An ideal gas initially at 0°C temperature, is compressed suddenly to one fourth of its volume. If the ratio of specific heat at constant pressure to that at constant volume is \( \frac{3}{2} \), the change in temperature due to the thermodynamics process is K.
Initial temperature, $T_1 = 0^\circ C = 273 \text{ K}$
Final volume, $V_2 = V_1 / 4$
Ratio of specific heats, $\gamma = C_p / C_v = 3/2$
For adiabatic compression: $T_2 V_2^{\gamma - 1} = T_1 V_1^{\gamma - 1}$
$\displaystyle T_2 / T_1 = (V_1 / V_2)^{\gamma - 1}$
$\displaystyle T_2 / 273 = (V_1 / (V_1/4))^{3/2 - 1}$
$\displaystyle T_2 / 273 = 4^{1/2} = 2$
$T_2 = 2 \times 273 = 546 \text{ K}$
$\Delta T = T_2 - T_1 = 546 - 273 = 273 \text{ K}$
$\boxed{273\ \text{K}}$