Conditions
Composition
| Component | zi |
|---|
Sum: 1.0000
Tick a component to include it in the mixture. Newly ticked components start at 0 — enter a value.
Results
Enter conditions and composition, then click Calculate.
Model: Peng-Robinson (1978) cubic EOS, van der Waals one-fluid mixing rules, literature/simulator-default
binary interaction parameters (kij) for light hydrocarbon pairs. Ideal-gas Cp from Reid/Prausnitz/Poling
polynomials (
IBP / FBP (mixtures only): bubble-point and dew-point temperature at the input pressure, found via the PR-EOS flash engine. Flash Point is a theoretical estimate using Antoine vapor pressures and the Le Chatelier lower-flammability-limit (LFL) mixing rule at 1 atm, approximating liquid composition ≈ feed composition — it is not a substitute for a laboratory-measured flash point (ASTM D56/D93/D3278) and should not be used as the sole basis for fire-safety classification or regulatory compliance.
Extended component set (1,3-butadiene, n-butane, C5H10/1-pentene, benzene, toluene, n-hexane, methanol, VCM, EDC, HCl, chlorine, EO, EG): critical properties (Tc, Pc, ω) are literature-typical values, and untabulated binary pairs default to kij=0 (ideal mixing) — verify against DIPPR/NIST/a process simulator before design or safety use. Saturation-temperature (Antoine) and Flash Point estimates are not yet available for these components (density, Cp, and JT/enthalpy calculations are unaffected).
Cp° = A + BT + CT² + DT³); real-gas Cp includes PR departure function.
Liquid-phase density from PR EOS without volume translation — expect ~2–5% deviation from measured
saturated-liquid density; cross-check against plant data or a process simulator for custody-transfer /
fiscal use. Not a substitute for validated process simulation for safety-critical design.
IBP / FBP (mixtures only): bubble-point and dew-point temperature at the input pressure, found via the PR-EOS flash engine. Flash Point is a theoretical estimate using Antoine vapor pressures and the Le Chatelier lower-flammability-limit (LFL) mixing rule at 1 atm, approximating liquid composition ≈ feed composition — it is not a substitute for a laboratory-measured flash point (ASTM D56/D93/D3278) and should not be used as the sole basis for fire-safety classification or regulatory compliance.
Extended component set (1,3-butadiene, n-butane, C5H10/1-pentene, benzene, toluene, n-hexane, methanol, VCM, EDC, HCl, chlorine, EO, EG): critical properties (Tc, Pc, ω) are literature-typical values, and untabulated binary pairs default to kij=0 (ideal mixing) — verify against DIPPR/NIST/a process simulator before design or safety use. Saturation-temperature (Antoine) and Flash Point estimates are not yet available for these components (density, Cp, and JT/enthalpy calculations are unaffected).
Inlet / Outlet Conditions
Adiabatic, isenthalpic (H1=H2) pressure reduction — e.g. across a control
valve or PRV. P2 must be less than P1. Solves for outlet T2 such that real-gas enthalpy
(PR EOS departure + ideal-gas Cp integral) is conserved.
Feed Composition
| Component | zi |
|---|
Sum: 1.0000
Tick a component to include it in the feed. Newly ticked components start at 0 — enter a value.
Results
Enter conditions and feed composition, then click Calculate T2.
Method: (1) Flash the feed at (T1,P1) via PR-EOS fugacities to get inlet molar
enthalpy H1 = ideal-gas Cp integral + phase-fraction-weighted PR departure function. (2) Search T2 at
P2 by bisection until H(T2,P2) = H1. For a pure component, phase change at fixed P
happens at a single saturation temperature (a true latent-heat jump in H, not a smooth kink) — so if
H1 falls between the saturated-liquid and saturated-vapor enthalpies at Tsat(P2), the
outlet is exactly at Tsat(P2) with vapor fraction from an enthalpy lever-rule balance,
rather than from a naive continuous T-search (which would straddle the discontinuity incorrectly).
For a mixture, the two-phase region spans a continuous range of T at fixed P, so
direct bisection on T finds the two-phase solution directly.
