\(\def \u#1{\,\mathrm{#1}}\) \(\def \abs#1{\left|#1\right|}\) \(\def \ast{*}\) \(\def \deg{^{\circ}}\) \(\def \ten#1{\times 10^{#1}}\) \(\def \redcancel#1{{\color{red}\cancel{#1}}}\) \(\def \BLUE#1{{\color{blue} #1}}\) \(\def \RED#1{{\color{red} #1}}\) \(\def \PURPLE#1{{\color{purple} #1}}\) \(\def \th#1,#2{#1,\!#2}\) \(\def \lshift#1#2{\underset{\Leftarrow\atop{#2}}#1}}\) \(\def \rshift#1#2{\underset{\Rightarrow\atop{#2}}#1}}\) \(\def \dotspot{{\color{lightgray}{\circ}}}\)
Chapter 6: Energy
2.

Work

Energy can be transferred from one object to another through two mechanisms. One method is heat, which is when energy flows from a hotter object to a colder object. We’ll talk about that in Heat.

The other mechanism is work, which is the exchange of energy by means of a force. When you give energy to an object, such as when you make a box go faster, then you are doing positive work on the object. Negative work is when you steal energy from an object, such as when you slow down a runaway shopping cart. Work is reciprocal, so if you do positive work on a box (by running into it, for example), the box does negative work on you (by slowing you down); thus it's important to specify which object is receiving the work (the target) and which object is the source of the work.

Work
\(W\)
J

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Work can be calculated using the formula

$$W=Fd\cos\theta$$

where

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Consider the three forces on the car in this picture; the car is moving to the right.

Because work is the only change in energy we will study in this chapter, we can write energy conservation as

$$E_f=E_i+W$$