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NEET PHYSICSMedium

A particle of mass mm is projected with a velocity, v=kvev = kv_e (k<1k < 1) from the surface of the earth. The maximum height, above the surface, reached by the particle is: (Where ve=v_e = escape velocity, R=R = the radius of the earth)

A

R2k1+k\frac{R^2k}{1+k}

B

Rk21k2\frac{Rk^2}{1-k^2}

C

R(k1k)2R\left(\frac{k}{1-k}\right)^2

D

R(k1+k)2R\left(\frac{k}{1+k}\right)^2

Step-by-Step Solution

  1. Conservation of Energy: The total mechanical energy of the particle is conserved. Let the maximum height reached be hh. At this point, the velocity of the particle is zero. Ei=EfE_i = E_f Ki+Ui=Kf+UfK_i + U_i = K_f + U_f
  2. Initial Energy: At the surface (r=Rr=R), velocity v=kvev = kv_e. Since escape velocity ve=2GMRv_e = \sqrt{\frac{2GM}{R}}, then v2=k22GMRv^2 = k^2 \frac{2GM}{R}. Ki=12mv2=12m(k22GMR)=k2GMmRK_i = \frac{1}{2}mv^2 = \frac{1}{2}m \left( k^2 \frac{2GM}{R} \right) = \frac{k^2 GMm}{R} Ui=GMmRU_i = -\frac{GMm}{R}
  3. Final Energy: At maximum height (r=R+hr = R+h), velocity is zero. Kf=0K_f = 0 Uf=GMmR+hU_f = -\frac{GMm}{R+h}
  4. Solve for h: k2GMmRGMmR=GMmR+h\frac{k^2 GMm}{R} - \frac{GMm}{R} = -\frac{GMm}{R+h} GMmR(k21)=GMmR+h\frac{GMm}{R}(k^2 - 1) = -\frac{GMm}{R+h} 1k2R=1R+h\frac{1-k^2}{R} = \frac{1}{R+h} R+h=R1k2R+h = \frac{R}{1-k^2} h=R1k2R=R(1(1k2)1k2)=Rk21k2h = \frac{R}{1-k^2} - R = R \left( \frac{1 - (1-k^2)}{1-k^2} \right) = \frac{Rk^2}{1-k^2}
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