δ PE Independent first-law residual. |
exergy_residual | Heat exergy minus work exergy minus entropy-derived destruction minus stored-exergy change. | kJ | R_E=E_q-E_w-E_d-Δ E Exergy closure; not used to define destruction. |
The exergy account reports stream exergies, useful product, supplied resource, destruction and closure with device-specific efficiency definitions. States and notes explain heat, mechanical-energy and environmental contributions.
For direct mixing, both streams share the same fluid model and pressure. Different cold-side fluids are available only in the non-mixing exchanger. Keep specific-energy and rate bases distinct, and read the reference environment and external heat sign with the exergy balance.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
T0 | Dead-state temperature: the temperature of the environment the system is eventually going to equilibrate with. Exergy is meaningless without it. | K | — |
p0 | Dead-state pressure: the pressure of that same environment. | Pa | — |
mdot | Mass flow rate. | kg/s | — |
component | Which component of the plant is being examined. | — | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
T2 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
Qdot | Rate of heat transfer. | kW | finite signed; zero is adiabaticFirst five devices: total external heat rate, positive in. For combustion, environmental heat is solved as an output instead. |
Tb | Temperature of the boundary where the heat crosses. Not the temperature of the system, and using the system's temperature instead is the standard error. | K | finite positive when Qdot is nonzeroFirst five devices: lumped boundary temperature; combustion fixes heat exchange at its chemical reference temperature. |
Wdot | Rate of work transfer, that is, power. | kW | Calculated signed shaft power output; turbine positive, compressor/pump negative, heat exchangers/mixing/throttle/combustor zero. |
V1 | Hot or single-stream inlet speed in the fixed laboratory frame. | m/s | finite; speeds nonnegative; g positiveHot or single-stream inlet speed in the fixed laboratory frame. |
V2 | Hot/single outlet; common mixed outlet for direct mixing. | m/s | finite; speeds nonnegative; g positiveHot/single outlet; common mixed outlet for direct mixing. |
Vc1 | Cold inlet speed for a two-stream exchanger. | m/s | finite; speeds nonnegative; g positiveCold inlet speed for a two-stream exchanger. |
Vc2 | Cold outlet speed for non-mixing exchange. | m/s | finite; speeds nonnegative; g positiveCold outlet speed for non-mixing exchange. |
z1 | Hot/single-stream inlet elevation. | m | finite; speeds nonnegative; g positiveHot/single-stream inlet elevation. |
z2 | Hot/single/common-mixed outlet elevation. | m | finite; speeds nonnegative; g positiveHot/single/common-mixed outlet elevation. |
zc1 | Cold inlet elevation. | m | finite; speeds nonnegative; g positiveCold inlet elevation. |
zc2 | Non-mixing cold outlet elevation. | m | finite; speeds nonnegative; g positiveNon-mixing cold outlet elevation. |
z0 | Environmental elevation datum; environment at rest. | m | finite; speeds nonnegative; g positiveEnvironmental elevation datum; environment at rest. |
g | Positive local gravitational acceleration. | m/s² | finite; speeds nonnegative; g positivePositive local gravitational acceleration. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
ef | Flow exergy: the most work a unit of a flowing stream could deliver as it comes to the dead state, including its kinetic and potential energy. | kJ/kg | e_f=(h-h_0)-T_0(s-s_0)+V²/2000+g(z-z_0)/1000 Mass h in kJ/kg, s in kJ/(kg K), speed m/s, elevation m; fixed laboratory frame. |
Efdot | Rate at which exergy is carried by a stream. | kW | Ė_f=ṁe_f |
Eqdot | Rate at which exergy accompanies a heat transfer. | kW | Ė_q=(1-T_0/T_j)Q̇_j |
Eddot | Rate of exergy destruction. | kW | Ė_d=T_0σ̇ |
epsilon | Exergetic efficiency: what the component actually delivered as a fraction of the exergy it was given. It asks a harder question than thermal efficiency and usually gets a worse answer. | - | — |
Wdot | Rate of work transfer, that is, power. | kW | Ẇ=Q̇+Σᵢₙṁ(h+k+gz)-Σₒᵤₜṁ(h+k+gz) Displayed as signed output; mechanical units converted consistently to kJ/kg. |
The water route reports sampled work, the same-duty inlet-volume shortcut, h₁ − h₂ and the signed quadrature discrepancy. Its v(p) area chart has linear axes, inlet/outlet marks and a constant-volume guide, and exports PNG/PDF/SVG. Choose 2–401 integer samples; no partial result is retained when a state fails.
