So, $Y=\frac{F L}{A \ell_{a}}=\frac{V \rho g L}{A \ell_{a}}$ $...(1)$
When the load is immersed in the liquid, then
$Y=\frac{F^{\prime} L}{A \ell_{w}}=\frac{(V \rho g-V \times 1 \times g) L}{A \ell_{w}}$ $...(2)$
(... Now net weight $=$ weight - upthrust) From eqs. $( 1)$ and $(2),$ we get
$\frac{\rho}{\ell_{\mathrm{a}}}=\frac{(\rho-1)}{\ell_{\mathrm{w}}}$ or $\rho=\frac{\ell_{\mathrm{a}}}{\left(\ell_{\mathrm{a}}-\ell_{\mathrm{w}}\right)}$
$(A)$ $\frac{\left|\overrightarrow{ V }_{ P }\right|}{\left|\overrightarrow{ V }_{ Q }\right|}=\frac{\eta_1}{\eta_2}$ $(B)$ $\frac{\left|\overrightarrow{ V }_{ P }\right|}{\left|\overrightarrow{ V }_{ Q }\right|}=\frac{\eta_2}{\eta_1}$
$(C)$ $\overrightarrow{ V }_{ P } \cdot \overrightarrow{ V }_{ Q } > 0$ $(D)$ $\overrightarrow{ V }_{ P } \cdot \overrightarrow{ V }_{ Q } < 0$

