Body A of mass 4m moving with speed u collides with another body B of mass 2m, at rest. The collision is head on and elastic in nature. After the collision the fraction of energy lost by the colliding body A is :
To solve the problem of determining the fraction of energy lost by body A after the collision, we need to apply concepts from elastic collision theory.
In an elastic collision, both momentum and kinetic energy are conserved.
Consider two bodies A and B. Initially, body A has mass 4m and velocity u, while body B has mass 2m and is at rest.
The initial momentum of the system is given by:
\( p_{\text{initial}} = (4m)u + (2m)(0) = 4mu \).
Let the final velocities of bodies A and B be v_1 and v_2 respectively.
The conservation of momentum gives us:
\( 4mu = 4mv_1 + 2mv_2 \)
Simplifying, we get:
\( 2u = 2v_1 + v_2 \) (Equation 1).
The conservation of kinetic energy gives us:
\( \frac{1}{2}(4m)u^2 = \frac{1}{2}(4m)v_1^2 + \frac{1}{2}(2m)v_2^2 \)
Simplifying, we get:
\( 2u^2 = 2v_1^2 + v_2^2 \) (Equation 2).
From Equations 1 and 2, we can solve for v_1 and v_2.
Solving these simultaneous equations, we find:
v_1 = \frac{u}{3} and v_2 = \frac{8u}{3}.
The initial kinetic energy of body A:
\( KE_{\text{initial}} = \frac{1}{2}(4m)u^2 = 2mu^2 \).
The final kinetic energy of body A:
\( KE_{\text{final}} = \frac{1}{2}(4m)\left(\frac{u}{3}\right)^2 = \frac{4m}{2} \cdot \frac{u^2}{9} = \frac{2mu^2}{9} \).
The energy lost by body A:
\( \Delta KE = KE_{\text{initial}} - KE_{\text{final}} = 2mu^2 - \frac{2mu^2}{9} = \frac{18mu^2}{9} - \frac{2mu^2}{9} = \frac{16mu^2}{9} \).
The fraction of the energy lost by body A is:
\( \frac{\Delta KE}{KE_{\text{initial}}} = \frac{\frac{16mu^2}{9}}{2mu^2} = \frac{16}{18} = \frac{8}{9} \).
Thus, the fraction of energy lost by the colliding body A is \(\frac{8}{9}\).