Resolved saturation crossings are added to the requested base mesh and shown as labelled vertices. Actual node count may therefore increase. Possible near-critical excluded crossings or unresolved IF97 seam entropies are refused even with a coarse mesh. The work is an integral along a chosen reversible path. It is not a compressor power prediction until losses and mass flow are supplied in the appropriate device calculation.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
v_liquid | Given constant specific volume for the independent incompressible shortcut. | m^3/kg | positive finiteGiven constant specific volume for the independent incompressible shortcut. |
p_liquid_in | Incompressible shortcut inlet pressure. | MPa | Incompressible shortcut inlet pressure. |
p_liquid_out | Incompressible shortcut outlet pressure. | MPa | Incompressible shortcut outlet pressure. |
v_gas_in | Given initial specific volume for the independent isothermal/polytropic gas shortcuts. | m^3/kg | Given initial specific volume for the independent isothermal/polytropic gas shortcuts. |
p_gas_in | Gas-shortcut inlet pressure. | MPa | Gas-shortcut inlet pressure. |
p_gas_out | Gas-shortcut outlet pressure. | MPa | Gas-shortcut outlet pressure. |
n | Polytropic exponent: the constant in a path where pressure times volume to this power stays fixed. Zero gives constant pressure, one gives constant temperature for an ideal gas, and the specific heat ratio gives an isentropic path. | - | Gas-shortcut polytropic exponent. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Water IF97 isentrope inlet pressure. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Water IF97 isentrope inlet temperature. |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Water IF97 isentrope outlet pressure. |
samples | Requested logarithmic-pressure quadrature nodes. | - | integer 2 to 401Base logarithmic-pressure quadrature nodes. Resolved saturation intersections are inserted in addition, so actual node count may be greater. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
w_rev | Reversible work per unit mass for a steady-flow device. | kJ/kg | w=-∫₁² v dp |
w_incompressible | The same work computed with the specific volume held constant, which is the shortcut used for pumps. | kJ/kg | w=-v₁(p₂-p₁) |
w_isothermal | Reversible ideal-gas isothermal shortcut using the independent gas input group. | kJ/kg | w=-p₁v₁ ln (p₂/p₁) Reversible ideal-gas isothermal shortcut using the independent gas input group. |
w_polytropic | The same work computed along a polytropic path. | kJ/kg | w=n(p₂v₂-p₁v₁)/(1-n) |
w_isentropic | Reversible adiabatic work per mass from the inlet and outlet enthalpy difference. | kJ/kg | w=h₁-h₂ Isentropic endpoint identity; compared with the sampled integral. |
w_quadrature_delta | Sampled reversible work minus the isentropic endpoint enthalpy difference. | kJ/kg | w_{sampled}-(h_1-h_2) Observed numerical discrepancy, not an uncertainty bound. |
integration_nodes | Pressure nodes actually used in the quadrature, including resolved saturation intersections. | - | Actual node count after inserting saturation intersections. |
saturation_crossings | Resolved liquid/vapour saturation intersections inserted into a property path. | - | Number of explicitly inserted resolved saturation intersections. |
Single-loop results include mass flow, power, heat rates, efficiency and component work/entropy changes. Binary results add flow ratio, both flows, combined power/efficiency, external heat totals, internal exchanger duty/entropy production, energy residual and two distinct temperature-approach estimates. Split cogeneration adds individual turbine/pump powers, industrial process heat, liquid mixing entropy production, electrical efficiency and heat-and-power utilization. The energy bars distinguish useful heat from electricity. Export the current results table or current chart.
Very small pressure or enthalpy differences are refused when work is unresolved. Saturated admission is unavailable above critical pressure; the boiler regime is labelled. Water erosion limits are not applied to refrigerants. Pressure scans are finite samples. Binary temperature crossing may occur between apparently valid terminals; an unresolved temperature bracket is reported separately from a physical crossing. The exchanger chart uses transferred heat fraction, not physical length, and does not size an exchanger. With steam pressure drop, endpoints do not determine the internal path; an optional linear-pressure plot establishes sampled values only. A zero process fraction disables return temperature. Near-isothermal mixing is refused when entropy production cannot be resolved; this is a numerical limit, not a physical ban on mixing.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
fluid | The chosen working substance and its property model. | - | water, R134a, NH3, propane, R22One fluid model is used for every state, including ideal pump and turbine PS states. In binary mode water is the topping fluid and this selection identifies the bottoming fluid. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | Turbine inlet, boiler pressure. |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Turbine inlet; equals saturation temperature if no superheat. |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | Condenser pressure. |
mdot | Mass flow rate. | kg/s | mdot > 0, finiteActive in mass-flow rating mode. Net-power rating instead solves for mass flow. |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | 0 < eta_t <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
