Chapter 7: Problem 15
A uniform spherical shell gradually shrinks maintaining its shape. The gravitational potential at the centre (A) Increases (B) Decreases (C) Remains constant (D) Oscillates
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Chapter 7: Problem 15
A uniform spherical shell gradually shrinks maintaining its shape. The gravitational potential at the centre (A) Increases (B) Decreases (C) Remains constant (D) Oscillates
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Suppose the gravitational force varies inversely as the \(n^{\text {th }}\) power of distance. Then the time period of a planet in circular orbit of radius \(R\) around the sun will be proportional to (A) \(R^{\left(\frac{n-2}{2}\right)}\) (B) \(R^{\left(\frac{n-1}{2}\right)}\) (C) \(R^{n}\) (D) \(R^{\left(\frac{n-2}{2}\right)}\)
A simple pendulum has a time period \(T_{1}\) when on the earth's surface, and \(T_{2}\) when taken to a height \(R\) above the earth's surface, where \(R\) is radius of earth. The value of \(T_{2} / T_{1}\) is (A) 1 (B) \(\sqrt{2}\) (C) 4 (D) 2
The height at which the acceleration due to gravity becomes \(\frac{g}{9}\) (where \(g\) = the acceleration due to gravity on the surface of the earth) in terms of \(R\), the radius of the earth is (A) \(\frac{R}{\sqrt{2}}\) (B) \(R / 2\) (C) \(\sqrt{2} R\) (D) \(2 R\)
Calculate the ratio \(m_{0} / m\) for a rocket if it is to escape from the earth. Given escape velocity \(=11.2 \mathrm{~km} / \mathrm{s}\) and exhaust speed of gases is \(2 \mathrm{~km} / \mathrm{s}\).
Four particles of equal mass \(M\) move along a circle of radius \(R\) under the action of their mutual gravitational attraction. The speed of each particle is (A) \(\frac{G M}{R}\) (B) \(\sqrt{\left(\frac{G M}{R}\right)}\) (C) \(\sqrt{\left[\frac{G M}{R}\left(\frac{2 \sqrt{2}+1}{4}\right)\right]}\) (D) \(\sqrt{\left[\frac{G M}{R}(\sqrt{2}+1)\right]}\)
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