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 \( \frac{7}{5} \).
Match List - I with List - II.
Consider the following statements:
(A) Availability is generally conserved.
(B) Availability can neither be negative nor positive.
(C) Availability is the maximum theoretical work obtainable.
(D) Availability can be destroyed in irreversibility's.
A bead of mass \( m \) slides without friction on the wall of a vertical circular hoop of radius \( R \) as shown in figure. The bead moves under the combined action of gravity and a massless spring \( k \) attached to the bottom of the hoop. The equilibrium length of the spring is \( R \). If the bead is released from the top of the hoop with (negligible) zero initial speed, the velocity of the bead, when the length of spring becomes \( R \), would be (spring constant is \( k \), \( g \) is acceleration due to gravity):
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: