← 2020 Paper 1

UPSC 2020 Maths Optional Paper 1 Q7c-ii — Step-by-Step Solution

10 marks · Section B

Orbits under inverse-square central force · Dynamics & Statics · asked 2× in 13 yrs · Read the full method →

Question

A particle starts at a great distance with velocity VV. Let pp be the length of the perpendicular from the centre of a star on the tangent to the initial path of the particle. Show that the least distance of the particle from the centre of the star is λ\lambda, where V2λ=μ2+p2V4μV^2\lambda=\sqrt{\mu^2+p^2V^4}-\mu. Here μ\mu is a constant.

Technique

Central orbit conservation laws: angular momentum h=pVh=pV from initial data; energy E=12V2E=\tfrac12V^2 at infinity; set r˙=0\dot r=0 at r=λr=\lambda and solve the resulting quadratic.

Solution

The particle moves under the star’s attraction. Per unit mass, the attractive central force is the inverse-square law F=μr2F=\dfrac{\mu}{r^2} (directed toward the centre), with potential energy U(r)=μrU(r)=-\dfrac{\mu}{r}. Two conserved quantities govern the motion: angular momentum and energy (both per unit mass).

Step 1 — Angular momentum (from the initial data)

At a great distance the speed is VV and the perpendicular from the centre on the line of motion (the impact parameter) is pp. Angular momentum per unit mass:

h=Vp=pV.h=V\cdot p=pV .

This is constant throughout the motion.

Step 2 — Energy (evaluate at infinity)

At “a great distance” rr\to\infty, U0U\to0, speed =V=V, so total energy per unit mass:

E=12V2+0=12V2.E=\tfrac12V^2+0=\tfrac12V^2 .

Step 3 — Condition at least distance

At the closest approach r=λr=\lambda, the radial velocity vanishes (r˙=0\dot r=0), so the whole speed is transverse:

vclosest=hλ=pVλ.v_{\text{closest}}=\frac{h}{\lambda}=\frac{pV}{\lambda}.

Energy conservation at r=λr=\lambda:

12(pVλ)2μλ=12V2.\tfrac12\Big(\frac{pV}{\lambda}\Big)^2-\frac{\mu}{\lambda}=\tfrac12V^2 .

Step 4 — Solve for λ\lambda

Multiply through by 2λ22\lambda^2:

p2V22μλ=V2λ2,p^2V^2-2\mu\lambda=V^2\lambda^2 , V2λ2+2μλp2V2=0.V^2\lambda^2+2\mu\lambda-p^2V^2=0 .

Quadratic in λ\lambda; take the positive root (distance >0>0):

λ=2μ+4μ2+4V2p2V22V2=μ+μ2+p2V4V2.\lambda=\frac{-2\mu+\sqrt{4\mu^2+4V^2\cdot p^2V^2}}{2V^2} =\frac{-\mu+\sqrt{\mu^2+p^2V^4}}{V^2}.

Hence

V2λ=μ2+p2V4μ.V^2\lambda=\sqrt{\mu^2+p^2V^4}-\mu .

Answer

 V2λ=μ2+p2V4μ \boxed{\ V^2\lambda=\sqrt{\mu^2+p^2V^4}-\mu\ }
We post more of this — worked solutions, CSAT trap breakdowns, guide chapters — a few times a week on Telegram. Free, no sign-in. Join

This solution is part of the Maths Coverage Map — 13 years, mapped. Get the take-away PDF free.