MHT CET · Physics · Mechanical Properties of Fluids
A hemispherical portion of radius ' \(R\) ' is removed from the bottom of a cylinder of radius ' R '. The volume of the remaining cylinder is ' \(V\) ' and its mass is ' \(M\) '. It is suspended by a string in a liquid of density ' \(\rho\) ' where it stays vertical. The upper surface of the cylinder is at a depth ' \(h\) ' below the liquid surface. The force on the bottom of the liquid is
- A Mg
- B \(\mathrm{Mg}-\mathrm{V} \rho \mathrm{g}\)
- C \(\mathrm{Mg}+\pi \mathrm{R}^2 \mathrm{~h} \rho g\)
- D \(\quad \rho g\left(V+\pi r^2 h\right)\)
Answer & Solution
Correct Answer
(D) \(\quad \rho g\left(V+\pi r^2 h\right)\)
Step-by-step Solution
Detailed explanation
Net upward zone force on the bottom of the liquid \(=\) weight of the liquid displaced by cylinder + thrust force on upper surface of the cylinder due to h column of liquid
\(\begin{aligned}
& F_{\text {net }}=\rho V g+\rho g h \times \pi r^2 \\
&=\rho g\left(V+\pi r^2 h\right)
\end{aligned}\)
\(\begin{aligned}
& F_{\text {net }}=\rho V g+\rho g h \times \pi r^2 \\
&=\rho g\left(V+\pi r^2 h\right)
\end{aligned}\)
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