← 2020 Paper 1

UPSC 2020 Maths Optional Paper 1 Q5e — Step-by-Step Solution

10 marks · Section B

Motion in a Plane (Resolved Components / Polar) · Dynamics & Statics · Read the full method →

Question

A light rigid rod ABCABC has three particles each of mass mm attached to it at AA, BB and CC. The rod is struck by a blow PP at right angles to it at a point distant from AA equal to BCBC. Prove that the kinetic energy set up is 12P2ma2ab+b2a2+ab+b2\frac{1}{2}\frac{P^2}{m}\frac{a^2-ab+b^2}{a^2+ab+b^2}, where AB=aAB=a and BC=bBC=b.

Technique

Impulsive motion of a free rigid body: linear impulse =Mv=Mv, moment of impulse about GG =IGω=I_G\omega; then T=12Mv2+12IGω2T=\tfrac12Mv^2+\tfrac12 I_G\omega^2. Cross-check via T=12PVDT=\tfrac12 P\,V_D.

Solution

Setup

Measure distance xx along the rod from AA. Particle positions:

A:  x=0,B:  x=a,C:  x=a+b.A:\;x=0,\qquad B:\;x=a,\qquad C:\;x=a+b .

Total mass =3m=3m. The blow PP (an impulse) is applied perpendicular to the rod at the point DD with AD=bAD=b.

Step 1 — Centre of mass

xˉ=m0+ma+m(a+b)3m=2a+b3.\bar x=\frac{m\cdot0+m\cdot a+m(a+b)}{3m}=\frac{2a+b}{3}.

The rod is free in the plane, struck by an impulse perpendicular to it. After the blow it has a transverse velocity vv of the centre of mass GG and an angular velocity ω\omega about GG.

Step 2 — Impulse–momentum equations

Linear impulse = change in linear momentum (all transverse):

P=3mv.(1)P = 3m\,v. \tag{1}

Angular impulse about GG = change in angular momentum about GG. The blow acts at DD, whose distance from GG (measured along the rod) is

d=xˉAD=2a+b3b=2a2b3=2(ab)3.d = \bar x - AD = \frac{2a+b}{3}-b=\frac{2a-2b}{3}=\frac{2(a-b)}{3}.

Moment of impulse about GG is PdP\cdot d (taking the transverse direction consistently). Thus

Pd=IGω,(2)P\,d = I_G\,\omega, \tag{2}

where IGI_G is the moment of inertia about GG.

Step 3 — Moment of inertia about GG

Distances of the particles from GG:

A:  xˉ0=2a+b3,B:  xˉa=ba3,C:  xˉ(a+b)=(a+2b)3.A:\;\bar x-0=\frac{2a+b}{3},\qquad B:\;\bar x-a=\frac{b-a}{3},\qquad C:\;\bar x-(a+b)=\frac{-(a+2b)}{3}. IG=m[(2a+b3)2+(ab3)2+(a+2b3)2]=m9[(2a+b)2+(ab)2+(a+2b)2].I_G=m\Big[\Big(\tfrac{2a+b}{3}\Big)^2+\Big(\tfrac{a-b}{3}\Big)^2+\Big(\tfrac{a+2b}{3}\Big)^2\Big] =\frac{m}{9}\Big[(2a+b)^2+(a-b)^2+(a+2b)^2\Big].

Expand:

(2a+b)2=4a2+4ab+b2,(ab)2=a22ab+b2,(a+2b)2=a2+4ab+4b2.(2a+b)^2=4a^2+4ab+b^2,\quad(a-b)^2=a^2-2ab+b^2,\quad(a+2b)^2=a^2+4ab+4b^2.

Sum =6a2+6ab+6b2=6(a2+ab+b2)=6a^2+6ab+6b^2=6(a^2+ab+b^2). Hence

IG=m96(a2+ab+b2)=2m3(a2+ab+b2).(3)I_G=\frac{m}{9}\cdot6(a^2+ab+b^2)=\frac{2m}{3}(a^2+ab+b^2). \tag{3}

Step 4 — Velocities

From (1): v=P3mv=\dfrac{P}{3m}.

From (2): ω=PdIG=P2(ab)32m3(a2+ab+b2)=P(ab)m(a2+ab+b2)\omega=\dfrac{P\,d}{I_G}=\dfrac{P\cdot\frac{2(a-b)}{3}}{\frac{2m}{3}(a^2+ab+b^2)}=\dfrac{P(a-b)}{m(a^2+ab+b^2)}.

Step 5 — Kinetic energy

T=12(3m)v2+12IGω2.T=\tfrac12(3m)v^2+\tfrac12 I_G\,\omega^2 .

First term:

12(3m)(P3m)2=3m2P29m2=P26m.\tfrac12(3m)\Big(\frac{P}{3m}\Big)^2=\frac{3m}{2}\cdot\frac{P^2}{9m^2}=\frac{P^2}{6m}.

Second term:

12IGω2=122m3(a2+ab+b2)P2(ab)2m2(a2+ab+b2)2=P2(ab)23m(a2+ab+b2).\tfrac12 I_G\omega^2=\tfrac12\cdot\frac{2m}{3}(a^2+ab+b^2)\cdot\frac{P^2(a-b)^2}{m^2(a^2+ab+b^2)^2} =\frac{P^2(a-b)^2}{3m(a^2+ab+b^2)}.

Add, with common factor P26m\dfrac{P^2}{6m}:

T=P26m[1+2(ab)2a2+ab+b2]=P26m(a2+ab+b2)+2(ab)2a2+ab+b2.T=\frac{P^2}{6m}\left[1+\frac{2(a-b)^2}{a^2+ab+b^2}\right] =\frac{P^2}{6m}\cdot\frac{(a^2+ab+b^2)+2(a-b)^2}{a^2+ab+b^2}.

Numerator:

(a2+ab+b2)+2(a22ab+b2)=3a23ab+3b2=3(a2ab+b2).(a^2+ab+b^2)+2(a^2-2ab+b^2)=3a^2-3ab+3b^2=3(a^2-ab+b^2).

Therefore

T=P26m3(a2ab+b2)a2+ab+b2=P22ma2ab+b2a2+ab+b2.T=\frac{P^2}{6m}\cdot\frac{3(a^2-ab+b^2)}{a^2+ab+b^2} =\frac{P^2}{2m}\cdot\frac{a^2-ab+b^2}{a^2+ab+b^2}.

Answer

T=12P2ma2ab+b2a2+ab+b2\boxed{\,T=\frac{1}{2}\frac{P^2}{m}\cdot\frac{a^2-ab+b^2}{a^2+ab+b^2}\,}
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