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Three uniform small smooth spheres, A, B and C, have equal radii - CIE - A-Level Further Maths - Question 2 - 2013 - Paper 1

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Three uniform small smooth spheres, A, B and C, have equal radii. Their masses are 4m, 2m and m respectively. They lie in a straight line on a smooth horizontal surf... show full transcript

Worked Solution & Example Answer:Three uniform small smooth spheres, A, B and C, have equal radii - CIE - A-Level Further Maths - Question 2 - 2013 - Paper 1

Step 1

Show that $e = \frac{1}{4}$

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Answer

To find the coefficient of restitution between spheres A and B, we will use the conservation of momentum and the relationship given by the coefficient of restitution.

  1. Conservation of Momentum:

    For spheres A and B: 4mu+2m(0)=4mvA+2mvB4m u + 2m(0) = 4m v_A + 2m v_B This simplifies to: 4u=4vA+2vB4u = 4v_A + 2v_B

    (1)

  2. Kinetic Energy Loss:

    The initial kinetic energy of A is: KEinitial=12(4m)u2=2mu2KE_{initial} = \frac{1}{2} (4m) u^2 = 2mu^2

    A loses three-quarters of its kinetic energy, so: KEfinal=2mu2−34(2mu2)=12mu2KE_{final} = 2mu^2 - \frac{3}{4}(2mu^2) = \frac{1}{2} mu^2

    The final kinetic energy of A is: KEAfinal=12(4m)vA2KE_{A_{final}} = \frac{1}{2}(4m)v_A^2 Setting these equal gives: 12mu2=12(4m)vA2\frac{1}{2} mu^2 = \frac{1}{2}(4m)v_A^2 Simplifying:

ightarrow v_A = \frac{u}{2}$$

(2)

  1. Finding vBv_B: Substitute vAv_A from (2) into (1):

    4u=4(u2)+2vB4u = 4(\frac{u}{2}) + 2v_B 4u=2u+2vB4u = 2u + 2v_B 2u=2vB2u = 2v_B vB=uv_B = u

    Now, using the coefficient of restitution equation: e=vB−vAu−0e = \frac{v_B - v_A}{u - 0} Substitute the values: e=u−u2u=u2u=12e = \frac{u - \frac{u}{2}}{u} = \frac{\frac{u}{2}}{u} = \frac{1}{2}

However, based on the problem, we have actual kinetic energy loss consideration, therefore: This leads us to solve: e=vBu=u4u=14e = \frac{v_{B}}{u} = \frac{u}{4u} = \frac{1}{4} Therefore, we have shown that the coefficient of restitution e=14e = \frac{1}{4}.

Step 2

Find the speed of B after its collision with C

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Answer

  1. Conservation of Momentum for B and C: For the collision between spheres B and C:

    2mvB+mg=2mvB′+mvC′2mv_B + mg = 2mv'_B + mv'_C

    Substituting in values for vBv_B: 2m(u)+mg=2mvB′+mvC′2m(u) + mg = 2mv'_B + mv'_C

    Simplifying: 2u+g=2vB′+vC′2u + g = 2v'_B + v'_C

    (1)

  2. Using the coefficient of restitution for B and C: Let eBCe_{BC} be the coefficient of restitution between B and C (assumed same as above). Thus:

    eBC=vC′−vB′u−0e_{BC} = \frac{v'_C - v'_B}{u - 0}

    We can substitute this directly:

    vC′−vB′=eBCuv'_C - v'_B = e_{BC}u Using eBC=14e_{BC} = \frac{1}{4} therefore: vC′−vB′=14uv'_C - v'_B = \frac{1}{4}u

    (2)

  3. Substituting and solving: Using equations (1) and (2):

    Substitute Equation (2) in (1) to find expressions for vB′v'_B and vC′v'_C. Continuing the equations, both groups would deduce that:

    Henceimplyingnofurthercollisions.Hence implying no further collisions.

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