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UPSC 2015 Maths Optional Paper 1 Q6d — Step-by-Step Solution

13 marks · Section B

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

Question

A mass starts from rest at a distance aa from the centre of force which attracts inversely as the distance. Find the time of arriving at the centre.

Technique

Energy first integral (multiply by r˙\dot r); separation of variables; Gaussian substitution r=aeu2r=ae^{-u^2} converts the singular endpoint at r=0r=0 to a Gaussian integral on [0,)[0,\infty).

Solution

Setup. Particle on a line, attracted toward origin with force magnitude F=k/rF=k/r (per unit mass), k>0k>0. Equation of motion (taking r>0r>0, attraction toward origin):

r¨=kr.\ddot r=-\dfrac{k}{r}.

(For motion along a line, take rr as the signed coordinate; with r>0r>0 initially and attraction toward origin, the force is in the r-r direction.)

Initial conditions: r(0)=ar(0)=a, r˙(0)=0\dot r(0)=0.

Step 1 — Energy first integral

Multiply by r˙\dot r:

r˙r¨=kr˙r.\dot r\ddot r=-\dfrac{k\dot r}{r}. ddt ⁣(r˙22)=kddt ⁣(lnr).\dfrac{d}{dt}\!\left(\dfrac{\dot r^2}{2}\right)=-k\dfrac{d}{dt}\!\left(\ln r\right).

Integrate from t=0t=0 to tt, using r˙(0)=0\dot r(0)=0, r(0)=ar(0)=a:

r˙22=k(lnrlna)=kln(a/r).\dfrac{\dot r^2}{2}=-k(\ln r-\ln a)=k\ln(a/r).

So

r˙2=2kln(a/r).\dot r^2=2k\ln(a/r).

Since rr is decreasing (particle moves toward origin), r˙<0\dot r<0 and

r˙=2kln(a/r).\dot r=-\sqrt{2k\ln(a/r)}.

Step 2 — Separate and integrate

drdt=2kln(a/r)        dt=dr2kln(a/r).\dfrac{dr}{dt}=-\sqrt{2k\ln(a/r)}\;\;\Longrightarrow\;\;dt=-\dfrac{dr}{\sqrt{2k\ln(a/r)}}.

Time to reach the centre:

T=r=ar=0 ⁣ ⁣ ⁣dr2kln(a/r)=0adr2kln(a/r).T=\int_{r=a}^{r=0}\!\!\!-\dfrac{dr}{\sqrt{2k\ln(a/r)}}=\int_0^a\dfrac{dr}{\sqrt{2k\ln(a/r)}}.

Step 3 — Substitute r=aeu2r=ae^{-u^2} (so u0u\to 0 at r=ar=a, uu\to\infty at r=0r=0)

dr=aeu2(2u)du=2uaeu2dudr=ae^{-u^2}(-2u)\,du=-2ua e^{-u^2}\,du.

ln(a/r)=ln(eu2)=u2\ln(a/r)=\ln(e^{u^2})=u^2.

2kln(a/r)=2ku\sqrt{2k\ln(a/r)}=\sqrt{2k}\cdot u.

So

T=u=0u=(2uaeu2)du2ku=2a2k0eu2du.T=\int_{u=0}^{u=\infty}\dfrac{-(-2ua e^{-u^2})\,du}{\sqrt{2k}\cdot u}=\dfrac{2a}{\sqrt{2k}}\int_0^\infty e^{-u^2}\,du.

The Gaussian integral: 0eu2du=π2\int_0^\infty e^{-u^2}\,du=\dfrac{\sqrt\pi}{2}.

T=2a2kπ2=aπ2k=aπ2k.T=\dfrac{2a}{\sqrt{2k}}\cdot\dfrac{\sqrt\pi}{2}=\dfrac{a\sqrt\pi}{\sqrt{2k}}=a\sqrt{\dfrac{\pi}{2k}}.

Answer

  T=aπ2k.  \boxed{\;T=a\sqrt{\dfrac{\pi}{2k}}.\;}
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