The process described is a reversible change with no heat exchange ($\Delta Q = 0$). This signifies an adiabatic process for the ideal gas.
The relationship between temperature ($T$) and volume ($V$) during an adiabatic process for an ideal gas is:
$ T V^{\gamma-1} = \text{constant} $
Here, $\gamma$ represents the adiabatic index, which depends on the gas type.
Let the initial state be (1) and the final state be (2). The formula can be written as:
$ T_1 V_1^{\gamma-1} = T_2 V_2^{\gamma-1} $
The problem states:
Substitute the given values into the adiabatic equation:
$ T_1 V_1^{\gamma-1} = \left(\frac{1}{4} T_1\right) (8V_1)^{\gamma-1} $
Divide both sides by $T_1$:
$ V_1^{\gamma-1} = \frac{1}{4} (8V_1)^{\gamma-1} $
Rearrange to isolate the volume terms:
$ 4 = \frac{(8V_1)^{\gamma-1}}{V_1^{\gamma-1}} $
Simplify using exponent rules:
$ 4 = \left(\frac{8V_1}{V_1}\right)^{\gamma-1} $
$ 4 = 8^{\gamma-1} $
Express both sides with the base 2:
$ 2^2 = (2^3)^{\gamma-1} $
$ 2^2 = 2^{3(\gamma-1)} $
Equate the exponents:
$ 2 = 3(\gamma-1) $
Solve for $\gamma$:
$ \gamma-1 = \frac{2}{3} $
$ \gamma = 1 + \frac{2}{3} = \frac{5}{3} $
The calculated adiabatic index is $\gamma = 5/3$. This value is characteristic of monatomic ideal gases.
From the given options, He (Helium) is a monatomic gas.
Rods x and y of equal dimensions but of different materials are joined as shown in figure. Temperatures of end points $A$ and $F$ are maintained at $100^\circ\text{C}$ and $40^\circ\text{C}$ respectively. Given the thermal conductivity of rod x is three times of that of rod y, the temperature at junction points $B$ and $E$ are (close to):

10 mole of an ideal gas is undergoing the process shown in the figure. The heat involved in the process from $P_1$ to $P_2$ is $\alpha \text{ Joule}$ ($P_1 = 21.7 \text{ Pa}$ and $P_2 = 30 \text{ Pa}, C_v = 21 \text{ J/K.mol}, R = 8.3 \text{ J/mol.K}$). The value of $\alpha$ is _______.

Rods x and y of equal dimensions but of different materials are joined as shown in figure. Temperatures of end points $A$ and $F$ are maintained at $100^\circ\text{C}$ and $40^\circ\text{C}$ respectively. Given the thermal conductivity of rod x is three times of that of rod y, the temperature at junction points $B$ and $E$ are (close to):
