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Two small spheres A and B of equal radiu...

Two small spheres `A` and `B` of equal radius but different masses of `3m` and `2m` are moving towards each other and impinge directly. The speeds of `A` and `B` before collision are, respectively, `4u` and `u`. The collision is such that `B` experiences an impulse of magnitude `6mcu`, where `c` is a constant. Determine
a. the coefficient of restitution,
b. the limits for the value of `c` for which such collision is possible.

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To solve the problem step by step, we will analyze the situation involving two spheres A and B, and derive the required results. ### Step 1: Define the given parameters - Mass of sphere A, \( m_A = 3m \) - Mass of sphere B, \( m_B = 2m \) - Initial velocity of sphere A, \( u_A = 4u \) (moving towards B) - Initial velocity of sphere B, \( u_B = -u \) (moving towards A) - Impulse experienced by B, \( J = 6mcu \) ### Step 2: Apply the conservation of linear momentum Using the conservation of momentum before and after the collision, we can write: \[ m_A u_A + m_B u_B = m_A v_A + m_B v_B \] Substituting the known values: \[ 3m(4u) + 2m(-u) = 3m v_A + 2m v_B \] This simplifies to: \[ 12m u - 2m u = 3m v_A + 2m v_B \] \[ 10m u = 3m v_A + 2m v_B \] Dividing through by \( m \): \[ 10u = 3v_A + 2v_B \quad \text{(Equation 1)} \] ### Step 3: Apply the impulse-momentum theorem for sphere B According to the impulse-momentum theorem: \[ J = \Delta p_B \] Where \( \Delta p_B \) is the change in momentum of sphere B: \[ 6mcu = m_B v_B - m_B u_B \] Substituting the values: \[ 6mcu = 2m v_B - 2m(-u) \] This simplifies to: \[ 6cu = 2v_B + 2u \] Dividing through by \( 2 \): \[ 3cu = v_B + u \] Rearranging gives: \[ v_B = 3cu - u \quad \text{(Equation 2)} \] ### Step 4: Substitute Equation 2 into Equation 1 Now we substitute \( v_B \) from Equation 2 into Equation 1: \[ 10u = 3v_A + 2(3cu - u) \] Expanding this: \[ 10u = 3v_A + 6cu - 2u \] Combining like terms: \[ 10u + 2u = 3v_A + 6cu \] \[ 12u = 3v_A + 6cu \] Solving for \( v_A \): \[ 3v_A = 12u - 6cu \] \[ v_A = 4u - 2cu \quad \text{(Equation 3)} \] ### Step 5: Calculate the coefficient of restitution The coefficient of restitution \( e \) is defined as: \[ e = \frac{v_B - v_A}{u_A - u_B} \] Substituting the values: \[ e = \frac{(3cu - u) - (4u - 2cu)}{4u - (-u)} \] This simplifies to: \[ e = \frac{3cu - u - 4u + 2cu}{4u + u} \] \[ e = \frac{5cu - 5u}{5u} \] \[ e = c - 1 \] ### Step 6: Determine the limits for the value of \( c \) Since the coefficient of restitution \( e \) must lie between 0 and 1: \[ 0 \leq c - 1 \leq 1 \] This implies: \[ 1 \leq c \leq 2 \] ### Final Answers a. The coefficient of restitution \( e = c - 1 \). b. The limits for the value of \( c \) are \( 1 \leq c \leq 2 \).

To solve the problem step by step, we will analyze the situation involving two spheres A and B, and derive the required results. ### Step 1: Define the given parameters - Mass of sphere A, \( m_A = 3m \) - Mass of sphere B, \( m_B = 2m \) - Initial velocity of sphere A, \( u_A = 4u \) (moving towards B) - Initial velocity of sphere B, \( u_B = -u \) (moving towards A) - Impulse experienced by B, \( J = 6mcu \) ...
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