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Notes on Relativity and Cosmology - Physics Department, UCSB

Notes on Relativity and Cosmology - Physics Department, UCSB

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6.4. MORE ON MASS, ENERGY, AND MOMENTUM 153<br />

6.4 More <strong>on</strong> Mass, Energy, <strong>and</strong> Momentum<br />

In the last secti<strong>on</strong> we saw that what we used to call mass <strong>and</strong> energy can be<br />

c<strong>on</strong>verted into each other – <strong>and</strong> in fact are c<strong>on</strong>verted into each other all of the<br />

time. Does this mean that mass <strong>and</strong> energy really are the same thing? Well,<br />

that depends <strong>on</strong> exactly how <strong>on</strong>e defines mass <strong>and</strong> energy.... the point is that,<br />

as with most things in physics, the old (Newt<strong>on</strong>ian) noti<strong>on</strong>s of mass <strong>and</strong> energy<br />

will no l<strong>on</strong>ger be appropriate. So, we must extend both the old c<strong>on</strong>cept of<br />

mass <strong>and</strong> the old c<strong>on</strong>cept of energy before we can even start talking. There are<br />

various ways to extend these c<strong>on</strong>cepts. I’m going to use a more modern choice<br />

which is st<strong>and</strong>ard in the technical literature. Unfortunately, this modern choice<br />

seems to be less comm<strong>on</strong> in the popular literature <strong>and</strong> may therefore seem to<br />

c<strong>on</strong>tradict things you have read elsewhere.<br />

6.4.1 Energy <strong>and</strong> Rest Mass<br />

My noti<strong>on</strong> of mass will be independent of reference frame. This is not the case<br />

for an older c<strong>on</strong>venti<strong>on</strong> which has a closer tie to the old F = ma. This older<br />

c<strong>on</strong>venti<strong>on</strong> then defines a mass that changes with velocity. However, for the<br />

moment, let me skirt around this issue by talking about the “rest mass” (m 0 ,<br />

by definiti<strong>on</strong> an invariant) of an object, which is just the mass (inertia) it has<br />

when it is at rest 8 . In particular, an object at rest has inertia m 0 c 2 .<br />

Recall that, in Newt<strong>on</strong>ian physics, an object also has an energy 1 2 m 0v 2 due to its<br />

moti<strong>on</strong>. Almost certainly, this expressi<strong>on</strong> will need to be modified in relativity,<br />

but it should be approximately correct for velocities small compared with the<br />

speed of light. Thus, for a slowly moving object we have<br />

E = m 0 c 2 + 1 2 m 0v 2 + small correcti<strong>on</strong>s. (6.5)<br />

Note that we can factor out an m 0 c 2 to write this as:<br />

E = m 0 c 2 (1 + 1 2<br />

v 2<br />

+ small correcti<strong>on</strong>s). (6.6)<br />

c2 In secti<strong>on</strong> 6.6 we will derive the precise form of these small correcti<strong>on</strong>s. However,<br />

this derivati<strong>on</strong> is somewhat technical <strong>and</strong> relies <strong>on</strong> a more in-depth knowledge of<br />

energy <strong>and</strong> momentum in Newt<strong>on</strong>ian physics than some of you will have. Since<br />

I do not want it to obscure the main points of our discussi<strong>on</strong>, I have relegated<br />

the derivati<strong>on</strong> to a separate secti<strong>on</strong> (6.6) at the end of the chapter. For the<br />

moment, we will c<strong>on</strong>tent ourselves with a well-motivated guess.<br />

8 I suspect that the linguistic evoluti<strong>on</strong> is as follows: People first used the old c<strong>on</strong>venti<strong>on</strong><br />

where mass meant inertia. They then introduced this separate noti<strong>on</strong> of ‘rest mass.’ As time<br />

passed, physicists found that the <strong>on</strong>ly time they ever used the word mass was in the phrase<br />

‘rest mass,’ as the other c<strong>on</strong>cept was in fact better served by the term energy (which, as we<br />

have seen, carried inertia). After awhile, they got tired of inserting the word ‘rest’ <strong>and</strong> writing<br />

the subscript 0.

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