To solve this problem, we need to find the ratio of the specific heat capacities at constant volume \( C_V \) for two ideal diatomic gases \( A \) and \( B \).
First, let's understand the properties of these gases:
The specific heat capacity at constant volume \( C_V \) for a diatomic gas can be calculated using the degrees of freedom \( f \). The formula is given by:
C_V = \frac{f}{2} R
where \( R \) is the ideal gas constant.
For a diatomic gas without vibrational modes, the degrees of freedom \( f \) are 5 (3 translational and 2 rotational).
Therefore, for gas \( A \):
C^A_V = \frac{5}{2} R
For a diatomic gas with an additional vibrational mode, there is 1 additional degree of freedom.
Thus, for gas \( B \), the degrees of freedom \( f \) are 7 (5 from the previous modes + 2 from vibrational mode).
Therefore, for gas \( B \):
C^B_V = \frac{7}{2} R
Now, calculate the ratio \( \frac{C^A_V}{C^B_V} \):
\frac{C^A_V}{C^B_V} = \frac{\frac{5}{2} R}{\frac{7}{2} R} = \frac{5}{7}
Thus, the ratio of specific heats \( \frac{C^A_V}{C^B_V} \) is \frac{5}{7}.
Therefore, the correct answer is: 5:07