eta_p | Isentropic pump efficiency, defined the same way round as the compressor value. | - | 0 < eta_p <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
Wdot_net | Net power: what the turbines produce less what the pumps and compressors take. | kW | positive finiteActive only when net power is the selected rating. |
scan_lower | The first pressure sampled in a finite pressure scan. | MPa | positive finite, below upper boundLower sampled boiler or condenser pressure. |
scan_upper | The final pressure sampled in a finite pressure scan. | MPa | finite, above lower boundUpper sampled boiler or condenser pressure; other inputs stay fixed. |
p_b_hi | Bottoming boiler pressure in binary mode. | MPa | positive finiteBottoming boiler pressure in binary mode. |
p_b_lo | Bottoming condenser pressure. | MPa | 0 < p_b_lo < p_b_hiBottoming condenser pressure. |
T_b1 | Optional bottoming turbine inlet temperature; omit for saturated vapour. | K | within selected EOS rangeOptional bottoming turbine inlet temperature; omit for saturated vapour. |
eta_tb | Bottoming turbine isentropic efficiency. | - | 0 < eta_tb <= 1Bottoming turbine isentropic efficiency. |
eta_pb | Bottoming pump isentropic efficiency. | - | 0 < eta_pb <= 1Bottoming pump isentropic efficiency. |
p_return | Split cogeneration common pressure of exchanger condensate and process return. | MPa | 0 < p_return <= p_exhaust < p_boilerSplit cogeneration common pressure of exchanger condensate and process return. |
p_exhaust | Steam exhaust pressure before the process/exchanger split. | MPa | p_return <= p_exhaust < p_boilerSteam exhaust pressure before the process/exchanger split. |
y_process | Fraction of full steam flow sent to process heating; the rest feeds the exchanger. | - | 0 <= y_process < 1Fraction of full steam flow sent to process heating; the rest feeds the exchanger. |
T_return | Process return temperature; inactive when process fraction is zero. | K | resolved liquid at return pressureProcess return temperature; inactive when process fraction is zero. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | η=(wₜ-wₚ)/qᵢₙ |
bwr | Back work ratio: the fraction of the turbine's output that is immediately spent driving the compressor or pump. Small for a vapour plant, large for a gas turbine, and that difference explains a great deal. | - | bwr=wₚ/wₜ |
Wdot_net | Net power: what the turbines produce less what the pumps and compressors take. | kW | — |
Qdot_in | Rate of heat supplied to the cycle. | kW | — |
Qdot_out | Rate of heat rejected by the cycle. | kW | — |
x2 | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | - | Turbine exit quality exists only in the two-phase region. The erosion warning applies to water only. |
mdot | Mass flow rate. | kg/s | — |
w_turbine | Work delivered by the turbine per kilogram of working fluid. | kJ/kg | turbine work |
w_pump | Work supplied to the pump per kilogram of working fluid. | kJ/kg | pump work |
sigma_t | Entropy produced in the adiabatic turbine per kilogram of working fluid. | kJ/(kg K) | turbine specific entropy generation |
sigma_p | Entropy produced in the adiabatic pump per kilogram of working fluid. | kJ/(kg K) | pump specific entropy generation |
mass_ratio | Bottoming mass flow divided by steam mass flow. | - | Bottoming mass flow divided by steam mass flow. |
mdot_hot | Steam mass flow. | kg/s | Steam mass flow. |
mdot_cold | Bottoming mass flow. | kg/s | Bottoming mass flow. |
Qdot_exchange | Internal steam-condenser/bottom-boiler heat rate, excluded from external heat totals. | kW | Internal steam-condenser/bottom-boiler heat rate, excluded from external heat totals. |
Sdot_gen_exchange | Sum of both streams entropy-flow changes. | kW/K | Sum of both streams entropy-flow changes. |
approach_bound | Lower temperature-approach estimate using forward-property brackets and a numerical error budget; temperature interval, not absolute temperature. | K | Lower temperature-approach estimate using forward-property brackets and a numerical error budget; temperature interval, not absolute temperature. |
sampled_approach | Minimum computed temperature difference at sampled heat fractions. | K | Minimum computed temperature difference at sampled heat fractions. |
energy_closure | External heat input minus external rejection and combined power. | kW | External heat input minus external rejection and combined power. |
Wdot_turbine | Turbine work rate; separate rows distinguish steam and bottoming machines. | kW | Turbine work rate; separate rows distinguish steam and bottoming machines. |
Wdot_pump | Pump work rate; full mixed steam flow passes through the feed pump. | kW | Pump work rate; full mixed steam flow passes through the feed pump. |
Qdot_process | Industrial process heat delivered by the split steam flow. | kW | Industrial process heat delivered by the split steam flow. |
utilization | Net electrical power plus useful process heat divided by external boiler heat; distinct from electrical efficiency. | - | Net electrical power plus useful process heat divided by external boiler heat; distinct from electrical efficiency. |
Sdot_gen_mix | Adiabatic mixer entropy-flow increase at the common return pressure. | kW/K | Adiabatic mixer entropy-flow increase at the common return pressure. |
The selected cycle gives station properties and performance. Design mode adds recovered reheat pressure, comparison efficiency and any boundary-limit explanation; the state diagram follows the selected solution.
