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UPSC 2014 Maths Optional Paper 1 Q8b — Step-by-Step Solution

15 marks · Section B

Rectilinear motion under variable force · Dynamics & Statics · asked 3× in 13 yrs · Read the full method →

Question

A particle is acted on by a force parallel to the axis of yy whose acceleration (always towards the axis of xx) is μy2\mu y^{-2} and when y=ay=a, it is projected parallel to the axis of xx with velocity 2μa\sqrt{\dfrac{2\mu}{a}}. Find the parametric equation of the path of the particle. Here μ\mu is a constant.

Technique

Energy integral for the yy-equation; eliminate tt to get xx as function of yy; trigonometric substitution leading to cycloid form.

Solution

Setup. Force only in yy-direction, magnitude μ/y2\mu/y^{2}, toward xx-axis (negative yy for y>0y>0):

x¨=0,y¨=μy2.\ddot x=0,\quad\ddot y=-\dfrac{\mu}{y^{2}}.

ICs at t=0t=0: x=0,y=ax=0,\,y=a; x˙=2μ/a,y˙=0\dot x=\sqrt{2\mu/a},\,\dot y=0.

Step 1 — Horizontal motion

x¨=0x˙=2μ/a\ddot x=0\Rightarrow\dot x=\sqrt{2\mu/a} constant, so x=t2μ/ax=t\sqrt{2\mu/a}.

Step 2 — Energy integral for yy

Multiply y¨=μ/y2\ddot y=-\mu/y^{2} by y˙\dot y and integrate w.r.t. tt:

12y˙2=μy+C.\dfrac{1}{2}\dot y^{2}=\dfrac{\mu}{y}+C.

IC (t=0t=0, y˙=0,y=a\dot y=0,\,y=a): C=μ/aC=-\mu/a. So

y˙2=2μ(ay)ay.\dot y^{2}=\dfrac{2\mu(a-y)}{ay}.

Step 3 — Eliminate tt to get path

The horizontal coordinate parametrised by yy:

x=2μ/at=2μ/aaydyy˙=2μ/aay12μ(ay)/(ay)dy=yayaydy.x=\sqrt{2\mu/a}\,t=\sqrt{2\mu/a}\int_a^y\dfrac{dy'}{\dot y}=\sqrt{2\mu/a}\int_a^y\dfrac{-1}{\sqrt{2\mu(a-y')/(ay')}}dy'=\int_y^a\sqrt{\dfrac{y'}{a-y'}}\,dy'.

(Negative sign of y˙\dot y flipped the integral limits.)

Step 4 — Trigonometric substitution

Let y=asin2ϕy'=a\sin^{2}\phi, so ay=acos2ϕa-y'=a\cos^{2}\phi, dy=asin2ϕdϕ=2asinϕcosϕdϕdy'=a\sin 2\phi\,d\phi=2a\sin\phi\cos\phi\,d\phi. Then y/(ay)=tanϕ\sqrt{y'/(a-y')}=\tan\phi.

y/(ay)dy=2asin2ϕdϕ=a(1cos2ϕ)dϕ.\sqrt{y'/(a-y')}\,dy'=2a\sin^{2}\phi\,d\phi=a(1-\cos 2\phi)\,d\phi.

Integrate from ϕ=ϕy\phi=\phi_y (where asin2ϕy=ya\sin^{2}\phi_y=y) to ϕ=π/2\phi=\pi/2 (where y=ay'=a):

x=ϕyπ/2a(1cos2ϕ)dϕ=a ⁣[ϕsin2ϕ2]ϕyπ/2=a ⁣(π2ϕy+sin2ϕy2).x=\int_{\phi_y}^{\pi/2}a(1-\cos 2\phi)\,d\phi=a\!\left[\phi-\dfrac{\sin 2\phi}{2}\right]_{\phi_y}^{\pi/2}=a\!\left(\dfrac{\pi}{2}-\phi_y+\dfrac{\sin 2\phi_y}{2}\right).

Step 5 — Substitute η=π2ϕy\eta=\pi-2\phi_y (cycloid parameter)

With η=π2ϕy\eta=\pi-2\phi_y, ϕy=(πη)/2\phi_y=(\pi-\eta)/2: sin2ϕy=sin(πη)=sinη\sin 2\phi_y=\sin(\pi-\eta)=\sin\eta. y=asin2ϕy=a(1cos2ϕy)/2=a(1cos(πη))/2=a(1+cosη)/2y=a\sin^{2}\phi_y=a(1-\cos 2\phi_y)/2=a(1-\cos(\pi-\eta))/2=a(1+\cos\eta)/2.

And π/2ϕy=π/2(πη)/2=η/2\pi/2-\phi_y=\pi/2-(\pi-\eta)/2=\eta/2. So

x=a ⁣(η2+sinη2)=a2(η+sinη).x=a\!\left(\dfrac{\eta}{2}+\dfrac{\sin\eta}{2}\right)=\dfrac{a}{2}(\eta+\sin\eta).

Step 6 — Parametric form

Answer

  x=a2(η+sinη),y=a2(1+cosη),η0.  \boxed{\;x=\dfrac{a}{2}(\eta+\sin\eta),\quad y=\dfrac{a}{2}(1+\cos\eta),\quad\eta\ge 0.\;}
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