Question:

Two bodies of masses $m_1$ and $m_2$ initially at rest at infinite distance apart move towards each other under gravitational force of attraction. Their relative velocity of approach when they are separated by a distance $r$ is (G = Universal gravitational constant)

Updated On: Apr 18, 2024
  • $\left[ \frac{2G\left(m_{1}-m_{2}\right)}{r}\right]^{\frac{1}{2}} $
  • $\left[ \frac{2G\left(m_{1} + m_{2}\right)}{r}\right]^{\frac{1}{2}} $
  • $\left[ \frac{r}{2G\left(m_{1} m_{2}\right)}\right]^{\frac{1}{2}} $
  • $\left[\frac{r}{2 G} m_{1} m_{2}\right]^{1 / 2}$
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The Correct Option is B

Solution and Explanation

Initially when the two masses are at an infinite distance from each other, their gravitational potential energy is zero. When they are at a distance $r$ from each, the gravitational $PE$ is
$PE =\frac{-G m_{1} m_{2}}{r^{2}}$
The minus sign-indicates that there is a decrease in PE. This gives rise to an increase in kinetic energy.
If $v_{1}$ and $v_{2}$ are their respective velocities when they are a distance $r$ apart then, from the law of conservation of energy, we have
$\frac{1}{2} m_{1} v_{1}^{2}=\frac{G m_{1} m_{2}}{r}$ or $v_{1}=\sqrt{\frac{2 G m_{2}}{r}}$
and $\frac{1}{2} m_{2} v_{2}^{2}=\frac{G m_{1} m_{2}}{r}$ or $v_{2}=\sqrt{\frac{2 G m_{1}}{r}}$
Therefore, their relative velocity of approach is
$ v_{1}+v_{2} =\sqrt{\frac{2 G m_{2}}{r}}+\sqrt{\frac{2 G m_{1}}{r}}=\sqrt{\frac{2 G}{r}\left(m_{1}+m_{2}\right)}$
$=\left(\frac{2 G\left(m_{1} \times m_{2}\right)}{r}\right)^{\frac{1}{2}}$
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Concepts Used:

Newtons Law of Gravitation

Gravitational Force

Gravitational force is a central force that depends only on the position of the test mass from the source mass and always acts along the line joining the centers of the two masses.

Newton’s Law of Gravitation:

According to Newton’s law of gravitation, “Every particle in the universe attracts every other particle with a force whose magnitude is,

  • Directly proportional to the product of their masses i.e. F ∝ (M1M2) . . . . (1)
  • Inversely proportional to the square of the distance between their center i.e. (F ∝ 1/r2) . . . . (2)

By combining equations (1) and (2) we get,

F ∝ M1M2/r2

F = G × [M1M2]/r2 . . . . (7)

Or, f(r) = GM1M2/r2 [f(r)is a variable, Non-contact, and conservative force]