The pressure search refines feasible intervals found by a logarithmic scan. A boundary-limited efficiency is approached, not an attained interior maximum, and narrow unsampled regions are not certified.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | Reheat pressure, the free parameter. |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Reheat outlet temperature. |
p4 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | Condenser pressure. |
x_target | A target value for a quantity the screen is solving backwards from, such as a required turbine exit quality. | - | Target turbine exit quality, when solving for reheat pressure. |
mdot | Mass flow rate. | kg/s | — |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | 0 < eta_t <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
eta_p | Isentropic pump efficiency, defined the same way round as the compressor value. | - | 0 < eta_p <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
p_reheat_second | Second reheater pressure, strictly between first reheater and condenser. | MPa | Second reheater pressure, strictly between first reheater and condenser. |
T_reheat_second | Second reheater outlet temperature. | K | Second reheater outlet temperature. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | Selected complete cycle; Wdot_net is mass flow times specific net work. Final turbine quality is absent for a superheated exit. |
bwr | Back work ratio: the fraction of the turbine's output that is immediately spent driving the compressor or pump. Small for a vapour plant, large for a gas turbine, and that difference explains a great deal. | - | Selected complete cycle; Wdot_net is mass flow times specific net work. Final turbine quality is absent for a superheated exit. |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | Last reheater pressure: supplied, refined efficiency optimum, or selected target-quality root. |
x4 | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | - | Selected complete cycle; Wdot_net is mass flow times specific net work. Final turbine quality is absent for a superheated exit. |
Wdot_net | Net power: what the turbines produce less what the pumps and compressors take. | kW | Selected complete cycle; Wdot_net is mass flow times specific net work. Final turbine quality is absent for a superheated exit. |
The cycle accounts for the reduced turbine flow after each extraction, feedwater heating and drain/pump work. Results include per-boiler-mass quantities, scaled rates and the selected cycle diagram.
All heaters use the selected type. Arbitrary mixtures of heater types or piping networks are not available. Invalid pressure order, negative extraction fractions and ill-conditioned balances are refused.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Extraction pressure. |
p3 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | Condenser pressure. |
nheater | How many feedwater heaters are in the arrangement. | - | 1 <= nheater <= 8Integer number of explicit heaters. |
mdot | Mass flow rate. | kg/s | mdot >= 0Boiler flow; zero reports zero rates while retaining per-unit-mass design results. |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | 0 < eta_t <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
eta_p | Isentropic pump efficiency, defined the same way round as the compressor value. | - | 0 < eta_p <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
y | Extraction fraction: the share of the steam bled off at an intermediate pressure to heat the feedwater. It comes out of an energy balance, never in as an input. | - | One resolved extraction fraction per heater, relative to boiler flow. |
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | — |
Wdot_net | Net power: what the turbines produce less what the pumps and compressors take. | kW | — |
Qdot_in | Rate of heat supplied to the cycle. | kW | — |
x | Quality: the fraction of a liquid-vapour mixture that is vapour, by mass. Meaningful only between the two saturation lines. | - | Last turbine-stage exit quality, when two-phase. |
The Otto-cycle results give heat addition/rejection, compression and expansion work, net work, efficiency and mean effective pressure. Both caloric choices use the selected input basis for every station.
This air-standard cycle models external heat addition, not fuel chemistry or real intake/exhaust strokes. Match the heat-input convention before comparing caloric models.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
r | Compression ratio: the volume before compression divided by the volume after it. | - | r > 1Compression ratio. |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Peak temperature. |
Qin | Total heat supplied to a cycle over one complete circuit, counted as a positive quantity. | kJ/kg | Heat added per unit mass, as an alternative to peak temperature. |
k | Specific heat ratio: cp divided by cv. It governs how steeply temperature changes when a gas is compressed without heat transfer. | - | Specific heat ratio for the cold-air-standard branch. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | η=1-(u₄-u₁)/(u₃-u₂) |
mep | Mean effective pressure: the constant pressure that would produce the same net work over the same swept volume. It lets engines of different size be compared. | Pa | mep=W_cycle/(V_1-V_2) |
Wcycle | Net work produced or consumed over one complete circuit of a cycle. | kJ/kg | — |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p3 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
The Diesel-cycle results include heat, work, efficiency, mean effective pressure and the expanded state sequence. The cutoff ratio explains how far the piston moves during constant-pressure heat addition.
