The heat capacity of a substance tells us how much heat is required to raise a certain amount of the substance by one degree. For a gas we can define a molar heat capacity C - the heat required to increase the temperature of 1 mole of the gas by 1 K.
Q = nCΔT
The value of the heat capacity depends on whether the heat is added at constant volume, constant pressure, etc.
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 we showed that | ΔEint | = |
|
nR ΔT |
Comparing our two equations
Q = nCV ΔT and Q = |
|
nR ΔT |
we see that, for a monatomic ideal gas:
CV | = |
|
R |
For diatomic and polyatomic ideal gases we get:
diatomic: CV | = |
|
R |
polyatomic: CV = 3R
This is from the extra 2 or 3 contributions to the internal energy from rotations.
Because Q = ΔEint when the volume is constant, the change in internal energy can always be written:
ΔEint = n CV ΔT