Advance Thermodynamics

  • Determine the value of f/P for nitrogen at 250K and (1) 200 bars and (2) 200 bars by the following methods: a> the gas is an ideal gas b> the gas follows the equation of state, Pv=RT+bP, where b=39.5-1X10(exp4)/T-1.084X10(exp6)/T(exp2), jT is in Kelvins and b is in cm(exp3)/gmol c> the two parameters generalized fugacity coefficient chart d> the Lee-Kessler three parameter data


  • You obviously made a mistake in copying the question; parts (1) and (2) both ask for the fugacity coefficient (f/P) at 200 bars. To answer parts c) and d), one needs information you haven't given us, namely the "generalized fugacity coefficient chart" referred to in part c), and the Lee-Kessler equation of state parameters needed for part d). Part a) is trivial. By definition for an ideal gas, the fugacity is equal to the partial pressure. f/P = 1 Part b) is asking for the fugacity coefficient for a nonideal gas that obeys the van der Waals equation of state when the size parameter (b parameter) dominates, and the intermolecular forces are negligible (a parameter = 0). Let g = f/P (g is the fugacity coefficient, usually written as a lower case Greek gamma). For any real gas, (d ln(g)/dp)_T = v/RT - 1/p, [look this up in your textbook] where (d ln(g)/dp)_T means the partial derivative of the ln of the fugacity coefficient with respect to pressure at constant temperature. Integrating this, we get: ln(g) - ln(g0) = Integral from p=0 to P { (v/RT -- 1/p) dp}, where g0 is the fugacity coefficient at P=0 bars. But the fugacity is defined to be equal to the pressure as P-> 0, so ln(g0) =ln(P/P) = 0. We are given that v = RT/p + b. Substituting this into the integrand above, you'll find that the RT/p terms cancel out, and we are left with: ln(g) = Integral from p = 0 to P {b/RT dp} = b/RT*(P-0) = bP/RT exponentiating both sides yields the desired result: g = f/P = exp(bP/RT) or, noting that from the equation of state that P/RT = 1/(V-b) g = f/P = exp(b/(V-b)) You need to plug in the particular values of b, T, and P (or V) corresponding to the conditions asked about in the problem. Note that b is a function of T.