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UPSC 2016 Maths Optional Paper 1 Q8c — Step-by-Step Solution

15 marks · Section B

Rectilinear motion under variable force · Dynamics & Statics · asked 3× in 14 yrs · Read the full method →

Question

A particle moves in a straight line. Its acceleration is directed towards a fixed point OO in the line and is always equal to μ(a5x2)1/3\mu\left(\dfrac{a^5}{x^2}\right)^{1/3} when it is at a distance xx from OO. If it starts from rest at a distance aa from OO, then find the time, the particle will arrive at OO.

Technique

v dv/dx=v\,dv/dx= acceleration to get v(x)v(x); then T=∫0adx/vT=\int_0^a dx/v; substitution x=as3x=a s^3 turns it into the Beta integral ∫01s2(1−s)−1/2ds=1615\int_0^1 s^2(1-s)^{-1/2}ds=\tfrac{16}{15}.

Solution

The acceleration magnitude is μ(a5/x2)1/3=μ a5/3x−2/3\mu\big(a^5/x^2\big)^{1/3}=\mu\,a^{5/3}x^{-2/3}, directed toward OO (i.e. in the −x-x direction). With the particle at distance x>0x>0,

x¨=−μ a5/3x−2/3.\ddot x=-\mu\,a^{5/3}x^{-2/3}.

Step 1 — First integral (energy / speed)

Use x¨=vdvdx\ddot x=v\dfrac{dv}{dx}:

vdvdx=−μ a5/3x−2/3.v\frac{dv}{dx}=-\mu\,a^{5/3}x^{-2/3}.

Integrate, with v=0v=0 at x=ax=a:

v22=−μ a5/3⋅3x1/3+const.\frac{v^2}{2}=-\mu\,a^{5/3}\cdot 3x^{1/3}+\text{const}.

At x=ax=a: 0=−3μa5/3a1/3+const⇒const=3μa20=-3\mu a^{5/3}a^{1/3}+\text{const}\Rightarrow\text{const}=3\mu a^{2}. Hence

v22=3μa5/3(a1/3−x1/3)⟹v2=6μa5/3(a1/3−x1/3).\frac{v^2}{2}=3\mu a^{5/3}\big(a^{1/3}-x^{1/3}\big)\quad\Longrightarrow\quad v^2=6\mu a^{5/3}\big(a^{1/3}-x^{1/3}\big).

Step 2 — Set up the time integral

Moving toward OO, xx decreases so v=dxdt<0v=\dfrac{dx}{dt}<0; take dxdt=−6μa5/3(a1/3−x1/3)\dfrac{dx}{dt}=-\sqrt{6\mu a^{5/3}\big(a^{1/3}-x^{1/3}\big)}. The time from x=ax=a to x=0x=0 is

T=∫0adx6μa5/3(a1/3−x1/3).T=\int_0^a\frac{dx}{\sqrt{6\mu a^{5/3}\big(a^{1/3}-x^{1/3}\big)}}.

Step 3 — Substitution

Let x=a s3x=a\,s^3 (so x1/3=a1/3sx^{1/3}=a^{1/3}s), dx=3a s2 dsdx=3a\,s^2\,ds; s:0→1s:0\to1. Then a1/3−x1/3=a1/3(1−s)a^{1/3}-x^{1/3}=a^{1/3}(1-s) and

6μa5/3⋅a1/3(1−s)=6μa2(1−s).6\mu a^{5/3}\cdot a^{1/3}(1-s)=6\mu a^{2}(1-s).

So

T=∫013a s2 ds6μa2(1−s)=3aa6μ∫01s21−s ds=36μ∫01s21−s ds.T=\int_0^1\frac{3a\,s^2\,ds}{\sqrt{6\mu a^2(1-s)}}=\frac{3a}{a\sqrt{6\mu}}\int_0^1\frac{s^2}{\sqrt{1-s}}\,ds=\frac{3}{\sqrt{6\mu}}\int_0^1\frac{s^2}{\sqrt{1-s}}\,ds.

Step 4 — Evaluate ∫01s21−s ds\displaystyle\int_0^1\frac{s^2}{\sqrt{1-s}}\,ds

This is a Beta integral: with u=1−su=1-s,

∫01s21−s ds=∫01(1−u)2u du=∫01(u−1/2−2u1/2+u3/2)du=2−43+25=1615.\int_0^1\frac{s^2}{\sqrt{1-s}}\,ds=\int_0^1\frac{(1-u)^2}{\sqrt u}\,du=\int_0^1\big(u^{-1/2}-2u^{1/2}+u^{3/2}\big)du=2-\frac43+\frac25=\frac{16}{15}.

Therefore

T=36μ⋅1615=48156μ=1656μ=1656 μ.T=\frac{3}{\sqrt{6\mu}}\cdot\frac{16}{15}=\frac{48}{15\sqrt{6\mu}}=\frac{16}{5\sqrt{6\mu}}=\frac{16}{5\sqrt6\,\sqrt\mu}.

Rationalising, 1656=16630=8615\dfrac{16}{5\sqrt6}=\dfrac{16\sqrt6}{30}=\dfrac{8\sqrt6}{15}, so

Answer

  T=8615μ=8156μ.  \boxed{\;T=\frac{8\sqrt6}{15\sqrt{\mu}}=\frac{8}{15}\sqrt{\frac{6}{\mu}}.\;}
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