Book cover for Classical Mechanics

Classical Mechanics

John R. Taylor

ISBN #9781891389221

1st Edition

744 Questions

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Example Problems

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Summary

Angular momentum is a fundamental physical quantity defined as the cross product of a particle's position vector and its momentum. For systems of particles, the total angular momentum is the sum of individual angular momenta. When internal forces are central, they do not contribute net torque, leading to the important result that the time rate of change of angular momentum is equal to the net external torque. This principle is pivotal in the analysis of rotational dynamics in both natural phenomena and engineered systems.

Learning Objectives

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Key Concepts

CONCEPT

DEFINITION

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Example Problems

Example 1

Consider a gun of mass $M$ (when unloaded) that fires a shell of mass $m$ with muzzle speed $v$. (That is, the shell's speed relative to the gun is $v$.) Assuming that the gun is completely free to recoil (no external forces on gun or shell), use conservation of momentum to show that the shell's speed relative to the ground is $v /(1+m / M).$

Example 2

A shell traveling with speed $v_{\mathrm{o}}$ exactly horizontally and due north explodes into two equal-mass fragments. It is observed that just after the explosion one fragment is traveling vertically up with speed $v_{\mathrm{o}} .$ What is the velocity of the other fragment?

Example 3

A shell traveling with velocity $\mathbf{v}_{\mathrm{o}}$ explodes into three pieces of equal masses. Just after the explosion, one piece has velocity $\mathbf{v}_{1}=\mathbf{v}_{\mathrm{o}}$ and the other two have velocities $\mathbf{v}_{2}$ and $\mathbf{v}_{3}$ that are equal in magnitude $\left(v_{2}=v_{3}\right)$ but mutually perpendicular. Find $\mathbf{v}_{2}$ and $\mathbf{v}_{3}$ and sketch the three velocities.

Example 4

Two hobos, each of mass $m_{\mathrm{h}}$, are standing at one end of a stationary railroad flatcar with frictionless wheels and mass $m_{\mathrm{fc}} .$ Either hobo can run to the other end of the flatcar and jump off with the same speed $u$ (relative to the car). (a) Use conservation of momentum to find the speed of the recoiling car if the two men run and jump simultaneously. (b) What is it if the second man starts running only after the first has already jumped? Which procedure gives the greater speed to the car? [Hint: The speed $u$ is the speed of either hobo, relative to the car just after he has jumped; it has the same value for either man and is the same in parts (a) and (b).]

Example 5

Many applications of conservation of momentum involve conservation of energy as well, and we haven't yet begun our discussion of energy. Nevertheless, you know enough about energy from your introductory physics course to handle some problems of this type. Here is one elegant example: An elastic collision between two bodies is defined as a collision in which the total kinetic energy of the two bodies after the collision is the same as that before. (A familiar example is the collision between two billiard balls, which generally lose extremely little of their total kinetic energy.) Consider an elastic collision between two equal mass bodies, one of which is initially at rest. Let their velocities be $\mathbf{v}_{1}$ and $\mathbf{v}_{2}=0$ before the collision, and $\mathbf{v}_{1}^{\prime}$ and $\mathbf{v}_{2}^{\prime}$ after. Write down the vector equation representing conservation of momentum and the scalar equation which expresses that the collision is elastic. Use these to prove that the angle between $\mathbf{v}_{1}^{\prime}$ and $\mathbf{v}_{2}^{\prime}$ is $90^{\circ} .$ This result was important in the history of atomic and nuclear physics: That two bodies emerged from a collision traveling on perpendicular paths was strongly suggestive that they had equal mass and had undergone an elastic collision.

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