Clasius-Clapeyron equation for water vapor

Input(s)

LvL_{v}: Heat of Vaporization of one mole of Liquid (J/mol)(\mathrm{J} / \mathrm{mol})

T1\mathrm{T}_{1}: Absolute Temperature of Condition 1(F)1\left({ }^{\circ} \mathrm{F}\right)

T2\mathrm{T}_{2}: Absolute Temperature of Condition 2(F)2\left({ }^{\circ} \mathrm{F}\right)

RR: Gas Constant for Water Vapor (psi/molFs2)\left(\mathrm{psi} / \mathrm{mol}^{\circ} \mathrm{F} \mathrm{s}{ }^{2}\right)

Output(s)

pv1p_{v 1}: Vapor Pressure at the Temperature T1(psi)\mathrm{T}_{1}(\mathrm{psi})

pv2p_{v 2}: Vapor Pressure at the Temperature T2(psi)\mathrm{T}_{2}(\mathrm{psi})

Formula(s)

ln(pv1pv2)=LvR(1 T11 T2)\ln \left(\frac{\mathrm{p}_{\mathrm{v} 1}}{\mathrm{p}_{\mathrm{v} 2}}\right)=\frac{\mathrm{L}_{\mathrm{v}}}{\mathrm{R}}\left(\frac{1}{\mathrm{~T}_{1}}-\frac{1}{\mathrm{~T}_{2}}\right)

Reference(s)

McCain Jr, W. D. (1990). Properties of Petroleum Fluids. PennWell Corporation. Page: 54.


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