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The work done in slowly lifting a body f...

The work done in slowly lifting a body from earth's surface to a height R (radius of earth) is equal to two times the work done in lifting the same body from earth's surface to a height h. Here h is equal to

A

`(R)/(4)`

B

`(R)/(3)`

C

`(R)/(6)`

D

`(R)/(2)`

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The correct Answer is:
To solve the problem, we need to find the height \( h \) such that the work done in lifting a body from the Earth's surface to a height \( R \) (the radius of the Earth) is equal to two times the work done in lifting the same body to a height \( h \). ### Step-by-Step Solution: 1. **Understanding Work Done in Lifting**: The work done in lifting a mass \( m \) to a height \( h \) in a gravitational field is equal to the change in gravitational potential energy. The formula for gravitational potential energy at a height \( h \) is given by: \[ U = -\frac{GMm}{r} \] where \( G \) is the gravitational constant, \( M \) is the mass of the Earth, and \( r \) is the distance from the center of the Earth. 2. **Work Done to Height \( R \)**: When lifting the body to a height \( R \): \[ W_1 = U_{\text{final}} - U_{\text{initial}} = \left(-\frac{GMm}{R}\right) - \left(-\frac{GMm}{R}\right) = \frac{GMm}{R} - \frac{GMm}{2R} \] Simplifying this gives: \[ W_1 = \frac{GMm}{2R} \] 3. **Work Done to Height \( h \)**: Now, for lifting the body to height \( h \): \[ W_2 = U_{\text{final}} - U_{\text{initial}} = \left(-\frac{GMm}{R+h}\right) - \left(-\frac{GMm}{R}\right) = \frac{GMm}{R} - \frac{GMm}{R+h} \] Simplifying this gives: \[ W_2 = GMm \left(\frac{1}{R} - \frac{1}{R+h}\right) = GMm \left(\frac{(R+h) - R}{R(R+h)}\right) = \frac{GMmh}{R(R+h)} \] 4. **Setting Up the Equation**: According to the problem, the work done to lift to height \( R \) is equal to twice the work done to lift to height \( h \): \[ W_1 = 2W_2 \] Substituting the expressions for \( W_1 \) and \( W_2 \): \[ \frac{GMm}{2R} = 2 \left(\frac{GMmh}{R(R+h)}\right) \] 5. **Canceling Common Terms**: We can cancel \( GMm \) from both sides (assuming \( m \neq 0 \)): \[ \frac{1}{2R} = \frac{2h}{R(R+h)} \] 6. **Cross-Multiplying**: Cross-multiplying gives: \[ R(R+h) = 4Rh \] This simplifies to: \[ R^2 + Rh = 4Rh \] Rearranging gives: \[ R^2 = 3Rh \] 7. **Solving for \( h \)**: Dividing both sides by \( R \) (assuming \( R \neq 0 \)): \[ h = \frac{R}{3} \] ### Final Answer: Thus, the height \( h \) is: \[ h = \frac{R}{3} \]
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