MHT CET · Physics · Oscillations
A U-tube of a uniform bore is with its arm vertical. The length of the liquid in the two arms or the U-tube is \(L\); the time period \(T\) of the oscillation of the liquid column when it is displaced by ' \(Y\) ' is ( \(g=\) acceleration due to gravity)
- A \(2 \pi \sqrt{\frac{Y}{g}}\)
- B \(2 \pi \sqrt{\frac{2 L}{g}}\)
- C \(2 \pi \sqrt{\frac{L}{g}}\)
- D \(2 \pi \sqrt{\frac{L}{2 g}}\)
Answer & Solution
Correct Answer
(D) \(2 \pi \sqrt{\frac{L}{2 g}}\)
Step-by-step Solution
Detailed explanation
Due to the tiny displacement \(y\), the force balance in the tube reads:
\(\begin{aligned} & \frac{d^2 y}{d t^2}=-\frac{F}{m}=-\left(\frac{2 y \rho g}{L A \rho}\right) \\ & \Rightarrow \frac{d^2 y}{d t^2}=-\left(\frac{2 g}{L}\right) y\end{aligned}\)
or
\(\omega^2=\frac{2 g}{L} \Rightarrow T=2 \pi \sqrt{\frac{L}{2 g}}\)
\(\begin{aligned} & \frac{d^2 y}{d t^2}=-\frac{F}{m}=-\left(\frac{2 y \rho g}{L A \rho}\right) \\ & \Rightarrow \frac{d^2 y}{d t^2}=-\left(\frac{2 g}{L}\right) y\end{aligned}\)
or
\(\omega^2=\frac{2 g}{L} \Rightarrow T=2 \pi \sqrt{\frac{L}{2 g}}\)
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