Comparing with an Otto cycle at equal compression ratio is a specified theoretical comparison, not a claim that practical engines operate at equal compression ratios.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
r | Compression ratio: the volume before compression divided by the volume after it. | - | r > 1 |
rc | Cutoff ratio: how far the piston has travelled by the time heat addition stops, as a volume ratio. | - | rc > 1Cutoff ratio. |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
k | Specific heat ratio: cp divided by cv. It governs how steeply temperature changes when a gas is compressed without heat transfer. | - | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | — |
mep | Mean effective pressure: the constant pressure that would produce the same net work over the same swept volume. It lets engines of different size be compared. | Pa | — |
Wcycle | Net work produced or consumed over one complete circuit of a cycle. | kJ/kg | — |
rc | Cutoff ratio: how far the piston has travelled by the time heat addition stops, as a volume ratio. | - | r_c=V_3/V_2 |
The dual-cycle account reports both heat-addition legs, work, efficiency and peak conditions. The diagram shows which part of heating occurs before and after the piston begins its constant-pressure motion.
Different input modes describe the same cycle only when their recovered split and peak state agree. Vanishing one heat-addition leg is a limiting cycle, not a reason to divide by its zero contribution.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
r | Compression ratio: the volume before compression divided by the volume after it. | - | r > 1 |
rp | Pressure ratio across the compressor, or in the dual cycle the pressure rise during the constant-volume part of heat addition. | - | rp >= 1Constant-volume pressure ratio. |
rc | Cutoff ratio: how far the piston has travelled by the time heat addition stops, as a volume ratio. | - | rc >= 1 |
k | Specific heat ratio: cp divided by cv. It governs how steeply temperature changes when a gas is compressed without heat transfer. | - | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | — |
mep | Mean effective pressure: the constant pressure that would produce the same net work over the same swept volume. It lets engines of different size be compared. | Pa | — |
Wcycle | Net work produced or consumed over one complete circuit of a cycle. | kJ/kg | — |
Cycle results and plots share the selected model. The design section reports net-work and efficiency optimum ratios, zero-work boundaries and a zero-heat-input boundary, with the selected ratio marked on the comparison curves.
Each pressure loss is a fraction of its own exchanger inlet pressure. A highest-efficiency limit at zero work is not a useful operating cycle and is not an attainable finite-power optimum.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | — |
rp | Pressure ratio across the compressor, or in the dual cycle the pressure rise during the constant-volume part of heat addition. | - | rp > 1Compressor pressure ratio. |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Turbine inlet temperature, the metallurgical limit. |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | 0 < eta_c <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | 0 < eta_t <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
mdot | Mass flow rate. | kg/s | finite mdot >= 0 with resolvable rates in selected unitsAir mass flow for plant rating. Zero flow gives zero rates; specific cycle properties and optimum ratios do not depend on flow. |
hot_pressure_loss | Fraction of combustor inlet pressure lost before turbine admission. | - | 0 <= hot_pressure_loss < 1Fraction of combustor inlet pressure lost before turbine admission. |
cold_pressure_loss | Fraction of heat-rejection inlet pressure lost before compressor admission. | - | 0 <= cold_pressure_loss < 1Fraction of heat-rejection inlet pressure lost before compressor admission. |
caloric_model | NASA polynomial, evaluated constant cp, or air-only cold-air standard. | - | NASA variable heat capacity or cold-air standardCold-air standard fixes its air heat capacities; k is not a separate editable field. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | — |
bwr | Back work ratio: the fraction of the turbine's output that is immediately spent driving the compressor or pump. Small for a vapour plant, large for a gas turbine, and that difference explains a great deal. | - | — |
Wdot_net | Net power: what the turbines produce less what the pumps and compressors take. | kW | Mass flow times specific net work; tuple element 0, kW. |
w_net | Net work per unit mass of working fluid. | kJ/kg | — |
rp_opt_work | The pressure ratio that produces the most work per unit of gas. | - | Bounded stationary search for the selected caloric model and losses; an efficiency limit at vanishing work cannot be applied. |
rp_opt_eta | The pressure ratio that produces the highest efficiency, which is a different and larger number. | - | Bounded stationary search for the selected caloric model and losses; an efficiency limit at vanishing work cannot be applied. |
Qdot_in | Rate of heat supplied to the cycle. | kW | Heat supply rate; tuple element 1, mass flow times the corresponding specific transfer. |
Qdot_out | Rate of heat rejected by the cycle. | kW | Heat rejection rate; tuple element 2, mass flow times the corresponding specific transfer. |
Wdot_compressor | Rate of shaft work supplied to the compressor. | kW | Compressor shaft input; tuple element 3, mass flow times the corresponding specific transfer. |
Wdot_turbine | Turbine work rate; separate rows distinguish steam and bottoming machines. | kW | Turbine shaft output; tuple element 4, mass flow times the corresponding specific transfer. |
The cycle includes interstage cooling, reheating and regeneration. The regenerator reports available heat, recovered heat and effectiveness read back from the states, alongside cycle efficiency and work.