For extended-set pure components without a loaded Antoine correlation, the saturation-temperature clamp at Tsat(P2) is skipped and the solver goes straight to bisection on T — this is fine away from a phase change, but can be less precise exactly at one.
For extended-set pure components without a loaded Antoine correlation, the saturation-temperature clamp at Tsat(P2) is skipped and the solver goes straight to bisection on T — this is fine away from a phase change, but can be less precise exactly at one.
Reference Conditions (volumetric basis)
Molar and mass-basis calorific values don't depend on this choice. Reference pressure fixed at
1 atm (101.325 kPa). Volumetric conversion uses the ideal-gas law — a simplified version of the
real-gas compressibility (summation-factor) correction in full ISO 6976 / GPA 2172; adequate for
typical fuel-gas heating value estimates but not for custody-transfer-grade certification.
Composition
| Component | zi |
|---|
Sum: 1.0000
Tick a component to include it in the mixture. Newly ticked components start at 0 — enter a value.
Results
Enter composition, then click Calculate.
Method: Molar GCV/NCV = Σ zi·(GCV or NCV)i, using
standard ideal-gas heats of combustion at 25°C (GPA 2145 / ISO 6976-consistent values; product
water liquid for GCV/gross/HHV, vapor for NCV/net/LHV). Mass basis divides by mixture MW. Volumetric
basis divides by the ideal-gas molar volume at the selected reference conditions. Specific gravity is
mixture MW over dry-air MW (28.9647 g/mol); Wobbe Index = volumetric CV / √(specific gravity).
Oxygen, Nitrogen, and Water are treated as inert (zero heating value) — they dilute the mixture but
don't consume heat in this convention.
Extended-set heats of combustion (butadiene, butane, C5H10, benzene, toluene, hexane, methanol, VCM, EDC, EO, EG) are approximate literature values; HCl and Chlorine are treated as inert (zero heating value) since they don't combust. Chlorinated species form HCl on combustion rather than only CO2/H2O, so treat their listed values as indicative only — verify before fiscal/custody use.
Extended-set heats of combustion (butadiene, butane, C5H10, benzene, toluene, hexane, methanol, VCM, EDC, EO, EG) are approximate literature values; HCl and Chlorine are treated as inert (zero heating value) since they don't combust. Chlorinated species form HCl on combustion rather than only CO2/H2O, so treat their listed values as indicative only — verify before fiscal/custody use.
Stream 1 — Conditions
Stream 1 — Composition
| Component | zi |
|---|
Sum: 1.0000
Tick a component to include it in Stream 1.
Stream 2 — Conditions
Stream 2 — Composition
| Component | zi |
|---|
Sum: 1.0000
Tick a component to include it in Stream 2.
Mixed Outlet — Pressure
Outlet temperature is solved from an adiabatic, steady-state energy balance
(F1H1+F2H2=FtotalHmix) at this pressure —
it is not an input.
Results
Enter both streams' conditions and composition, then click Calculate Mix.
Method: each inlet stream's molar enthalpy is evaluated at its own T, P, and
declared phase (ideal-gas Cp° integral + PR-EOS departure, same convention as the
Density & Cp tab). The two streams are combined on a molar basis into a single feed composition,
and the outlet temperature at the specified final pressure is found by solving the steady-state,
adiabatic energy balance F1H1 + F2H2 = Ftotal·Hmix(T,Pf).
No heat loss, no shaft work, and no pressure-drop-induced flashing beyond what the energy balance itself
predicts are assumed (a real tee/header may lose heat to ambient or have a different pressure profile).
The outlet phase (vapor / liquid / two-phase) is not assumed — it is determined rigorously from a PT flash (Rachford-Rice + PR fugacity coefficients) on the combined composition at the solved temperature and specified pressure, exactly as in the Isenthalpic (JT) tab. If the result is two-phase, vapor and liquid density/Cp are reported separately in addition to the flow-weighted apparent values.
The outlet phase (vapor / liquid / two-phase) is not assumed — it is determined rigorously from a PT flash (Rachford-Rice + PR fugacity coefficients) on the combined composition at the solved temperature and specified pressure, exactly as in the Isenthalpic (JT) tab. If the result is two-phase, vapor and liquid density/Cp are reported separately in addition to the flow-weighted apparent values.