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Derive an expression for the speeds of two colliding bodies having one dimensional elastic collision.

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Let two bodies A and B of masses m1 and m2 are moving in a straight line with velocities u1 and u2 respectively (u1 > u2) After collision, let their velocities be changed to v1 and v2 respectively. (Fig above)

Total linear momentum of the system (bodies A & B) before collision = m1u1 + m2u2

Total linear momentum of the system (bodies A and B) after collision = m1v1 + m2v2

According to the law low of conservation of linear momentum,

m1u1 + m2u2 = m1v1 + m2v2   ...(i)

or, m1(u1 - u2) = m2(v2 - u2)    ....(ii)

As the collision is elastic, so the kinetic energy of the system also remains conserved:

i.e., 1/2 m1u12 + 1/2 m2u22 = 1/2 m1v12 + 1/2 m2v22   ....(iii)

m1(u12 - v12) = m2(v22 - u22)

or, m1(u12 - v12)(u1 - v1) = m2(v2 - u2)(v2 - u2)  ...(iv)

Dividing equation (iv) by equation (ii) we get

u1 + v1 = v2 + u2   ...(v)

or, u1 + u2 = v2 + v1   ...(vi)

or, Relative velocity of approach = Relative velocity of separation. That is, in an elastic one-dimensional collision, the relative velocity of approach before collision is equal to the relative velocity of separation after the collision.

The ratio of the relative velocity of separation to the relative velocity of approach is called coefficient of restitution (e), i.e.,

e = {v2 - v1}/{u1 - u2}   ...(vii)

The value of e depends upon the nature of materials of the colliding bodies.

For perfectly elastic collision, e = 1

Velocities after collision:

From equation (vi), v2 = u1 - u2 + v1   ...(viii)

Substituting the value of v2 in equation (ii), we have,

m1(u1 - v1) = m2[u1 - 2u2 + v1]

or, v1 = {2m2u2 + u1(m1 - m2)}/{(m1m2)}  ...(ix)

Substituting the value of v1 in equation (viii), we have,

v2 = {2m1u1 + u2(m2 - m1)}/{m1 + m2}    ...(x)

Special cases:

(1) When the two bodies have equal masses i.e., m1 = m2 = m (say).

From equation (ix), we get

and from equation (ix), we get

It follows from equation (xi) and (xii) that if two bodies of equal masses undergo one dimensional elastic collision, then their velocities are swapped after collision.

(2) When u2 = 0, i.e., body B is at rest

In such a situation, equation (ix) and (x) reduce to;

Three sub-cases arise:

(i) When m1 = m2, i.e., both bodies A and B have same mass.

Then from equations (xiii) and (xiv), we have v1 = 0 and v2 = u1

Thus, in an elastic collision in one dimension, when a body collides with another body at rest and of same mass, it is stopped and the other body begins to move with the velocity of the first.

(ii) When m1 > m2, i.e., body B is lighter than the body A. In such a situation, m2 can neglected as compared to m1

Thus, if a massive body collides with a lighter body at rest, there is practically no change in its velocity, whereas the stationary body begins to move with twice the velocity of the first.

(iii) When m1 << m2, i.e., body A is lighter than body B. In such a situation, m1 can be neglected as compared to m2

Thus, if a light body collides elastically with a heavy body at rest, it rebounds with its original velocity, whereas the heavy body practically remains at rest.

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