One mole of an ideal diatomic gas undergoes a process as shown in the figure. The molar specific heat of the gas in the process is:

The process shown in the figure indicates an isochoric process where the volume of the gas is directly proportional to the inverse of the temperature. For an ideal gas undergoing such a process, the relation between the pressure, volume, and temperature is: \[ V \propto \frac{1}{T} \] This implies that the process follows a path where the slope of \( V \) versus \( \frac{1}{T} \) is constant. For an ideal diatomic gas, the molar specific heat \( C \) is related to the slope of the curve in the diagram. From the relationship for an ideal gas: \[ C = C_V + R \] where \( C_V \) is the molar specific heat at constant volume for a diatomic gas, which is \( \frac{5R}{2} \). Since the process shown is a specific heat process that involves both heat exchange and work, the total molar specific heat will be \( \frac{3R}{2} \).
Thus, the molar specific heat of the gas in the process is \( \boxed{\frac{3R}{2}} \).
The stopping potential (\(V_0\)) versus frequency (\(\nu\)) of a graph for the photoelectric effect in a metal is given. From the graph, the Planck's constant (\(h\)) is:

In the diagram shown below, both the strings AB and CD are made of the same material and have the same cross-section. The pulleys are light and frictionless. If the speed of the wave in string AB is \( v_1 \) and in CD is \( v_2 \), then the ratio \( \frac{v_1}{v_2} \) is:
