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Question: A partical of mass m is thrown in a parabolic path towards earth having mass M and radius R. It come...

A partical of mass m is thrown in a parabolic path towards earth having mass M and radius R. It comes to a greatest approach distance R/2 from surface of earth. Magnitude of total energy change required to make the particle moving in an elliptical path having eccentricity 1/2, with the greatest approach point either aphelion or perihelion are :

A

13GMmR\frac{1}{3} \frac{GMm}{R}

B

16GMmR\frac{1}{6} \frac{GMm}{R}

C

12GMmR\frac{1}{2} \frac{GMm}{R}

D

GMmR\frac{GMm}{R}

Answer

B, C

Explanation

Solution

The particle is initially moving in a parabolic path towards the Earth. For a parabolic trajectory under a central gravitational force, the total mechanical energy of the particle is zero.

Einitial=0E_{initial} = 0.

The particle's point of greatest approach to the Earth's surface is R/2R/2. This means the closest distance from the center of the Earth is rmin=R+R/2=3R/2r_{min} = R + R/2 = 3R/2. This point is the periapsis of the parabolic path.

The particle's trajectory is changed to an elliptical path with eccentricity e=1/2e = 1/2. The point r=3R/2r = 3R/2 is given to be either the aphelion (apoapsis) or the perihelion (periapsis) of the new elliptical orbit. Let aa be the semi-major axis of the elliptical orbit. The total energy of a particle in an elliptical orbit is given by Efinal=GMm2aE_{final} = -\frac{GMm}{2a}.

Case 1: The point r=3R/2r = 3R/2 is the perihelion of the elliptical orbit.

The distance of the perihelion from the center is rp=a(1e)r_p = a(1-e).

Given rp=3R/2r_p = 3R/2 and e=1/2e = 1/2.

3R/2=a(11/2)=a(1/2)3R/2 = a(1 - 1/2) = a(1/2)

a=3Ra = 3R.

The total energy of this elliptical orbit is Efinal,1=GMm2a=GMm2(3R)=GMm6RE_{final, 1} = -\frac{GMm}{2a} = -\frac{GMm}{2(3R)} = -\frac{GMm}{6R}.

The change in energy required is ΔE1=Efinal,1Einitial=GMm6R0=GMm6R\Delta E_1 = E_{final, 1} - E_{initial} = -\frac{GMm}{6R} - 0 = -\frac{GMm}{6R}.

The magnitude of the energy change is ΔE1=GMm6R|\Delta E_1| = \frac{GMm}{6R}.

Case 2: The point r=3R/2r = 3R/2 is the aphelion of the elliptical orbit.

The distance of the aphelion from the center is ra=a(1+e)r_a = a(1+e).

Given ra=3R/2r_a = 3R/2 and e=1/2e = 1/2.

3R/2=a(1+1/2)=a(3/2)3R/2 = a(1 + 1/2) = a(3/2)

a=Ra = R.

The total energy of this elliptical orbit is Efinal,2=GMm2a=GMm2(R)=GMm2RE_{final, 2} = -\frac{GMm}{2a} = -\frac{GMm}{2(R)} = -\frac{GMm}{2R}.

The change in energy required is ΔE2=Efinal,2Einitial=GMm2R0=GMm2R\Delta E_2 = E_{final, 2} - E_{initial} = -\frac{GMm}{2R} - 0 = -\frac{GMm}{2R}.

The magnitude of the energy change is ΔE2=GMm2R|\Delta E_2| = \frac{GMm}{2R}.

The question asks for the magnitudes of the total energy change required, given that the point r=3R/2r=3R/2 can be either the aphelion or the perihelion. We found two possible magnitudes: GMm6R\frac{GMm}{6R} and GMm2R\frac{GMm}{2R}.

Therefore, options (B) and (C) are correct.