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If R is the radius of the earth, the work done to move an earth satellite of mass m from an orbit of radius 2R to another orbit of radius 3R is-
1. \(\frac{GMm}{12R}\)
2. \(\frac{GMm}{R}\)
3. \(\frac{GMm}{5R}\)
4. zero

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Correct Answer - Option 1 : \(\frac{GMm}{12R}\)

The correct answer is option 1) i.e. \(\frac{GMm}{12R}\)

CONCEPT:

  • Gravitational Potential Energy: It is the energy possessed by a body at a certain point when work is done by the force of gravity in bringing the object from infinity to that point.
    • The gravitational potential energy between two masses m1 and m2 separated by a distance r is given by

\(U = -\frac{Gm_1m_2}{r}\)

EXPLANATION:

  • The gravitational potential energy of the satellite\(U = -\frac{GMm}{R}\) (where M is the mass of earth)

The kinetic energy of the satellite\(K =\frac{1}{2}mv^2\)

The centripetal force of the satellite is provided by the gravitational force exerted by the earth:

\(\Rightarrow \frac{mv^2}{R} = \frac{GMm}{R^2}\)

\(\Rightarrow v^2 = \frac{GM}{R}\)      ----(1)

The total energy of the satellite, TE = K + U

\(\Rightarrow TE =\frac{1}{2}mv^2 +( -\frac{GMm}{R})\)      ----(2)

Substituting (1) in (2),

\(\Rightarrow TE= \frac{1}{2}m(\frac{GM}{R}) +( -\frac{GMm}{R})\)

\(\Rightarrow TE =- \frac{GMm}{2R}\)

The work done or energy required to move from 2R to 3R will be:

\(\Rightarrow W =- \frac{GMm}{2}\times [\frac{1}{3R} - \frac{1}{2R}]\)

\(\Rightarrow W = \frac{GMm}{12R}\)

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