Total mass can be assumed to be concentrated at center of mass at distance $\frac{L}{2}$ from top
$\frac{M}{L}=\lambda$
$M=\lambda L$
$\Delta x=\frac{F L / 2}{A Y}=\frac{1}{2} \times \frac{\lambda L^2 g}{A Y}$
| Column $-I$ | Column $-II$ |
| $(a)$ When temperature raised Young’s modulus of body | $(i)$ Zero |
| $(b)$ Young’s modulus for air | $(ii)$ Infinite |
| $(iii)$ Decreases | |
| $(iv)$Increases |