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Pressure, Temperature and Phase Changes

The advantage of carrying out thermal processes under vacuum pressures can be seen if the liquid-gas boundary is considered. [Pg.177]

The Clapeyron equation states the relationship between a phase change for a pure material and changes in pressure and temperature. For vaporisation  [Pg.177]

Using the Clapeyron equation, calculate the enthalpy of vaporisation (evaporation) of water from the following data  [Pg.177]

As vvap is much larger than vh in Equation (6.1) (vvap - v7) can be replaced by vvapm, where the subscript m refers to a unit amount (mol-1, kmol-1), or, better, vm(vap). If it is assumed that the vapour behaves ideally (vm = RT/p), then the Clausius-Clapeyron equation is obtained  [Pg.178]

If it is further assumed that A//vapm does not depend on temperature then Equation (6.2) integrates to  [Pg.178]


See other pages where Pressure, Temperature and Phase Changes is mentioned: [Pg.177]   


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