The principle of corresponding states has far greater applicability in thermodynamics than was indicated in the discussion

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The principle of corresponding states has far greater applicability in thermodynamics than was indicated in the discussion of Sec. 6.6. For example, it is possible to construct corresponding-states relations for both the vapor and liquid densities along the coexistence curve, and for the vapor pressure and enthalpy change on vaporization (ΔvapH) as a function of reduced temperature. This will be demonstrated here using the van der Waals equation as a model equation of state.

a. Show that at vapor-liquid equilibrium 

Syt  (P), V T dV = 0

b. Show that the solution to this equation for the van der Waals fluid is

In 3VL 3V,V + (3VV  1)- + (3V  1)- - 9 VL 47. V. (1 - 1) = 4T,VL + where V = V/V and V = VV/V. = 0

c. Construct a corresponding-states curve for the reduced vapor pressure Prvap of the van der Waals fluid as a function of its reduced temperature.

d. Describe how a corresponding-states curve for the enthalpy change on vaporization as a function of the reduced temperature can be obtained for the van der Waals fluid.

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