A small sphere of radius r is placed as a concave surface of radius of curvature R a little away from the center. When the sphere is released, it oscillates. Assuming the Oscillation to be simple harmonic motion, and r << R then the time period is

1
\(2\pi \sqrt\frac{R}{g}\)
2
\(2\pi \sqrt\frac{3R}{2g}\)
3
\(2\pi \sqrt\frac{2R}{3g}\)
4
\(2\pi \sqrt\frac{R}{2g}\)

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