The problem asks us to determine the molar specific heat at constant volume for a diatomic gas with one additional vibrational mode, using the law of equipartition of energy.
According to the law of equipartition of energy, each degree of freedom contributes \(\frac{1}{2} R\) (where \(R\) is the universal gas constant) to the molar specific heat.
For a diatomic gas, consider the following degrees of freedom:
In total, the degrees of freedom are 3 (translational) + 2 (rotational) + 1 (vibrational) = 6.
Therefore, the molar specific heat at constant volume \(C_v\) is given by:
\(C_v = \frac{1}{2}R \times \text{(Number of degrees of freedom)}\)
Substituting the degrees of freedom:
\(C_v = \frac{1}{2}R \times 6 = \frac{6}{2}R = 3R\)
However, this total includes one vibrational mode's energy, which involves both kinetic and potential energy contributions. Each vibrational mode effectively contributes \(R\) (i.e., \(\frac{1}{2}R\) from kinetic + \(\frac{1}{2}R\) from potential), thus we need to account for \(2R\) for the additional vibrational mode, not just \(1R\).
As a diatomic molecule in general without vibration contributes \(\frac{5}{2}R\), adding the vibration contribution, the correct molar specific heat becomes:
\(C_v = \frac{5}{2}R + R = \frac{7}{2}R\)
Thus, the molar specific heat of a diatomic gas at constant volume, where the molecule has one additional vibrational mode, is \(\frac{7}{2}R\). Therefore, the correct answer is:
Correct Answer: \(\frac{7}{2} R\)