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Escape Velocity Multiplier for Vertical Launch on Spherical Planet

A projectile is launched vertically upwards with initial speed vv from the surface of a spherical planet. Upon reaching its maximum height, its gravitational acceleration drops to 1/4th1/4^{\text{th}} of its value at the surface of the planet. If the escape speed from this planet is given by vesc=vNv_{\text{esc}} = v\sqrt{N}, calculate the value of NN (neglect any atmospheric resistance).

Official Numerical Answer2

Topics & Concepts

Step-by-Step Solution

Let MM and RR be the mass and radius of the spherical planet, respectively.

Step 1: Determine the maximum height reached by the projectile

The acceleration due to gravity at a distance rr from the center of the planet is given by: g(r)=GMr2g(r) = \frac{GM}{r^2}

At the surface of the planet (r=Rr = R), the gravitational acceleration is: g0=GMR2g_0 = \frac{GM}{R^2}

It is given that at the maximum height (distance rr from the center), the gravitational acceleration drops to 14th\frac{1}{4}^{\text{th}} of its surface value: g(r)=14g0g(r) = \frac{1}{4} g_0

Substituting the expressions for gravitational acceleration: GMr2=14GMR2\frac{GM}{r^2} = \frac{1}{4} \frac{GM}{R^2}

Solving for rr: r2=4R2  ⟹  r=2Rr^2 = 4R^2 \implies r = 2R

Step 2: Apply the law of conservation of mechanical energy

At the surface of the planet, the mechanical energy EiE_i of the projectile is: Ei=12mv2−GMmRE_i = \frac{1}{2} m v^2 - \frac{GMm}{R}

At the maximum height r=2Rr = 2R, the projectile momentarily comes to rest (vf=0v_f = 0), so its mechanical energy EfE_f is: Ef=0−GMm2RE_f = 0 - \frac{GMm}{2R}

By conservation of mechanical energy (Ei=EfE_i = E_f): 12mv2−GMmR=−GMm2R\frac{1}{2} m v^2 - \frac{GMm}{R} = -\frac{GMm}{2R}

12mv2=GMmR−GMm2R=GMm2R\frac{1}{2} m v^2 = \frac{GMm}{R} - \frac{GMm}{2R} = \frac{GMm}{2R}

v2=GMRv^2 = \frac{GM}{R}

Step 3: Calculate the escape velocity

The escape speed vescv_{\text{esc}} from the surface of the planet is defined as: vesc=2GMRv_{\text{esc}} = \sqrt{\frac{2GM}{R}}

Substituting GMR=v2\frac{GM}{R} = v^2 into the escape velocity formula: vesc=2v2=v2v_{\text{esc}} = \sqrt{2 v^2} = v \sqrt{2}

Comparing this with the given relation vesc=vNv_{\text{esc}} = v\sqrt{N}: N=2N = 2