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Q. A bullet is fired vertically upwards with velocity $v$ from the surface of a spherical planet. When it reaches its maximum height, its acceleration due to the planets gravity is $1/4^{th}$ of its value at the surface of the planet. If the escape velocity from the planet is $v_{esc} = v\,\sqrt{N}$, then the value of $N$ is (ignore energy loss due to atmosphere)

Gravitation

Solution:

Given situation is shown in the figure.
image
Let acceleration due to gravity at the surface of the planet be $g$. At height $h$ above planets surface $v = 0$.
According to question, acceleration due to gravity of the planet at height $h$ above its surface becomes $g/4$.
$g_{h} = \frac{g}{4} = \frac{g}{\left(1+\frac{h}{R}\right)^{2}}$
$4 = \left(1+\frac{h}{R}\right)^{2}$
$\Rightarrow 1+\frac{h}{R}=2$
$\frac{h}{R} = 1$
$\Rightarrow h = R$.
So, velocity of the bullet becomes zero at $h = R$.
Also $v_{esc} = v\sqrt{N}$
$\Rightarrow \sqrt{\frac{2\,GM}{R}} = v\sqrt{N}\quad\ldots\left(i\right)$
Applying energy conservation principle,
Energy of bullet at surface of earth
$=$ Energy of bullet at highest point
$\frac{-GMm}{R}+\frac{1}{2}mv^{2} = \frac{-GMm}{2R}$
$\frac{1}{2}mv^{2} = \frac{GMm}{2R}$
$\therefore v = \sqrt{\frac{GM}{R}}$
Putting this value in eqn. $\left(i\right)$, we get
$\sqrt{\frac{2\,GM}{R}} = \sqrt{\frac{NGM}{R}}$
$\therefore N = 2$