Heat required to increase the temperature

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Homework Statement


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At high temperatures the nitrogen molecule behaves like a one-dimensional harmonic oscillator. In this situation, estimate how much heat must be added to the system in order to increase the temperature of 1 mole of nitrogen gas by 10 degrees Celsius (for constant volume and constant pressure respectively). Take into account all degrees of freedom: translational, rotational and vibrational.

Homework Equations


Average energy per degree of freedom: ##kT/2##

The Attempt at a Solution


A one-dimensional harmonic oscillator has two degrees of freedom, therefore according to the equipartition theorem the average energy of a nitrogen molecule must be ##kT##. One mole of nitrogen has ##N_A## molecules and so the total internal energy of the gas is ##U=N_A k T##. Therefore if the process is isochoric the amount of heat we need to add to the system in order to increase the temperature by 10 degrees is
$$dQ=N_A k dT=N_A k \cdot 10\text{K} \approx 19.8 \text{cal}$$
However the correct answer is ##70 \text{cal}## and I don't understand why.
Also, I have no idea how to find the heat for the case of an isobaric process since this is not an ideal gas (the answer for constant pressure case is ##90 \text{cal}##).
 
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Orodruin said:
First of all, a nitrogen molecule is not a one dimensional harmonic oscillator. You are missing a lot of degrees of freedom by this assumption.
But that's how the question was formulated. It's not my assumption.
 
Orodruin said:
It is an oscillator that in addition can translate and rotate. Only the vibrational spectrum is described by an actual harmonic oscillator.
Oh I see. So the translational motion contributes 3 degrees of freedom whereas the rotational contributes 2. Therefore there are 7 degrees of freedom and the heat required is approximately 70cal, as expected.
But what about the constant pressure case? How can I approach this problem?
Thank you.
Edit: nevermind. I think the reason why it's ##90 \text{cal}## for constant pressure case is because ##C_p-C_v=2 \frac{\text{cal}}{\text{mol}\,\text{K}}## for nitrogen (apparently it does behave approximately as an ideal gas). So it requires additional $$\left(2 \,\frac{\text{cal}}{\text{mol}\,\text{K}} \right )\cdot (10 \,\text{K})=20 \,\frac{\text{cal}}{\text{mol}}$$ heat for constant pressure case.
 
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