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A ball of mass A moving with velocity V, collides with another B of the same mass at rest. If the coefficient of restriction between the balls is e, the ratio of final and initial velocity of A is

Physics

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Answer

1−e2\frac{1-e}{2}

12\frac{1}{2}

Step-by-step solution

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Here are the solutions to the collision problems.

:
A ball of mass A moving with velocity V, collides with another B of the same mass at rest. If the coefficient of restriction between the balls is e, the ratio of final and initial velocity of A is

  • Given:

    • Mass of ball A: mA=mm_A = m
    • Initial velocity of ball A: VA=VV_A = V
    • Mass of ball B: mB=mm_B = m (same mass as A)
    • Initial velocity of ball B: VB=0V_B = 0 (at rest)
    • Coefficient of restitution: ee
  • To find: The ratio VA′VA\frac{V_A'}{V_A}

  1. Apply the principle of conservation of momentum.

    mAVA+mBVB=mAVA′+mBVB′m_A V_A + m_B V_B = m_A V_A' + m_B V_B'

    Substitute the given values:

    mV+m(0)=mVA′+mVB′m V + m (0) = m V_A' + m V_B' mV=m(VA′+VB′)m V = m (V_A' + V_B') V=VA′+VB′(Equation 1)V = V_A' + V_B' \quad \text{(Equation 1)}
  2. Apply the definition of the coefficient of restitution.

    e=−VB′−VA′VB−VAe = -\frac{V_B' - V_A'}{V_B - V_A}

    Substitute the given values:

    e=−VB′−VA′0−Ve = -\frac{V_B' - V_A'}{0 - V} e=VB′−VA′Ve = \frac{V_B' - V_A'}{V} eV=VB′−VA′(Equation 2)e V = V_B' - V_A' \quad \text{(Equation 2)}
  3. Solve the system of equations for VA′V_A'.

    We have:

    1. VA′+VB′=VV_A' + V_B' = V
    2. −VA′+VB′=eV-V_A' + V_B' = e V

    Subtract Equation 2 from Equation 1:

    (VA′+VB′)−(−VA′+VB′)=V−eV(V_A' + V_B') - (-V_A' + V_B') = V - e V 2VA′=V(1−e)2 V_A' = V(1 - e) VA′=V(1−e)2V_A' = \frac{V(1 - e)}{2}
  4. Calculate the ratio VA′VA\frac{V_A'}{V_A}.

    VA′VA=V(1−e)2V\frac{V_A'}{V_A} = \frac{\frac{V(1 - e)}{2}}{V} VA′VA=1−e2\frac{V_A'}{V_A} = \frac{1 - e}{2}

    The ratio of final and initial velocity of A is 1−e2\boxed{\frac{1-e}{2}}.


    :
    A block of mass m moving with a speed v collides with another object of mass 2m at rest. The lighter block comes to rest after the collision. The coefficient of restitution is

    • Given:

      • Mass of lighter block (A): mA=mm_A = m
      • Initial speed of lighter block (A): VA=vV_A = v
      • Mass of heavier block (B): mB=2mm_B = 2m
      • Initial speed of heavier block (B): VB=0V_B = 0 (at rest)
      • Final speed of lighter block (A): VA′=0V_A' = 0 (comes to rest)
    • To find: The coefficient of restitution, ee

  5. Apply the principle of conservation of momentum.

    mAVA+mBVB=mAVA′+mBVB′m_A V_A + m_B V_B = m_A V_A' + m_B V_B'

    Substitute the given values:

    m(v)+(2m)(0)=m(0)+(2m)VB′m(v) + (2m)(0) = m(0) + (2m)V_B' mv=2mVB′mv = 2m V_B' VB′=mv2mV_B' = \frac{mv}{2m} VB′=v2V_B' = \frac{v}{2}
  6. Apply the definition of the coefficient of restitution.

    e=−VB′−VA′VB−VAe = -\frac{V_B' - V_A'}{V_B - V_A}

    Substitute the known values:

    e=−v2−00−ve = -\frac{\frac{v}{2} - 0}{0 - v} e=−v2−ve = -\frac{\frac{v}{2}}{-v} e=v2ve = \frac{\frac{v}{2}}{v} e=12e = \frac{1}{2}

    The coefficient of restitution is 12\boxed{\frac{1}{2}}.

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