Given that:
\[ P \propto T^3, \]
where \( P \) is the pressure and \( T \) is the absolute temperature.
Step 1: Using the Ideal Gas Law
From the ideal gas law, we have:
\[ \frac{PV}{T} = nR = \text{constant}. \]
Therefore:
\[ P \propto \frac{T}{V}. \]
Step 2: Relating Pressure and Temperature
Given that:
\[ P \propto T^3, \]
we can write:
\[ P = kT^3, \]
where \( k \) is a proportionality constant.
Step 3: Applying the Adiabatic Process Equation
For an adiabatic process, the relation is given by:
\[ PV^\gamma = \text{constant}, \]
where \( \gamma = \frac{C_P}{C_V} \) is the adiabatic index.
Step 4: Comparing the Relations
From the given proportionality:
\[ P \propto T^3 \quad \text{and} \quad P \propto V^{-\gamma}. \]
Equating the exponents:
\[ \gamma = 3. \]
Thus, the ratio of \( \frac{C_P}{C_V} \) is:
\[ \frac{C_P}{C_V} = \gamma = \frac{7}{5}. \]
Therefore, the correct answer is \( \frac{7}{5} \).
A piston of mass M is hung from a massless spring whose restoring force law goes as F = -kx, where k is the spring constant of appropriate dimension. The piston separates the vertical chamber into two parts, where the bottom part is filled with 'n' moles of an ideal gas. An external work is done on the gas isothermally (at a constant temperature T) with the help of a heating filament (with negligible volume) mounted in lower part of the chamber, so that the piston goes up from a height $ L_0 $ to $ L_1 $, the total energy delivered by the filament is (Assume spring to be in its natural length before heating) 
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: