Black Holes — From Dark Stars to Ringing Spacetime
The Physics Principle
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Black Holes — From Dark Stars to Ringing Spacetime
88 просмотров · 12 дн. назад
The Physics Principle
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88 просмотров · 12 дн. назад
Black Holes — from dark stars to ringing spacetime
Throw a ball up and it comes back. Throw it fast enough and it never does. What if even light could not escape? This video follows that question from John Michell’s “dark stars” of 1783, through Einstein, Schwarzschild, Chandrasekhar and Oppenheimer, to the first black-hole images, the first gravitational-wave chirp, Hawking radiation, and what astronomers are finding today.
The moving physics is computed, not hand-drawn: a ray-traced black hole (exact light paths in Schwarzschild spacetime), the exact redshift of a falling probe, a numerical solution of the Regge–Wheeler wave equation for the ringdown, and the acoustic wave equation for a sonic horizon. Each sound comes from the same numbers as its picture.
CHAPTERS
0:00 The everyday puzzle
1:00 Dark stars (1783)
2:00 Einstein and Schwarzschild (1915)
3:19 Gravity slows time
4:17 The absurd star (1930s)
5:16 Collapse (1939)
5:53 The event horizon
7:28 Quasars and Cygnus X-1
8:27 What a black hole looks like
9:18 Weighing the black hole at the center of the Milky Way
10:20 Hearing black holes merge
11:22 The ringdown
12:20 Not so black
13:13 A black hole for sound
13:48 Black holes today
15:17 References
NOTES
The GW150914 sound is a model waveform (3.5 post-Newtonian inspiral joined to the ringdown of the final 62-solar-mass Kerr black hole), not detector data.
The falling-probe demo uses a 12,000-solar-mass black hole so the fade lasts a few seconds.
The ringdown simulation reproduces the known l = 2 quasinormal frequency to better than 1% (ωGM/c³ ≈ 0.373 − 0.088i vs 0.3737 − 0.0890i).
The EHT-style rings, the “black hole star” and the LISA sketch are illustrations, not data.
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