What Is the Equation of State Given Compressibility and Expansivity Relations?

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SUMMARY

The discussion focuses on deriving the equation of state using compressibility and expansivity relations defined by k = aT^(3) / P^2 and B = bT^(2) / P. The solution reveals that the equation of state is V = V0exp(aT^(3)/P). Participants explore integration techniques and the implications of partial derivatives in the context of thermodynamic relationships, specifically addressing the exact differential of lnV and its implications for the relationship between temperature and pressure derivatives.

PREREQUISITES
  • Understanding of thermodynamic principles, specifically compressibility and expansivity.
  • Familiarity with partial derivatives and their applications in thermodynamics.
  • Knowledge of integrating differential equations in the context of state equations.
  • Basic grasp of exponential functions and their role in physical equations.
NEXT STEPS
  • Study the derivation of the ideal gas law and its relation to real gas behavior.
  • Learn about the implications of exact differentials in thermodynamics.
  • Explore advanced integration techniques for solving differential equations in physics.
  • Investigate the relationship between compressibility, expansivity, and phase transitions in materials.
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Students and professionals in thermodynamics, particularly those focused on physical chemistry, chemical engineering, and anyone involved in deriving equations of state for gases and liquids.

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Homework Statement


Find the equation of state given that k = aT^(3) / P^2 (compressibility) and B = bT^(2) / P (expansivity) and the ratio, a/b?

Homework Equations


B = 1/v (DV /DT)Pressure constant ; k = -1/v (DV /DP)Temperature constant D= Partial derivative
dV = BVdT -kVdP (1)
ANSWER is V = V0exp(aT^(3)/P)

The Attempt at a Solution


a. Integrate (1) and obtain v = voexp (bT^(3)/3P) + 2aT^(3)/P^3) WRONG
b. Hint by Professor: rewrite as: (Let "D" = partial derivative): D/DP (lnV) = 1/V (DV/DP) then D/DP (lnV) + aT^(3)/P = 0. Write as D/DP(lnv + g(P,T)) = 0 where g is a function only of V. ==> lnV + g(P,T) = f(V) where V is an arbitrary function.

I don't understand "b" but following attempt "a" gave me the proper result for a very similar problem?
 
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Your starting equations are:

$$\frac{\partial \ln V}{\partial P}=-a\frac{T^3}{P^2}$$
$$\frac{\partial \ln V}{\partial T}=b\frac{T^2}{P}$$
Together with $$d\ln V=\frac{\partial \ln V}{\partial P}dP+\frac{\partial \ln V}{\partial T}dT$$
The last equation implies that d lnV is an exact differential. What does that imply about the relationship between ##\frac{\partial}{\partial T}\left(\frac{\partial \ln V}{\partial P}\right)## and ##\frac{\partial}{\partial P}\left(\frac{\partial \ln V}{\partial T}\right)##?

Chet
 

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