Gas falling toward a black hole rarely falls straight in — leftover angular momentum flattens it into a spinning accretion disk. Friction between neighboring rings orbiting at different speeds (viscous heating) converts orbital energy into heat, and that heat is radiated away as light whose color depends on local temperature. This simulation reproduces that process with real inverse-square gravity and the classical Shakura-Sunyaev disk temperature law.
F ∝ M / r² and drift slowly inward due to viscous torque, exactly like real accreting gas.T(r) ∝ (Rin/r)^0.75 · √(1 − √(Rin/r)), the Shakura-Sunyaev profile, running from dull red (cool, outer disk) through orange-yellow to blue-white (hot, inner disk).A black hole itself emits no light — every photon associated with an "image" of a black hole, including the Event Horizon Telescope's pictures of M87* and Sagittarius A*, actually comes from glowing gas in the accretion disk (or jets) outside the event horizon.
Thousands of particles orbit a black hole under real inverse-square gravity and spiral inward through viscous drag, colored live by the Shakura-Sunyaev temperature law — from dull red at the outer edge to blue-white near the innermost stable orbit.
Orbital speed, viscous heating, and the innermost stable circular orbit (ISCO) combine to set an accretion disk's temperature — and therefore color — as a function of radius, plus the plunge that happens once matter crosses the ISCO.
Adjust black hole mass, accretion rate, and spin to see the disk's inner edge, peak temperature, and color balance respond. Toggle Doppler beaming to see the approaching side of the disk brighten.
A black hole itself emits no light — every "image" of a black hole, including the Event Horizon Telescope's pictures, actually shows glowing gas in its accretion disk, not the hole.