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Ratio of String Lengths for Vertical Circular Motion Collision

Consider a bob of mass mm, suspended by a string of length l1l_1, which is imparted a minimum velocity required to complete a full circle in the vertical plane. At its highest point, it undergoes an elastic collision with another bob of mass mm suspended by a string of length l2l_2, which is initially at rest. Both strings are massless and inextensible. If the second bob, following the collision, acquires the minimum speed required to complete a full circle in the vertical plane, the ratio l1l2\frac{l_1}{l_2} is

Official Numerical Answer5

Step-by-Step Solution

To find the ratio l1l2\frac{l_1}{l_2}, we analyze the motion of the two bobs step-by-step:

  1. Motion of the First Bob: A bob of mass mm suspended by a string of length l1l_1 is given the minimum speed at the lowest point required to complete a full vertical circle: vlowest=5gl1v_{\text{lowest}} = \sqrt{5gl_1}

    Using conservation of mechanical energy between the lowest point and the highest point: 12mvlowest2=12mvtop2+mg(2l1)\frac{1}{2}m v_{\text{lowest}}^2 = \frac{1}{2}m v_{\text{top}}^2 + mg(2l_1) 12m(5gl1)=12mvtop2+2mgl1\frac{1}{2}m (5gl_1) = \frac{1}{2}m v_{\text{top}}^2 + 2mgl_1 vtop=gl1v_{\text{top}} = \sqrt{gl_1}

    Thus, the speed of the first bob at its highest point, just before the collision, is: u1=gl1u_1 = \sqrt{gl_1}

  2. Collision Between the Bobs: The second bob of mass mm is initially at rest hanging vertically from a string of length l2l_2, meaning it is located at the lowest point of its own path: u2=0u_2 = 0

    Since the collision is head-on and perfectly elastic between two bodies of equal mass (m1=m2=mm_1 = m_2 = m), they exchange their velocities: v1′=u2=0v_1' = u_2 = 0 v2′=u1=gl1v_2' = u_1 = \sqrt{gl_1}

    Therefore, immediately after the collision, the second bob acquires a horizontal speed of: v2′=gl1v_2' = \sqrt{gl_1}

  3. Motion of the Second Bob: For the second bob to complete a full circle in the vertical plane from its lowest point, the minimum initial speed required is: vmin=5gl2v_{\text{min}} = \sqrt{5gl_2}

    According to the problem, the speed acquired by the second bob after the collision equals this minimum speed: v2′=5gl2v_2' = \sqrt{5gl_2}

    Equating the two expressions for the speed: gl1=5gl2\sqrt{gl_1} = \sqrt{5gl_2}

    Squaring both sides: gl1=5gl2gl_1 = 5gl_2

    l1l2=5\frac{l_1}{l_2} = 5