JEE Challenger
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Angle at Which Bob Speed is Half Initial Velocity in Vertical Circular Motion

A bob of mass M is suspended by a massless string of length L. The horizontal velocity V at position A is just sufficient to make it reach the point B. The angle θ\theta at which the speed of the bob is half of that at A, satisfies

Diagram 0

Options

A

θ=π4\theta = \frac{\pi}{4}

B

π4<θ<π2\frac{\pi}{4} < \theta < \frac{\pi}{2}

C

π2<θ<3π4\frac{\pi}{2} < \theta < \frac{3\pi}{4}

D

3π4<θ<π\frac{3\pi}{4} < \theta < \pi

Correct

Step-by-Step Solution

To find the angle θ\theta at which the speed of the bob is half of its initial speed at AA, we analyze the motion using the principle of conservation of mechanical energy.

Step 1: Determine the velocity at AA

For the bob suspended by a string to just reach the top point BB of the vertical circular path, the tension in the string at point BB must be zero (TB=0T_B = 0).

At point BB, gravity provides the required centripetal acceleration:
MvB2L=Mg  ⟹  vB2=gL\frac{M v_B^2}{L} = M g \implies v_B^2 = gL

Using the conservation of mechanical energy between the lowest point AA (taken as the reference level for potential energy, UA=0U_A = 0) and the highest point BB (at a height 2L2L above AA):
12MV2=12MvB2+Mg(2L)\frac{1}{2} M V^2 = \frac{1}{2} M v_B^2 + Mg(2L)
V2=vB2+4gL=gL+4gL=5gLV^2 = v_B^2 + 4gL = gL + 4gL = 5gL
V=5gLV = \sqrt{5gL}


Step 2: Relate speed vv at angle θ\theta to the initial speed VV

Let θ\theta be the angle made by the string with the downward vertical line passing through AA. The height hh of the bob above point AA at angle θ\theta is:
h=L(1−cos⁡θ)h = L(1 - \cos\theta)

Applying the conservation of mechanical energy between point AA and the point at angle θ\theta:
12MV2=12Mv2+MgL(1−cos⁡θ)\frac{1}{2} M V^2 = \frac{1}{2} M v^2 + M g L (1 - \cos\theta)
v2=V2−2gL(1−cos⁡θ)v^2 = V^2 - 2gL(1 - \cos\theta)

Substituting V2=5gLV^2 = 5gL:
v2=5gL−2gL(1−cos⁡θ)=gL(3+2cos⁡θ)v^2 = 5gL - 2gL(1 - \cos\theta) = gL(3 + 2\cos\theta)


Step 3: Find θ\theta when v=V2v = \frac{V}{2}

Given that the speed of the bob is half of its velocity at AA, v=V2v = \frac{V}{2}:
v2=(V2)2=V24=5gL4v^2 = \left(\frac{V}{2}\right)^2 = \frac{V^2}{4} = \frac{5gL}{4}

Equating this to the energy expression for v2v^2:
gL(3+2cos⁡θ)=5gL4gL(3 + 2\cos\theta) = \frac{5gL}{4}
3+2cos⁡θ=543 + 2\cos\theta = \frac{5}{4}
2cos⁡θ=54−3=−742\cos\theta = \frac{5}{4} - 3 = -\frac{7}{4}
cos⁡θ=−78=−0.875\cos\theta = -\frac{7}{8} = -0.875


Step 4: Determine the interval for θ\theta

We know the standard values of cosine in the second quadrant:
cos⁡(3π4)=−12≈−0.707\cos\left(\frac{3\pi}{4}\right) = -\frac{1}{\sqrt{2}} \approx -0.707
cos⁡(π)=−1\cos(\pi) = -1

Since −1<−0.875<−0.707-1 < -0.875 < -0.707, it follows that:
cos⁡(π)<cos⁡θ<cos⁡(3π4)\cos(\pi) < \cos\theta < \cos\left(\frac{3\pi}{4}\right)

Since cos⁡θ\cos\theta is a strictly decreasing function in the range [0,π][0, \pi], reversing the inequalities gives:
3π4<θ<π\frac{3\pi}{4} < \theta < \pi

Thus, the correct option is D.