Book cover for Classical Mechanics

Classical Mechanics

John R. Taylor

ISBN #9781891389221

1st Edition

744 Questions

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Summary

Learning Objectives

Key Concepts

Example Problems

Explanations

Common Mistakes

Summary

This chapter focuses on the conservation of energy, highlighting its complexity compared to linear and angular momentum conservation due to the many forms in which energy can exist. It emphasizes the significance of understanding energy transformations and introduces new vector calculus tools like the gradient and curl. A key takeaway is that while energy is always conserved, the processes involved in its transformation require careful analysis and the application of advanced mathematical concepts.

Learning Objectives

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Key Concepts

CONCEPT

DEFINITION

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Example Problems

Example 1

By writing a $\cdot \mathbf{b}$ in terms of components prove that the product rule for differentiation applies to the dot product of two vectors; that is, $\frac{d}{d t}(\mathbf{a} \cdot \mathbf{b})=\frac{d \mathbf{a}}{d t} \cdot \mathbf{b}+\mathbf{a} \cdot \frac{d \mathbf{b}}{d t}$.

Example 2

Evaluate the work done $W=\int_{O}^{P} \mathbf{F} \cdot d \mathbf{r}=\int_{O}^{P}\left(F_{x} d x+F_{y} d y\right)$ by the two-dimensional force $\mathbf{F}=\left(x^{2}, 2 x y\right)$ along the three paths joining the origin to the point $P=(1,1)$ as shown in Figure $4.24(\mathrm{a})$ and defined as follows: (a) This path goes along the $x$ axis to $Q=(1,0)$ and then straight up to $P .$ (Divide the integral into two pieces, $\int_{O}^{P}=\int_{O}^{Q}+\int_{Q}^{P}) .$ (b) On this path $y=x^{2},$ and you can replace the term $d y$ in (4.100) by $d y=2 x d x$ and convert the whole integral into an integral over $x$. (c) This path is given parametrically as $x=t^{3}, y=t^{2} .$ In this case rewrite $x, y, d x,$ and $d y$ in (4.100) in terms of $t$ and $d t,$ and convert the integral into an integral over $t$.

Example 3

Do the same as in Problem $4.2,$ but for the force $\mathbf{F}=(-y, x)$ and for the three paths joining $P$ and $Q$ shown in Figure $4.24(\mathrm{b})$ and defined as follows: (a) This path goes straight from $P=(1,0)$ to the origin and then straight to $Q=(0,1) .$ (b) This is a straight line from $P$ to $Q$. (Write $y$ as a function of $x$ and rewrite the integral as an integral over $x$.) (c) This is a quarter-circle centered on the origin. (Write $x$ and $y$ in polar coordinates and rewrite the integral as an integral over $\phi .$ )

Example 4

A particle of mass $m$ is moving on a frictionless horizontal table and is attached to a massless string, whose other end passes through a hole in the table, where I am holding it. Initially the particle is moving in a circle of radius $r_{\mathrm{o}}$ with angular velocity $\omega_{\mathrm{o}},$ but $\mathrm{I}$ now pull the string down through the hole until a length $r$ remains between the hole and the particle. (a) What is the particle's angular velocity now? (b) Assuming that I pull the string so slowly that we can approximate the particle's path by a (a) (b)

Example 5

(a) Consider a mass $m$ in a uniform gravitational field $\mathbf{g},$ so that the force on $m$ is $m \mathbf{g},$ where $\mathbf{g}$ is a constant vector pointing vertically down. If the mass moves by an arbitrary path from point 1 to point $2,$ show that the work done by gravity is $W_{\mathrm{grav}}(1 \rightarrow 2)=-m g h$ where $h$ is the vertical height gained between points 1 and 2. Use this result to prove that the force of gravity is conservative (at least in a region small enough so that $\mathrm{g}$ can be considered constant). (b) Show that, if we choose axes with $y$ measured vertically up, the gravitational potential energy is $U=m g y$ (if we choose $U=0$ at the origin).

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