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Question: A uniform rod AB of length $l$ can slide between the floor and the wall as shown in the figure. If t...

A uniform rod AB of length ll can slide between the floor and the wall as shown in the figure. If the end A is moving with uniform velocity vAv_A away from the wall, find the:

A

velocity of the end B.

B

angular velocity of the rod.

C

velocity of the mass center.

D

distance from end A of the point on the rod that has the minimum speed.

Answer

a, d

Explanation

Solution

  1. Coordinate System and Kinematic Relations: Set up a coordinate system with the origin at the wall-floor corner. Let end A be at (x,0)(x,0) and end B at (0,y)(0,y). The rod length ll implies x2+y2=l2x^2 + y^2 = l^2. Also, from trigonometry, x=lcosθx = l \cos\theta and y=lsinθy = l \sin\theta. Given dxdt=vA\frac{dx}{dt} = v_A.

  2. Velocity of End B: Differentiate x2+y2=l2x^2 + y^2 = l^2 with respect to time to get 2xdxdt+2ydydt=02x\frac{dx}{dt} + 2y\frac{dy}{dt} = 0. Substitute dxdt=vA\frac{dx}{dt} = v_A and dydt=vB\frac{dy}{dt} = v_B. Solve for vBv_B and substitute x=lcosθx = l \cos\theta, y=lsinθy = l \sin\theta to get vB=vAcotθv_B = -v_A \cot\theta. Magnitude is vAcotθv_A \cot\theta.

  3. Angular Velocity: Differentiate x=lcosθx = l \cos\theta with respect to time to get dxdt=lsinθdθdt\frac{dx}{dt} = -l \sin\theta \frac{d\theta}{dt}. Substitute dxdt=vA\frac{dx}{dt} = v_A and dθdt=ω\frac{d\theta}{dt} = \omega. Solve for ω\omega to get ω=vAlsinθ\omega = -\frac{v_A}{l \sin\theta}. Magnitude is vAlsinθ\frac{v_A}{l \sin\theta}.

  4. Velocity of Mass Center: The mass center is at the midpoint (x/2,y/2)(x/2, y/2). Differentiate these coordinates to find vGx=vA2v_{Gx} = \frac{v_A}{2} and vGy=vB2=vAcotθ2v_{Gy} = \frac{v_B}{2} = -\frac{v_A \cot\theta}{2}. The magnitude vCM=vGx2+vGy2=vA2sinθv_{CM} = \sqrt{v_{Gx}^2 + v_{Gy}^2} = \frac{v_A}{2\sin\theta}.

  5. Point of Minimum Speed: Let P be a point at distance rr from A. Use the section formula to find its coordinates: Px=(lr)xlP_x = \frac{(l-r)x}{l} and Py=rylP_y = \frac{ry}{l}. Differentiate these to find vPxv_{Px} and vPyv_{Py}. Calculate vP2=vPx2+vPy2v_P^2 = v_{Px}^2 + v_{Py}^2. Minimize vP2v_P^2 by differentiating with respect to rr and setting the derivative to zero. This yields r=lsin2θr = l \sin^2\theta.