A cylindrical vessel containing a liquid of density \(\rho\) is closed by a smooth piston of mass \(m\) as shown. If atmospheric pressure is \(P_{0}\), radius of cylinder is '\(r\)' and height of liquid is '\(h\)', then the force at the bottom of the cylinder is
Show Hint
Pressure at the bottom is atmospheric pressure plus the piston's weight per area plus the liquid column pressure; multiply by the base area.
Step 1: Understanding the Concept
Pressure just below the piston is \(P_{0}+\frac{mg}{\pi r^{2}}\), since the piston's weight is spread over the area \(\pi r^{2}\).
Step 2: Calculation
Going down a depth \(h\) adds \(\rho gh\). Pressure at the bottom \(=P_{0}+\frac{mg}{\pi r^{2}}+\rho gh\). Force \(=\) pressure \(\times\) area \(=\left(P_{0}+\frac{mg}{\pi r^{2}}+\rho gh\right)\pi r^{2}\).
Step 3: Compare the options
This matches the first option. The third option multiplies by \(\pi r\), which is not an area.
Final Answer:
The force at the bottom is \(\left(P_{0}+\frac{mg}{\pi r^{2}}+\rho gh\right)\pi r^{2}\).
\[ \boxed{\text{(A) }\left(P_{0}+\dfrac{mg}{\pi r^{2}}+\rho gh\right)\pi r^{2}} \]