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Let a uniform rod of mass M and length 2l lie on a smooth horizontal surface.a particle of mass m, moving with velocity v1,strikes at one end of rod,perpendicularly with a coeff.of restitution of e,Finf 1. angular velocity of rod about centre 2. linear velocity about centre of mass 3. final velocity

rajat agarwal , 16 Years ago
Grade 11
anser 1 Answers
Askiitians Tutor Team

To analyze the situation where a particle strikes a uniform rod, we need to consider the principles of conservation of momentum and the effects of the coefficient of restitution. Let's break this down step by step to find the angular velocity of the rod about its center, the linear velocity of the center of mass, and the final velocity of the particle after the collision.

Initial Setup

We have a uniform rod of mass M and length 2l resting on a smooth horizontal surface. A particle of mass m strikes one end of the rod perpendicularly with an initial velocity v1. The coefficient of restitution, e, describes how elastic the collision is, affecting the velocities after the impact.

1. Angular Velocity of the Rod about its Center

When the particle strikes the rod, it exerts a force that causes the rod to rotate about its center of mass. To find the angular velocity (ω) of the rod after the collision, we first need to determine the impulse imparted to the rod.

  • The initial momentum of the particle before the collision is given by: p_initial = mv1.
  • After the collision, the particle will have a new velocity, which we will denote as v2.
  • Using the coefficient of restitution, we can express the relationship between the velocities before and after the collision: e = (v2 - ω(2l/2)) / (v1 - 0).

Here, (2l/2) is the distance from the center of the rod to the point of impact. Rearranging this gives us:

v2 = v1 - e * v1 + ωl.

Next, we apply the conservation of angular momentum about the center of mass of the rod:

m * v1 * l = I * ω + m * v2 * l,

where I is the moment of inertia of the rod about its center, which is I = (1/12) * M * (2l)^2 = (1/3) * Ml^2.

Substituting I into the equation gives us:

m * v1 * l = (1/3) * Ml^2 * ω + m * v2 * l.

2. Linear Velocity of the Center of Mass

The linear velocity of the center of mass (V_cm) of the rod can be found using the conservation of linear momentum:

m * v1 = (M + m) * V_cm.

From this, we can solve for V_cm:

V_cm = (m * v1) / (M + m).

3. Final Velocity of the Particle

To find the final velocity of the particle (v2), we can substitute our expression for V_cm back into the equation derived from the coefficient of restitution:

v2 = v1(1 - e) + V_cm.

Substituting V_cm into this equation gives:

v2 = v1(1 - e) + (m * v1) / (M + m).

Summary of Results

After performing these calculations, we can summarize our findings:

  • The angular velocity of the rod about its center is determined by the relationship between the initial momentum of the particle and the moment of inertia of the rod.
  • The linear velocity of the center of mass of the rod is influenced by the masses involved and the initial velocity of the particle.
  • The final velocity of the particle after the collision is affected by both the coefficient of restitution and the conservation of momentum.

This systematic approach allows us to understand the dynamics of the collision and the resulting motion of both the rod and the particle. If you have any further questions or need clarification on any of the steps, feel free to ask!

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