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Question

In heat capacity how could we get the specific heat capacity relation at constant volume please explain me in a detailed way

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Solution

Heat Capacity at Constant Volume

Q = nCVΔT

For an ideal gas, applying the First Law of Thermodynamics tells us that heat is also equal to:

Q = ΔEint + W, although W = 0 at constant volume.

For a monatomic ideal gas ΔEint = (3/2)nRΔT

Comparing our two equations

Q = nCVΔT and Q = (3/2)nRΔT

we see that, for a monatomic ideal gas:

CV = (3/2)R

For diatomic and polyatomic ideal gases we get:

diatomic: CV = (5/2)R

polyatomic: CV = 3R

This is from the extra 2 or 3 contributions to the internal energy from rotations.


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