MHT CET · Physics · Oscillations
A coin is placed on the horizontal plate. Plate performs S.H.M. vertically with
angular frequency ' \(\omega^{\prime}\). The amplitude (A) of oscillations is gradually increased.
The coin will lose contact with plate for the first time when amplitude is
\((\mathrm{g}=\) acceleration due to gravity \()\)
- A \(\frac{\mathrm{g}}{\omega^{2}}\)
- B zero
- C \(\frac{\omega^{2}}{\mathrm{~g}}\)
- D \(\frac{\mathrm{A}}{2}\)
Answer & Solution
Correct Answer
(A) \(\frac{\mathrm{g}}{\omega^{2}}\)
Step-by-step Solution
Detailed explanation
(D)
The coin will lose contact with the plate when its acceleration in downward direction just exceeds acceleration due to gravity.
\(\begin{array}{l}
\therefore \omega^{2} \mathrm{x}=\mathrm{g} \\
\therefore \mathrm{x} \quad=\frac{\mathrm{g}}{\omega^{2}}
\end{array}\)
The coin will lose contact with the plate when its acceleration in downward direction just exceeds acceleration due to gravity.
\(\begin{array}{l}
\therefore \omega^{2} \mathrm{x}=\mathrm{g} \\
\therefore \mathrm{x} \quad=\frac{\mathrm{g}}{\omega^{2}}
\end{array}\)
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