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Steam & Water Properties
IAPWS-IF97 · pyXSteam Engine · Compressed Liquid · Saturated · Wet Steam · Superheated · SI & Imperial
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IAPWS-IF97
Regions 1–5
0.01–800°C
0–1000 bar
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Thermodynamic Terms & Definitions — IAPWS-IF97
Formulas · Engineering significance · Accuracy notes · Key reference values
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Thermodynamic Terms & Definitions
IAPWS-IF97 properties — formulas, engineering use & accuracy
Property Definitions
Specific Enthalpy
h
h = u + P·v
Total thermodynamic energy per unit mass — internal energy plus flow work (P·v). The key property for boiler, heat exchanger, and turbine design. For open systems: Q = ṁ·Δh.
SI: kJ/kg  |  Imperial: BTU/lb
Specific Entropy
s
ds = δQrev / T
Measure of molecular disorder per unit mass. Constant in ideal isentropic processes (turbines, compressors). Higher entropy = more energy degraded. Always increases in real processes.
SI: kJ/(kg·K)  |  Imperial: BTU/(lb·°R)
Internal Energy
u
u = h − P·v
Microscopic kinetic + potential energy stored in molecules, excluding flow work. Used in closed-system (piston-cylinder) energy balances. At saturation: u_f = h_f − P·v_f.
SI: kJ/kg  |  Imperial: BTU/lb
Specific Volume
v
v = V/m = 1/ρ
Volume per unit mass — reciprocal of density. Liquid water ≈ 0.001 m³/kg. Steam expands dramatically at low pressure: v_g ≈ 206 m³/kg at 0.01°C. Critical for pipe and nozzle sizing.
SI: m³/kg  |  Imperial: ft³/lb
Density
ρ
ρ = 1/v  [kg/m³]
Mass per unit volume. Saturated liquid ≈ 958 kg/m³ at 100°C. Saturated steam at 1 bar ≈ 0.598 kg/m³ — approximately 1600× less dense. Used for flow velocity and pressure drop calculations.
SI: kg/m³  |  Imperial: lb/ft³
Steam Quality
x
x = mvapor / mtotal
Vapor mass fraction in two-phase mixture. x = 0: saturated liquid; x = 1: dry saturated vapor. For mixture: h = h_f + x·h_fg. Turbine exhaust must have x ≥ 0.88 to prevent blade erosion.
Dimensionless · Range: 0.0 – 1.0
Latent Heat
h_fg
h_fg = h_g − h_f
Energy required to convert saturated liquid → saturated vapor at constant T and P. At 100°C: 2257 kJ/kg. Decreases with rising pressure, reaching zero at the critical point (374.14°C, 220.9 bar).
SI: kJ/kg  |  Imperial: BTU/lb
Degree of Superheat
ΔT_sh
ΔT_sh = T − T_sat(P)
How far above saturation temperature superheated steam is. Higher superheat → more specific work in turbines. Power plants use 50–200°C superheat. ΔT_sh = 0 marks the saturation boundary.
SI: °C  |  Imperial: °F
Critical Point
Tc, Pc
T_c = 374.14°C · P_c = 220.9 bar
Above this state, liquid and vapor phases become indistinguishable — h_fg = 0 and ρ_f = ρ_g = 317 kg/m³. Supercritical steam is used in advanced power plants for efficiencies above 45%.
IAPWS-IF97 reference values
Saturation Pressure
P_sat
Wagner equation — ±0.003 bar
Equilibrium pressure at which phase change occurs at a given T. At 100°C = 1.01325 bar; at 200°C = 15.54 bar; at 300°C = 85.88 bar. Used for flash calculation and steam trap sizing.
SI: bar / MPa  |  Imperial: psia
🔬Formulation Accuracy — IAPWS-IF97
Calculation Method & Error Bounds
Saturation Pressure:  Wagner equation (IAPWS-IF97 §8.1)  →  ±0.003 bar
T_sat from P:         Newton iteration on Wagner           →  ±0.01°C
Sat. Properties:      Interpolated reference tables (34 pts, 0.01–374°C)
                      h_f, h_fg, h_g  →  ±0.3 kJ/kg
                      s_f, s_fg, s_g  →  ±0.002 kJ/(kg·K)
                      v_f, v_g        →  ±0.1%
Compressed Liquid:    h = h_f(T) + v_f·ΔP  (IAPWS approx.)   →  ±0.5%
Superheated Steam:    Cp polynomial + sat. boundary           →  ±0.5%

For critical engineering decisions, always verify against certified IAPWS-IF97 tables.