Regeneration needs turbine exhaust hotter than compressor discharge. Ideal intercooling, reheating and equal stage allocation are model assumptions; this entry does not predict exchanger geometry or pressure losses.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
rp | Pressure ratio across the compressor, or in the dual cycle the pressure rise during the constant-volume part of heat addition. | - | — |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
eta_reg | Regenerator effectiveness: how much of the available temperature rise the regenerator actually delivers. | - | 0 <= eta_reg <= 1 |
nstage_c | How many compression stages, when compression and expansion are staged independently. | - | nstage_c >= 1 |
nstage_t | How many expansion stages. | - | nstage_t >= 1 |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | 0 < eta_c <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | 0 < eta_t <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | — |
bwr | Back work ratio: the fraction of the turbine's output that is immediately spent driving the compressor or pump. Small for a vapour plant, large for a gas turbine, and that difference explains a great deal. | - | — |
w_net | Net work per unit mass of working fluid. | kJ/kg | — |
eta_reg | Regenerator effectiveness: how much of the available temperature rise the regenerator actually delivers. | - | η_reg=(h_x-h_2)/(h_4-h_2) |
pi_opt | The intermediate pressure that minimises total work, which for two ideal stages is the geometric mean of the end pressures. | Pa | — |
The combined result reports steam per gas mass, steam flow, net power, efficiency, stack temperature, closest approach and energy closure. Both cycle diagrams accompany the shared heat-recovery profile.
Recovered exhaust heat is an internal transfer and must not be counted twice as external heat input. The reported pinch is a sampled temperature-profile constraint, not exchanger-area sizing.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
rp | Pressure ratio across the compressor, or in the dual cycle the pressure rise during the constant-volume part of heat addition. | - | — |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p6 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | Steam-side boiler pressure. |
T7 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Steam-side turbine inlet temperature. |
p8 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | Condenser pressure. |
mdot1 | Mass flow rate. | kg/s | Gas-side flow. |
DeltaT_pinch | Pinch-point temperature difference: the smallest gap between the two streams anywhere inside a heat recovery generator. It is the binding constraint on how much steam can be raised. | K | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
eta | Thermal efficiency: net work out divided by heat in. The fraction of what was paid for that came back as work. | - | — |
mdot6 | Mass flow rate. | kg/s | steam_per_gas is a mass ratio; the displayed steam flow multiplies it by the entered gas mass flow in PresentationIndustrialView.plantFlows. |
Wdot_net | Net power: what the turbines produce less what the pumps and compressors take. | kW | net_work_per_gas is kJ/kg; the displayed power multiplies it by the entered gas mass flow in PresentationIndustrialView.plantFlows. |
DeltaT_pinch | Pinch-point temperature difference: the smallest gap between the two streams anywhere inside a heat recovery generator. It is the binding constraint on how much steam can be raised. | K | — |
Results include thrust and specific thrust, exit velocity, station temperatures, compressor/turbine work, supplied heat and nozzle inlet stagnation enthalpy. The turbine work is matched to the compressor demand.
The model uses temperature-dependent air properties and momentum thrust for expansion to ambient. Fuel mass addition, choked-nozzle geometry and a separate pressure-thrust term are not solved.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Ambient. |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
vel1 | Velocity of the stream, which matters only when it is fast enough for its kinetic energy to compete with its enthalpy. | m/s | Flight velocity. |
rp | Pressure ratio across the compressor, or in the dual cycle the pressure rise during the constant-volume part of heat addition. | - | Compressor pressure ratio. |
T4 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Turbine inlet temperature. |
mdot | Mass flow rate. | kg/s | — |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | — |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | — |
eta_n | Isentropic nozzle efficiency: actual kinetic energy at the exit divided by what an ideal expansion would have produced. | - | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
vel6 | Velocity of the stream, which matters only when it is fast enough for its kinetic energy to compete with its enthalpy. | m/s | — |
F_thrust | Thrust produced by the engine. | N | F=ṁ(V₆-V₁) |
F_specific | Thrust per unit mass flow, which is what decides how big the engine has to be. | N s/kg | — |
h0 | Stagnation enthalpy: the enthalpy a stream would have if it were brought to rest without loss. Conserved through an adiabatic duct with no work. | kJ/kg | hₒ=h+V²/2 Stagnation enthalpy at the nozzle inlet. The displayed nozzle exit temperature is the actual static temperature, including nozzle efficiency. |
The account closes supplied exergy against net work, component destruction and exergy carried outside. Fuel mode adds fuel consumption, exhaust exergy and fuel-conversion/heat-supply destruction. Main rankings group components below 0.5% of supply, while retaining detailed rows.
