That is one example of using the change in total energy ΔE with the changes in two particular kinds of energy (kinetic and potential). But why stop there? Let's generalize this formula for energy conservation to keep track of all different kinds of energy that we might encounter, such as those listed at the beginning of the chapter:
| The different terms in the equation correspond to changes in kinetic, potential, radiant, nuclear, electrical, chemical, thermal, and pressure energy, respectively. When solving physics problems using the form of the law of conservation of energy in equation (3.7), many of the kinds of energy listed are unchanged—so you can set them to zero and drop them out of the equation.
As an example, if we want to talk about the conservation of energy for an electric circuit containing a battery and a lamp (that both lights up and radiates heat), we can use only those terms for changes in energy that are important for our closed system (electric, radiant, and thermal) and eliminate all the other changes of energy terms (because they are equal to zero):
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