$ \Delta \ell=\frac{\mathrm{F} \ell}{\mathrm{AY}} $
$ \mathrm{V}=\mathrm{A} \ell \Rightarrow \ell=\frac{\mathrm{V}}{\mathrm{A}} $
$ \Delta \ell=\frac{\mathrm{FV}}{\mathrm{A}^2 \mathrm{Y}}$
$Y$ & $V$ is same for both the wires
$ \Delta \ell \propto \frac{\mathrm{F}}{\mathrm{A}^2} $
$ \frac{\Delta \ell_1}{\Delta \ell_2}=\frac{\mathrm{F}_1}{\mathrm{~A}_1^2} \times \frac{\mathrm{A}_2^2}{\mathrm{~F}_2} $
$ \Delta \ell_1=\Delta \ell_2 $
$ \mathrm{~F}_1 \mathrm{~A}_2^2=\mathrm{F}_2 \mathrm{~A}_1^2 $
$ \frac{\mathrm{F}_1}{\mathrm{~F}_2}=\frac{\mathrm{A}_1^2}{\mathrm{~A}_2^2}=\left(\frac{4}{1}\right)^2=16$
| Column $-I$ | Column $-II$ |
|
$(a)$ Stress is proportional to strain. |
$(i)$ Elastic limit |
| $(b)$ When the load of the wire is removed, the body does regain its original dimension. | $(ii)$ Limit of pro-portionality |
| $(iii)$ Plastic deformation |
