This problem describes a specific type of collision: a head-on elastic collision. Let's break down the initial conditions:
In an elastic collision, two fundamental conservation laws apply:
Our goal is to find the fraction of energy lost specifically by Body A after this collision.
Let $v_A$ be the final velocity of Body A and $v_B$ be the final velocity of Body B after the collision.
1. Conservation of Momentum:
Initial momentum = Final momentum
$m \cdot u + (3m) \cdot 0 = m \cdot v_A + (3m) \cdot v_B$Simplifying this equation by dividing by $m$ (since $m \neq 0$):
$u = v_A + 3v_B \quad \quad (1)$2. Relative Velocity in Elastic Collisions:
For a head-on elastic collision, the relative speed of approach is equal to the relative speed of separation.
$u_{approach} = u_A - u_B = u - 0 = u$ $u_{separation} = v_B - v_A$Equating them:
$u = v_B - v_A \quad \quad (2)$Now we have a system of two linear equations (1) and (2) with two unknowns ($v_A$ and $v_B$). Let's solve them:
So, after the collision, Body A moves with velocity $v_A = -u/2$ (meaning it reverses direction) and Body B moves with velocity $v_B = u/2$.
We need to find the energy lost by Body A. First, let's calculate its initial and final kinetic energy ($KE$).
Initial Kinetic Energy of Body A ($KE_{A, initial}$):
$KE_{A, initial} = \frac{1}{2} m u^2$Final Kinetic Energy of Body A ($KE_{A, final}$):
Using the final velocity $v_A = -u/2$:
$KE_{A, final} = \frac{1}{2} m (v_A)^2 = \frac{1}{2} m \left(-\frac{u}{2}\right)^2$ $KE_{A, final} = \frac{1}{2} m \left(\frac{u^2}{4}\right) = \frac{1}{8} m u^2$Energy Lost by Body A:
Energy lost is the difference between initial and final kinetic energy:
$\Delta KE_A = KE_{A, initial} - KE_{A, final}$ $\Delta KE_A = \frac{1}{2} m u^2 - \frac{1}{8} m u^2$To subtract, find a common denominator (which is 8):
$\Delta KE_A = \left(\frac{4}{8} - \frac{1}{8}\right) m u^2$ $\Delta KE_A = \frac{3}{8} m u^2$The question asks for the fraction of energy lost by Body A. This is calculated by dividing the energy lost by Body A by its initial kinetic energy.
$ \text{Fraction Lost} = \frac{\Delta KE_A}{KE_{A, initial}} $ $ \text{Fraction Lost} = \frac{\frac{3}{8} m u^2}{\frac{1}{2} m u^2} $The terms $m u^2$ cancel out:
$ \text{Fraction Lost} = \frac{3/8}{1/2} $Dividing by a fraction is the same as multiplying by its reciprocal:
$ \text{Fraction Lost} = \frac{3}{8} \times \frac{2}{1} = \frac{6}{8} $Simplifying the fraction:
$ \text{Fraction Lost} = \frac{3}{4} $Therefore, the fraction of kinetic energy lost by colliding body A after the head-on elastic collision is $3/4$. This matches option 2.
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