Condition for Non-Overtaking Collision of Two Balls

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Kinematics Advanced linear motion

Source: Physics Competition - Mechanics

Problem Sets:

Kinematics set 1

Problem

Two identical small balls, A and B, both with mass $m$, are initially at rest. Ball A is a distance $a$ behind ball B. At the same instant, ball A is given an impulse $I$ and ball B is subjected to a constant force $F$. Both the impulse and the force are directed along the line connecting A to B.

Determine the condition for which ball A will not overtake ball B.

The condition for which ball A will not overtake ball B is:

$$I^2 \le 2mFa$$

[Q1] Determine the condition for which ball A will not overtake ball B.

Let the initial position of ball A be $x_A(0) = 0$ and ball B be $x_B(0) = a$.

  1. Equations of Motion

    • Ball A: At $t=0$, it receives an impulse $I$. From the impulse-momentum theorem, its initial (and constant) velocity is $v_A = I/m$. The position of ball A at time $t$ is: $$x_A(t) = v_A t = \frac{I}{m} t$$
    • Ball B: At $t=0$, it is subjected to a constant force $F$. Its constant acceleration is $a_B = F/m$. Starting from rest, its position at time $t$ is: $$x_B(t) = x_B(0) + v_{B,0} t + \frac{1}{2} a_B t^2 = a + \frac{1}{2} \frac{F}{m} t^2$$
  2. Condition for Non-Overtaking For ball A not to overtake ball B, its position must always be less than or equal to ball B's position for all times $t \ge 0$.

    $$x_A(t) \le x_B(t)$$

    The limiting case is when A "just touches" B. At this specific instant, say $t_c$, both balls are at the same position and must have the same velocity. If A's velocity were greater at that point, it would overtake B.

  3. Derivation of the Critical Condition First, we find the time $t_c$ when their velocities are equal. The velocity of ball A is constant: $v_A(t) = I/m$. The velocity of ball B is: $v_B(t) = a_B t = (F/m)t$. Setting $v_A(t_c) = v_B(t_c)$:

    $$\frac{I}{m} = \frac{F}{m} t_c \implies t_c = \frac{I}{F}$$

    Next, for the "just touching" condition, we require their positions to be equal at this time $t_c$.

    $$x_A(t_c) = x_B(t_c)$$ $$\frac{I}{m} t_c = a + \frac{1}{2} \frac{F}{m} t_c^2$$

    Substitute the expression for $t_c$:

    $$\frac{I}{m} \left(\frac{I}{F}\right) = a + \frac{1}{2} \frac{F}{m} \left(\frac{I}{F}\right)^2$$ $$\frac{I^2}{mF} = a + \frac{1}{2} \frac{F}{m} \frac{I^2}{F^2}$$ $$\frac{I^2}{mF} = a + \frac{I^2}{2mF}$$

    Solving for $a$:

    $$a = \frac{I^2}{mF} - \frac{I^2}{2mF} = \frac{I^2}{2mF}$$

    This gives the critical relation:

    $$I^2 = 2mFa$$

    This equation defines the boundary condition. For A not to overtake B, its initial impulse must be less than or equal to this critical value. A larger impulse would cause A to reach B while still traveling faster, thus overtaking it.

Therefore, the condition for non-overtaking is $I^2 \le 2mFa$.