Compare audits only with the same boundary and per-boiler-mass basis. Frozen combustion is not chemical equilibrium. Changing a sink temperature changes the split between destruction and carried-out exergy.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T0 | Dead-state temperature: the temperature of the environment the system is eventually going to equilibrate with. Exergy is meaningless without it. | K | — |
p0 | Dead-state pressure: the pressure of that same environment. | MPa | — |
cycle_ref | Which cycle, defined on another screen, this audit is being run against. | — | basic Rankine, single reheat, double reheat, regenerativeUse the existing M18–M20 topology, including explicit heater pressures and heater arrangement. |
Tsource | The temperature at which heat enters the plant, which is what fixes how much exergy came in with it. | K | Temperature at which heat enters the steam generator. |
mdot | Mass flow rate. | kg/s | finite, >= 0Boiler inlet mass flow; all extracted branch flows scale from this basis. Zero retains the per-kg design with zero rates. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
Eddot | Rate of exergy destruction. | kW | kW at the stated boiler inlet flow; per-boiler-kg values are also displayed. |
epsilon | Exergetic efficiency: what the component actually delivered as a fraction of the exergy it was given. It asks a harder question than thermal efficiency and usually gets a worse answer. | - | — |
Eloss | Exergy that left the boundary without being destroyed inside it, for instance in a hot exhaust stream. | kW | kW at the stated boiler inlet flow; per-boiler-kg values are also displayed. |
rank | The ordering of components by how much exergy each destroys, largest first. | — | Components ordered by destruction, largest first. |
Read the four actual station pressures, temperatures and phases with COP, duty, compressor power, rejection duty, mass/molar flow and flash fraction. Choose T–s, p–h, p–v or h–s for the same solved cycle.
The model label distinguishes four Helmholtz refrigerants from CO2's Peng–Robinson approximation. The reference-temperature Carnot COP is not a full external-reservoir calculation with varying exchanger temperatures.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | Four published Helmholtz fluids or approximate CO2 Peng–Robinson. |
Te_ref | Saturation temperature used to set the evaporator inlet pressure. | K | Saturation reference at evaporator inlet: sets p4, not p1. |
Tr_ref | Condenser inlet saturation reference, or gas-cooler outlet temperature in transcritical operation. | K | Subcritical: saturation reference sets condenser inlet p2. Transcritical: specified gas-cooler outlet T3. |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | MPa | p > 0Explicit compressor discharge pressure in transcritical mode; outlet p3 must remain above critical. |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | 0 < eta_c <= 1Adiabatic compressor isentropic efficiency. |
superheat | Temperature above local saturated vapour at the same pressure. | K | superheat >= 0Temperature increment above saturation at suction p1. |
subcool | Temperature below local saturated liquid at the same pressure. | K | subcool >= 0Temperature decrement below saturation at condenser outlet p3; exactly zero in transcritical mode. |
evaporator_loss | Fraction of evaporator inlet pressure lost through that exchanger. | - | 0 <= evaporator_loss < 1Fraction (p4-p1)/p4, based on its own exchanger inlet. |
rejection_loss | Fraction of heat-rejection inlet pressure lost through that exchanger. | - | 0 <= rejection_loss < 1Fraction (p2-p3)/p2, based on its own exchanger inlet. |
Qdot_L | Rate of heat removed from the cold side, which is the useful output of a refrigerator. | kW | Qdot_L >= 0Refrigerating capacity; zero retains the specific-state design. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
beta | Coefficient of performance of a refrigerator: heat removed from the cold space divided by the work it cost. Routinely greater than one, which is why it is not called an efficiency. | - | β=(h₁-h₄)/(h₂-h₁) |
Qdot_L | Rate of heat removed from the cold side, which is the useful output of a refrigerator. | kW | Q̇_L=ṁ(h_1-h_4) |
Wdot | Rate of work transfer, that is, power. | kW | — |
Qdot_H | Rate of heat delivered to the warm side, which is the useful output of a heat pump. | kW | — |
mdot | Mass flow rate. | kg/s | Converts the cycle kmol/s flow to kg/s with the selected fluid molar mass. |
tons | Refrigeration capacity expressed in the unit the industry actually uses, rather than in kilowatts. | ton | Refrigeration tons, because the industry states capacity that way. |
The selected cycle reports cooling duty, work input, rejection, COP, lowest temperature and internal heat transfer. Air results separate compressor and expander work; CO2 results retain its real-fluid state and exchanger limitations.
