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Notes on Relativity and Cosmology - Physics Department, UCSB

Notes on Relativity and Cosmology - Physics Department, UCSB

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9.3. BEYOND THE HORIZON 247<br />

<strong>and</strong> the past interior should be much like the future interior. This part of the<br />

spacetime is often called a ‘white hole’ as there is no way that any object can<br />

remain inside: everything must pass outward into <strong>on</strong>e of the exterior regi<strong>on</strong>s<br />

through <strong>on</strong>e of the horiz<strong>on</strong>s!<br />

r = R s<br />

r = 0<br />

r = R s<br />

r < R s<br />

r > R s<br />

r < R s<br />

r > R s<br />

r = R s<br />

r = 0<br />

r = R s<br />

As we menti<strong>on</strong>ed briefly with regard to the sec<strong>on</strong>d exterior, the past interior<br />

does not really exist for the comm<strong>on</strong> black holes found in nature. Let’s talk<br />

about how this works. So far, we have been studying the pure Schwarzschild<br />

soluti<strong>on</strong>. As we have discussed, it is <strong>on</strong>ly a valid soluti<strong>on</strong> in the regi<strong>on</strong> in which<br />

no matter is present. Of course, a little bit of matter will not change the picture<br />

much. However, if the matter is an important part of the story (for example,<br />

if it is matter that causes the black hole to form in the first place), then the<br />

modificati<strong>on</strong>s will be more important.<br />

Let us notice that in fact the ‘hole’ (whether white or black) in the above spacetime<br />

diagram has existed since infinitely far in the past. If the Schwarzschild<br />

soluti<strong>on</strong> is to be used exactly, the hole (including the wormhole) must have been<br />

created at the beginning of the universe. We expect that most black holes were<br />

not created with the beginning of the universe, but instead formed later when<br />

too much matter came too close together. Recall that a black hole must form<br />

when, for example, too much thin gas gets clumped together.<br />

Once the gas gets into a small enough regi<strong>on</strong> (smaller than its Schwarzschild<br />

radius), we have seen that a horiz<strong>on</strong> forms <strong>and</strong> the gas must shrink to a smaller<br />

size. No finite force (<strong>and</strong>, in some sense, not even infinite force) can prevent the<br />

gas from shrinking. Now, outside of the gas, the Schwarzschild soluti<strong>on</strong> should<br />

be valid. So, let me draw a worldline <strong>on</strong> our Schwarzschild spacetime diagram<br />

that represents the outside edge of the ball of gas. This breaks the diagram into<br />

two pieces: an outside that correctly describes physics outside the gas, <strong>and</strong> an<br />

inside that has no direct physical relevance <strong>and</strong> must be replaced by something<br />

that depends <strong>on</strong> the details of the matter:

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