The vibrational contribution to the heat capacity is given by e-eV /2T Cm = R -e-eV/T Show that in the high temperature limit (when 0' « T) T. = R. (HINT: for small values of x, e* = 1+ x). Explain each step in your derivation.

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the vibrational contribution to the heat capacity is given by the photo below. show that in the high temperature limit C=R.(For small values of x, e^x=1+x)

The image contains a physics problem regarding the vibrational contribution to heat capacity. The problem is as follows:

**The vibrational contribution to the heat capacity is given by:**

\[ C_{V_m} = R \left( \frac{\theta_v}{T} \right)^2 \frac{e^{\theta_v/T}}{(e^{\theta_v/T} - 1)^2} \]

**Show that in the high temperature limit (when \(\theta_v \ll T\)):**

\[ C_{V_m} = R \]

**(HINT: For small values of \(x\), \(e^x = 1 + x\). Explain each step in your derivation.)**

Below this, there is a partial derivation that uses the hint provided:

\[ e^{x} \approx 1 + x \]
\[ C_{V_m} = R \left( \frac{\theta_v}{T} \right)^2 \]

The task is to derive the expression for \( C_{V_m} \) in the high temperature limit, using the approximation for small \(x\).
Transcribed Image Text:The image contains a physics problem regarding the vibrational contribution to heat capacity. The problem is as follows: **The vibrational contribution to the heat capacity is given by:** \[ C_{V_m} = R \left( \frac{\theta_v}{T} \right)^2 \frac{e^{\theta_v/T}}{(e^{\theta_v/T} - 1)^2} \] **Show that in the high temperature limit (when \(\theta_v \ll T\)):** \[ C_{V_m} = R \] **(HINT: For small values of \(x\), \(e^x = 1 + x\). Explain each step in your derivation.)** Below this, there is a partial derivation that uses the hint provided: \[ e^{x} \approx 1 + x \] \[ C_{V_m} = R \left( \frac{\theta_v}{T} \right)^2 \] The task is to derive the expression for \( C_{V_m} \) in the high temperature limit, using the approximation for small \(x\).
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