Thus we get
$\frac{F}{A}=\mu \frac{u}{y}$
or
$F=\frac{A \mu u}{y} \propto u$
Thus we get
$\frac{F_{1}}{u_{1}}=\frac{F_{2}}{u_{2}}$
Substituting the values we get
$\frac{800}{1.5}=\frac{2400}{u_{2}}$
Thus we get $u_{2}=4.5 \mathrm{cm} / \mathrm{s}$


$(A)$ $\beta=0$ when $a= g / \sqrt{2}$
$(B)$ $\beta>0$ when $a= g / \sqrt{2}$
$(C)$ $\beta=\frac{\sqrt{2}-1}{\sqrt{2}}$ when $a= g / 2$
$(D)$ $\beta=\frac{1}{\sqrt{2}}$ when $a= g / 2$
[Given: $\pi=22 / 7, g=10 ms ^{-2}$, density of water $=1 \times 10^3 kg m ^{-3}$, viscosity of water $=1 \times 10^{-3} Pa$-s.]
$(A)$ The work done in pushing the ball to the depth $d$ is $0.077 J$.
$(B)$ If we neglect the viscous force in water, then the speed $v=7 m / s$.
$(C)$ If we neglect the viscous force in water, then the height $H=1.4 m$.
$(D)$ The ratio of the magnitudes of the net force excluding the viscous force to the maximum viscous force in water is $500 / 9$.