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NEET PHYSICSEasy

Assuming that the gravitational potential energy of an object at infinity is zero, the change in potential energy (final - initial) of an object of mass mm when taken to a height hh from the surface of the earth (of radius RR and mass MM), is given by:

A

GMmR+h-\frac{GMm}{R+h}

B

GMmhR(R+h)\frac{GMmh}{R(R+h)}

C

mghmgh

D

GMmR+h\frac{GMm}{R+h}

Step-by-Step Solution

  1. Formula: The gravitational potential energy of a mass mm at a distance rr from the center of the Earth is given by U(r)=GMmrU(r) = -\frac{GMm}{r} [Eq. 7.23, 7.24].
  2. Initial State: At the surface of the Earth, the distance from the center is RR. Thus, the initial potential energy is Ui=GMmRU_i = -\frac{GMm}{R}.
  3. Final State: At a height hh above the surface, the distance from the center is r=R+hr = R + h. Thus, the final potential energy is Uf=GMmR+hU_f = -\frac{GMm}{R+h}.
  4. Change in Potential Energy (ΔU\Delta U): ΔU=UfUi\Delta U = U_f - U_i ΔU=(GMmR+h)(GMmR)\Delta U = \left( -\frac{GMm}{R+h} \right) - \left( -\frac{GMm}{R} \right) ΔU=GMmRGMmR+h\Delta U = \frac{GMm}{R} - \frac{GMm}{R+h} ΔU=GMm(1R1R+h)\Delta U = GMm \left( \frac{1}{R} - \frac{1}{R+h} \right) ΔU=GMm(R+hRR(R+h))\Delta U = GMm \left( \frac{R+h-R}{R(R+h)} \right) ΔU=GMmhR(R+h)\Delta U = \frac{GMmh}{R(R+h)} (Note: This expression reduces to mghmgh only when hRh \ll R).
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