A spherical solid ball of volume $V$ is made of a material of density $\rho_1$ . It is falling through a liquid of density $\rho_2 (\rho_2 < \rho_1 )$. Assume that the liquid applies a viscous force on the ball that is proportional to the square of its speed $v$, i.e., $F_{viscous}= -kv^2 (k >0 )$,The terminal speed of the ball is
$\frac{{Vg\left( {{\rho _1} - {\rho _2}} \right)}}{k}$
$\sqrt {\;\frac{{Vg\left( {{\rho _1} - {\rho _2}} \right)}}{k}} $
$\;\frac{{Vg{\rho _1}}}{k}$
$\;\sqrt {\frac{{Vg{\rho _1}}}{k}} $
A particle released from rest is falling through a thick fluid under gravity. The fluid exerts a resistive force on the particle proportional to the square of its speed. Which one of the following graphs best depicts the variation of its speed $v$ with time $t$ ?
Which of the following is not the property of an ideal fluid?
Why not rain drops do not posses greater velocity than some velocity ? Explain.
The terminal velocity of a copper ball of radius $5\,mm$ falling through a tank of oil at room temperature is $10\,cm\,s ^{-1}$. If the viscosity of oil at room temperature is $0.9\,kg\,m ^{-1} s ^{-1}$, the viscous drag force is :
An air bubble of $1\, cm$ radius is rising at a steady rate of $2.00\, mm/sec$ through a liquid of density $1.5\, gm$ per $cm^3$. Neglect density of air. If $g$ is $1000\, cm/sec^2$, then the coefficient of viscosity of the liquid is