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JEE Advanced 2017 · System of Particles and Rotational Motion

A rigid uniform bar ABAB of length LL is slipping from its vertical position on a frictionless floor (as shown in the figure). At some instant of time, the angle made by the bar with the vertical is θ\theta. Which of the following statements about its motion is/are correct?

Answers: A. The midpoint of the bar will fall vertically downward · C. Instantaneous torque about the point in contact with the floor is proportional to sin⁡θ\sin\theta · D. When the bar makes an angle θ\theta with the vertical, the displacement of its midpoint from the initial position is proportional to (1−cos⁡θ)(1 - \cos\theta)

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Written solution

Step 1: Analyze the forces acting on the bar.

The forces acting on the uniform bar ABAB of mass mm and length LL are the gravitational force mgmg acting vertically downwards at the midpoint, and the normal force NN acting vertically upwards at the contact point BB.

Since the floor is frictionless, there are no horizontal forces.

Fx=0F_x = 0

Step 2: Analyze the motion of the midpoint.

Since there is no horizontal force, the horizontal position of the center of mass (midpoint) remains constant.

xCM=0x_{\text{CM}} = 0

Thus, the midpoint falls vertically downward. This confirms statement (1) is correct.

Step 3: Determine the trajectory of point AA.

Let the vertical line of fall of the midpoint be the y-axis, so xCM=0x_{\text{CM}} = 0.

The coordinates of point AA at any angle θ\theta with the vertical are given by:

xA=−L2sin⁡θx_A = -\frac{L}{2}\sin\theta yA=Lcos⁡θy_A = L\cos\theta

Eliminating θ\theta yields the equation of the trajectory:

(xAL/2)2+(yAL)2=1\left(\frac{x_A}{L/2}\right)^2 + \left(\frac{y_A}{L}\right)^2 = 1

This is the equation of an ellipse, not a parabola. This confirms statement (2) is incorrect.

Step 4: Calculate the torque about the contact point BB.

The torque about the contact point BB is due solely to the gravitational force acting at the midpoint.

τB=mg(L2sin⁡θ)\tau_B = mg \left(\frac{L}{2}\sin\theta\right) τB∝sin⁡θ\tau_B \propto \sin\theta

This confirms statement (3) is correct.

Step 5: Calculate the displacement of the midpoint.

The initial height of the midpoint is L2\frac{L}{2}, and its height at angle θ\theta is L2cos⁡θ\frac{L}{2}\cos\theta.

The vertical displacement ΔyCM\Delta y_{\text{CM}} is:

ΔyCM=L2−L2cos⁡θ\Delta y_{\text{CM}} = \frac{L}{2} - \frac{L}{2}\cos\theta ΔyCM=L2(1−cos⁡θ)\Delta y_{\text{CM}} = \frac{L}{2}(1 - \cos\theta) ΔyCM∝(1−cos⁡θ)\Delta y_{\text{CM}} \propto (1 - \cos\theta)

This confirms statement (4) is correct.

Answer: Statements (1), (3), and (4) are correct.

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