The two arrangements use different physical models. CO2's internal exchanger transfers enthalpy between its streams; an invalid pinch or phase state is refused rather than represented by a clipped effectiveness.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
rp | Pressure ratio across the compressor, or in the dual cycle the pressure rise during the constant-volume part of heat addition. | - | — |
T3 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Temperature after heat rejection. |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | — |
eta_t | Isentropic turbine efficiency: actual work out divided by the work an ideal expansion to the same pressure would have produced. | - | Air turbine only; the CO2 branch has an isenthalpic expansion valve. |
eta_reg | Regenerator effectiveness: how much of the available temperature rise the regenerator actually delivers. | - | Air regenerator effectiveness. CO2 branch instead labels this control cold-side enthalpy approach: a = q/[h(pLow,TgasCooler)-h6], validated by sampled temperature differences and positive entropy integration. |
mdot | Mass flow rate. | kg/s | — |
T_evap_CO2 | CO2 saturated-vapor evaporator exit temperature; property solver enforces its model range. | K | co2_triple_temperature < T_evap_CO2 < Tcrit_CO2CO2 saturated-vapor evaporator exit temperature; property solver enforces its model range. |
T_cooler_CO2 | CO2 gas-cooler exit temperature. | K | T_cooler_CO2 > Tcrit_CO2CO2 gas-cooler exit temperature. |
p_high_CO2 | Explicit discharge pressure for the CO2 automotive arrangement. | MPa | p_high_CO2 > pcrit_CO2Explicit discharge pressure for the CO2 automotive arrangement. |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
beta | Coefficient of performance of a refrigerator: heat removed from the cold space divided by the work it cost. Routinely greater than one, which is why it is not called an efficiency. | - | CO2 branch uses composition.co2_refrigeration.analyse: capacity/power already include kg/s to molar-state conversion; lowest temperature is taken over all six states. |
Qdot_L | Rate of heat removed from the cold side, which is the useful output of a refrigerator. | kW | The solver returns specific energy in kJ/kg. PresentationIndustrialView.refrigerationRates multiplies by the entered mass flow to produce kW. CO2 branch uses composition.co2_refrigeration.analyse: capacity/power already include kg/s to molar-state conversion; lowest temperature is taken over all six states. |
Wdot | Rate of work transfer, that is, power. | kW | The solver returns specific energy in kJ/kg. PresentationIndustrialView.refrigerationRates multiplies by the entered mass flow to produce kW. CO2 branch uses composition.co2_refrigeration.analyse: capacity/power already include kg/s to molar-state conversion; lowest temperature is taken over all six states. |
T5 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Lowest temperature reached, which is the figure of merit for cryogenic use. CO2 branch uses composition.co2_refrigeration.analyse: capacity/power already include kg/s to molar-state conversion; lowest temperature is taken over all six states. |
q_IHX_CO2 | CO2 internal heat transferred per unit mass. | kJ/kg | CO2 internal heat transferred per unit mass. |
sigma_IHX_CO2 | CO2 internal-HX entropy production rate; positive reciprocal-temperature integral times heat and mass flow. | kW/K | CO2 internal-HX entropy production rate; positive reciprocal-temperature integral times heat and mass flow. |
pinch_IHX_CO2 | Minimum sampled CO2 counterflow temperature difference over65 equal-duty points. | ΔK | Minimum sampled CO2 counterflow temperature difference over65 equal-duty points. |
Operating results include heating/cooling COP, capacity, compressor power, flow and suction volume. The balance-point section shows capacity and load curves, crossing status, supplementary heat and design-point combined COP. Export graph saves those same coordinates, both curve identities and the crossing/no-crossing status as PNG, PDF or SVG.
The operating outdoor-temperature field does not change the balance calculation's fixed design temperature. A missing crossing can mean the pump covers the displayed range or never covers it; read the curve and status. Design-point supplemental heating and combined COP are not a seasonal performance calculation.
| Symbol | Meaning | Unit | Valid range |
|---|---|---|---|
substance | Which working fluid the screen is operating on. | — | — |
p1 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
p2 | Pressure: the normal force a fluid exerts per unit of the area it pushes on. Always absolute inside the app; gauge is a display mode. | Pa | — |
T1 | Temperature: the property two bodies share when nothing flows between them on contact. Always absolute inside the app. | K | Evaporator, tracking outdoor temperature. |
eta_c | Isentropic compressor efficiency: the work an ideal compression would have taken divided by the work actually taken. | - | 0 < eta_c <= 1Isentropic efficiency: the actual device measured against the reversible one working between the same two states. The ratio is written so that it cannot exceed one, and reaches one only for a reversible machine. |
Qdot_H | Rate of heat delivered to the warm side, which is the useful output of a heat pump. | kW | Building heat demand. |
UA_building | How readily the building loses heat: its conductance to outdoors. | kW/K | — |
T_indoor | The indoor temperature the building is being held at. | K | — |
| Symbol | Meaning | Unit | Relation |
|---|---|---|---|
gamma | Coefficient of performance of a heat pump: heat delivered to the warm space divided by the work it cost. Always exactly one more than the refrigeration value for the same machine. | - | γ=(h₂-h₃)/(h₂-h₁) |
Qdot_H | Rate of heat delivered to the warm side, which is the useful output of a heat pump. | kW | — |
Wdot | Rate of work transfer, that is, power. | kW | — |
T_balance | The outdoor temperature at which a heat pump's capacity has fallen to exactly meet the building's demand. Below it, something else has to make up the difference. | K | Outdoor temperature at which capacity equals demand. |