Use a Maxwell relation from the previous problem 1 and the

Chapter 5, Problem 13P

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QUESTION:

Use a Maxwell relation from the previous problem 1 and the third law of thermodynamics to prove that the thermal expansion coefficient \(\beta \) (defined in Problem 2) must be zero at T = 0.

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QUESTION:

Use a Maxwell relation from the previous problem 1 and the third law of thermodynamics to prove that the thermal expansion coefficient \(\beta \) (defined in Problem 2) must be zero at T = 0.

ANSWER:

Step 1 of 2

The thermal expansion coefficient \(\beta \) is defined as the fractional change in the volume per unit temperature change.

\(\beta  = \dfrac{{\dfrac{{\Delta V}}{V}}}{{\Delta V}}\)

\(\beta  = \dfrac{1}{V}{\left( {\dfrac{{\partial V}}{{\partial T}}} \right)_P}\)

Here, V is the volume, T is the temperature, and P is the system's pressure.

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