MHT CET · Physics · Mechanical Properties of Fluids
The velocity of a small ball of mass ' \(M\) ' and density ' \(\mathrm{d}_1\) ' when dropped in a container filled with glycerin becomes constant after some time. If the density of glycerin is ' \(\mathrm{d}_2\) ', the viscous force acting on the ball is ( \(\mathrm{g}\) = acceleration due to gravity)
- A \(\operatorname{Mg} \frac{\mathrm{d}_1}{\mathrm{~d}_2}\)
- B \(\operatorname{Mgd}_1 \mathrm{~d}_2\)
- C \(\operatorname{Mg}\left(\mathrm{d}_1-\mathrm{d}_2\right)\)
- D \(\operatorname{Mg}\left(1-\frac{\mathrm{d}_2}{\mathrm{~d}_1}\right)\)
Answer & Solution
Correct Answer
(D) \(\operatorname{Mg}\left(1-\frac{\mathrm{d}_2}{\mathrm{~d}_1}\right)\)
Step-by-step Solution
Detailed explanation
Since the velocity is constant, the net force acting on the ball is zero.
\(
\begin{aligned}
& \mathrm{F}_{\mathrm{V}}+\mathrm{F}_{\mathrm{B}}=\mathrm{Mg} \\
& \mathrm{F}_{\mathrm{V}}+\mathrm{Vd}_2 \mathrm{~g}=\mathrm{Mg}
\end{aligned}
\)
\(
\mathrm{F}_{\mathrm{v}}+\frac{\mathrm{M}}{\mathrm{d}_1} \mathrm{~d}_2 \mathrm{~g}=\mathrm{Mg}
\)
\(
\mathrm{F}_{\mathrm{V}}=\mathrm{Mg}\left(1-\frac{\mathrm{d}_2}{\mathrm{~d}_1}\right)
\)
\(
\begin{aligned}
& \mathrm{F}_{\mathrm{V}}+\mathrm{F}_{\mathrm{B}}=\mathrm{Mg} \\
& \mathrm{F}_{\mathrm{V}}+\mathrm{Vd}_2 \mathrm{~g}=\mathrm{Mg}
\end{aligned}
\)
\(
\mathrm{F}_{\mathrm{v}}+\frac{\mathrm{M}}{\mathrm{d}_1} \mathrm{~d}_2 \mathrm{~g}=\mathrm{Mg}
\)
\(
\mathrm{F}_{\mathrm{V}}=\mathrm{Mg}\left(1-\frac{\mathrm{d}_2}{\mathrm{~d}_1}\right)
\)
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