



To determine the temperature dependence of the total specific heat \( C_v \) for a two-dimensional metallic solid at low temperatures, we need to understand how specific heat behaves in such systems.
At low temperatures, the specific heat of a metal is typically described by the expression:
\[ C_v = \gamma T + \beta T^2 \]
where:
For a two-dimensional metallic solid, at low temperatures, the electronic contribution dominates according to the linear term \( \gamma T \). However, this specific context implies that both electronic and phononic contributions are considered.
Given the options available, the correct graph should represent this behavior where specific heat \( C_v \) initially increases linearly with temperature and shows curvature due to the phononic \( T^2 \) term. The correct graph among the provided options should reflect an initial linear rise followed by a slight curve, indicating the increasing influence of phononic contributions as the temperature increases.
Examining the options, the correct graph for the temperature dependence of specific heat at low temperatures in a two-dimensional metallic solid is:

This graph shows a clear linear rise initially (due to the \( \gamma T \) term) with a subsequent rise indicative of a \( T^2 \) contribution (showing curvature), thus accurately representing the expected behavior of \( C_v \) at low temperatures.
One mole of an ideal gas expands isothermally and reversibly from $10 \mathrm{dm}^{3}$ to $20 \mathrm{dm}^{3}$ at $300 \mathrm{~K} . \Delta \mathrm{U}$, q and work done in the process respectively are : Given : $\mathrm{R}=8.3 \mathrm{JK}^{-1}$ and $\mathrm{mol}^{-1}$ In $10=2.3$ $\log 2=0.30$ $\log 3=0.48$
