Chapter 8: Problem 41
Energy required to move a body of mass \(m\) from an orbit of radius \(2 R\) to \(3 R\) is (a) \(\frac{G M m}{12 R^{2}}\) (b) \(\frac{G M m}{3 R^{2}}\) (c) \(\frac{G M m}{8 R}\) (d) \(\frac{G M m}{6 R}\)
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Chapter 8: Problem 41
Energy required to move a body of mass \(m\) from an orbit of radius \(2 R\) to \(3 R\) is (a) \(\frac{G M m}{12 R^{2}}\) (b) \(\frac{G M m}{3 R^{2}}\) (c) \(\frac{G M m}{8 R}\) (d) \(\frac{G M m}{6 R}\)
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A satellite is revolving round the earth with orbital speed \(v_{0}\). If it stops suddenly, the speed with which it will strike the surface of earth would be \(\left(v_{e}=\right.\) escape velocity of a particle on earth's surface) (a) \(\frac{v_{e}^{2}}{v_{0}}\) (b) \(v_{0}\) (c) \(\sqrt{v_{e}^{2}-v_{0}^{2}}\) (d) \(\sqrt{v_{e}^{2}-2 v_{0}^{2}}\)
The gravitational potential due to the earth at infinite distance from it is zero. Let the gravitational potential at a point \(P\) be \(-5 J / k g\). Suppose, we arbitrarily assume the gravitational potential at infinity to \(\mathrm{be}+10 \mathrm{~J} / \mathrm{kg}\), then the gravitational potential at \(P\) will be (a) \(-5 \mathrm{~J} / \mathrm{kg}\) (b) \(+5 J / k g\) (c) \(-15 \mathrm{~J} / \mathrm{kg}\) (d) \(+15 J / k g\)
Two types of balances, the beam balance and the spring balance are commonly used for measuring weight in shops. If we are on the moon, we can continue to use (a) Only the beam type balance without any change (b) Only the spring balance without any change (c) Both the balances without any change (d) Neither of the two balances without making any change
A boy can jump to a height \(h\) on ground level. What should be the radius of a sphere of density \(d\) such that on jumping on it, he escapes out of the gravitational field of the sphere (a) \(\left[\frac{4 \pi}{3} \frac{G d}{g h}\right]^{1 / 2}\) (b) \(\left[\frac{4 \pi}{3} \frac{g h}{G d}\right]^{1 / 2}\) (c) \(\left[\frac{3}{4 \pi} \frac{g h}{G d}\right]^{1 / 2}\) (d) \(\left[\frac{3}{4 \pi} \frac{G d}{g h}\right]^{1 / 2}\)
A spherical planet far out in space has a mass \(M_{0}\) and diameter \(D_{0}\). A particle of mass \(m\) falling freely near the surface of this planet will experience an acceleration due to gravity which is equal to (a) \(G M_{0} / D_{0}^{2}\) (b) \(4 m G M_{0} / D_{0}^{2}\) (c) \(4 G M_{0} / D_{0}^{2}\) (d) \(G m M_{0} / D_{0}^{2}\)
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