← 2013 Paper 1

UPSC 2013 Maths Optional Paper 1 Q7a — Step-by-Step Solution

20 marks · Section B

Constrained motion · Dynamics & Statics · asked 8× in 14 yrs · Read the full method →

Question

A particle of mass 2.52.5 kg hangs at the end of a string, 0.90.9 m long, the other end of which is attached to a fixed point. The particle is projected horizontally with a velocity 88 m/sec. Find the velocity of the particle and tension in the string when the string is (i) horizontal (ii) vertically upward.

Technique

Energy conservation for speed; radial Newton’s-second-law for tension (centripetal equation).

Solution

Setup. m=2.5m=2.5 kg, ℓ=0.9\ell=0.9 m, u=8u=8 m/s, g=9.8g=9.8 m/s². Let θ\theta be the angle the string makes with the downward vertical (so θ=0\theta=0 at start, θ=π/2\theta=\pi/2 horizontal, θ=π\theta=\pi vertically up).

Step 1 — Energy conservation to find speed at angle θ\theta

The particle rises by ℓ(1−cos⁡θ)\ell(1-\cos\theta) from the starting point. Conservation of energy:

12mv2+mgℓ(1−cos⁡θ)=12mu2  ⟹  v2=u2−2gℓ(1−cos⁡θ).\tfrac{1}{2}mv^{2}+mg\ell(1-\cos\theta)=\tfrac{1}{2}mu^{2}\;\Longrightarrow\;v^{2}=u^{2}-2g\ell(1-\cos\theta).

Step 2 — Centripetal equation

At angle θ\theta, the centripetal force toward the pivot is mv2/ℓmv^{2}/\ell, supplied by tension TT and the radial component of gravity. With “outward” defined as away from the pivot:

A clean unified form (taking inward as positive): T−mgcos⁡θ=mv2/ℓT-mg\cos\theta=mv^{2}/\ell for θ≤π/2\theta\le\pi/2. For θ>π/2\theta>\pi/2 (particle above pivot), gravity also points inward (downward, same direction as tension when string vertical-up), so T+mg∣cos⁡θ∣=mv2/ℓT+mg|\cos\theta|=mv^{2}/\ell.

For the two cases asked:

Step 3 — Case (i): String horizontal, θ=π/2\theta=\pi/2

1−cos⁡θ=11-\cos\theta=1:

v12=u2−2gℓ=64−2(9.8)(0.9)=64−17.64=46.36.v_1^{2}=u^{2}-2g\ell=64-2(9.8)(0.9)=64-17.64=46.36. v1=46.36≈6.81 m/s.v_1=\sqrt{46.36}\approx 6.81\text{ m/s}.

Gravity has no radial component at θ=π/2\theta=\pi/2:

T1=mv12ℓ=2.5×46.360.9=115.90.9≈128.78 N.T_1=\frac{mv_1^{2}}{\ell}=\frac{2.5\times 46.36}{0.9}=\frac{115.9}{0.9}\approx 128.78\text{ N}.

In symbolic form: T1=mu2/ℓ−2mg=(2.5)(64)/0.9−2(2.5)(9.8)=177.78−49=128.78T_1=mu^{2}/\ell-2mg=(2.5)(64)/0.9-2(2.5)(9.8)=177.78-49=128.78 N ✓.

Step 4 — Case (ii): String vertically upward, θ=π\theta=\pi

1−cos⁡θ=21-\cos\theta=2:

v22=u2−4gℓ=64−4(9.8)(0.9)=64−35.28=28.72.v_2^{2}=u^{2}-4g\ell=64-4(9.8)(0.9)=64-35.28=28.72. v2=28.72≈5.36 m/s.v_2=\sqrt{28.72}\approx 5.36\text{ m/s}.

(Sanity check: does the particle reach the top? Required v22≥gℓv_2^{2}\ge g\ell, i.e. 28.72≥8.8228.72\ge 8.82 ✓.)

At θ=π\theta=\pi, both tension (pulling down toward pivot) and gravity (also down) point inward toward pivot:

T2+mg=mv22ℓ  ⟹  T2=mv22ℓ−mg=2.5×28.720.9−2.5(9.8)=79.78−24.5≈55.28 N.T_2+mg=\frac{mv_2^{2}}{\ell}\;\Longrightarrow\;T_2=\frac{mv_2^{2}}{\ell}-mg=\frac{2.5\times 28.72}{0.9}-2.5(9.8)=79.78-24.5\approx 55.28\text{ N}.

In symbolic form: T2=mu2/ℓ−5mg=177.78−122.5=55.28T_2=mu^{2}/\ell-5mg=177.78-122.5=55.28 N ✓.

Summary

Answer

  (i) Horizontal: v1≈6.81 m/s,  T1≈128.78 N.(ii) Vertically up: v2≈5.36 m/s,  T2≈55.28 N.  \boxed{\;\begin{array}{l}\text{(i) Horizontal: }v_1\approx 6.81\text{ m/s},\;T_1\approx 128.78\text{ N}.\\[4pt]\text{(ii) Vertically up: }v_2\approx 5.36\text{ m/s},\;T_2\approx 55.28\text{ N}.\end{array}\;}
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