Specific heat of a monotomic gas

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Apashanka
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Homework Statement
The problem is attached below
Relevant Equations
The problem is attached below
IMG_20200304_112027.jpg

Given this problem I have calculated the partition function as $$z=1+e^{-\beta E_1}$$
And calculated the average internal energy as $$<U>=\frac{E_1 e^{-\beta E_1}}{1+e^{-\beta E_1}}$$
And thereafter taking the partial derivative of <E> with respect to temp. T the specific heat obtained is option (b)...
Am I correct??
 
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on Phys.org
Apashanka said:
Homework Statement:: The problem is attached below
Relevant Equations:: The problem is attached below

View attachment 258085
Given this problem I have calculated the partition function as $$z=1+e^{-\beta E_1}$$
And calculated the average internal energy as $$<U>=\frac{E_1 e^{-\beta E_1}}{1+e^{-\beta E_1}}$$
And thereafter taking the partial derivative of <E> with respect to temp. T the specific heat obtained is option (b)...
Am I correct??
It looks good.
See @mjc123's post.
 
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mjc123 said:
That deals with the electronic energy of the atoms. What other energy do they have?
Then what should be the answer
 
mjc123 said:
Working that out is your job.
Actually I need some help regarding this...one part I have got but how to get the next part..,can you suggest something??
 
When you have independent degrees of freedom, the energy is a sum of terms for the different degrees of freedom. For example, you usually have for a diatomic gas molecule
$$
E_\mathrm{total} = E_\mathrm{translation} + E_\mathrm{rotation}.
$$
The separability applies also to the averages,
$$
\langle E_\mathrm{total} \rangle = \langle E_\mathrm{translation}\rangle + \langle E_\mathrm{rotation} \rangle.
$$