Interactive three-dimensional simulations & visualizations

Visualizing the beauty in physics and mathematics


Project maintained by zhendrikse Hosted on GitHub Pages — Theme by mattgraham

Rendering a black hole using ray tracing


Image rendition explained


Black hole explained
Black hole picture explained (nasa.gov)

Real images of black holes


For comparison, below are some real images of black holes, showing a bright ring formed as light bends in the intense gravity around a black hole.

Sagittarius A*          
On May 12, 2022, the Event Horizon Telescope managed to reveal Sagittarius A*, the supermassive black hole at the center of our Milky Way.
Black hole M87          
Another supermassive black hole, at the center of the galaxy M87, that is 6.5 billion times more massive than the sun, taken by the same Event Horizon Telescope.

Einstein and Oppenheimer
Size comparison for supermassive black holes such as TON 618, see also this fantastic video.

A concise history


Black holes are an outcome of the Einstein field equations (EFE):

$R_{\mu\nu} -\frac{1}{2}R G_{\mu\nu} + \lambda g_{\mu\nu} = k T_{\mu\nu}$

The expression on the left represents the curvature of spacetime as determined by the metric; the expression on the right represents the stress–energy–momentum content of spacetime. The EFE can then be interpreted as a set of equations dictating how stress–energy–momentum determines the curvature of spacetime.

[…]

The equations are more complex than they appear. Given a specified distribution of matter and energy in the form of a stress–energy tensor, the EFE are understood to be equations for the metric tensor $g_{\mu\nu}$, since both the Ricci tensor and scalar curvature depend on the metric in a complicated nonlinear manner. When fully written out, the EFE are a system of ten coupled, nonlinear, hyperbolic-elliptic partial differential equations. — Wikipedia


This led John Archibald Wheeler, the “hero of the black hole story” according to Steven Hawking and the first to coin the term black hole, to state that

Spacetime tells matter how to move; matter tells spacetime how to curve.


Back in 1915, Karl Schwarzschild was the first to actually derive an exact solution to these equations, which is quite an achievement, even more so when you consider that he accomplished this feat while he was serving in the German army during World War I. He left clues in his work, clues that are now known as the Schwarzschild radius and the existence of singularities.

Around the same time, Einstein was theorizing about the existence of what we now call black holes, when he tried to prove that celestial objects that are so dense that their gravity prevents even light from escaping, could not exist.

But in 1939, physicists J. Robert Oppenheimer (about whom the famous movie was made) and Hartland Snyder published a paper called “On Continued Gravitational Contraction”, which provided a solution to the EFE based on the Schwarzschild metric, which describes the collapse of an extremely massive object into a black hole.

Einstein and Oppenheimer
Einstein did, in fact, tell Oppenheimer to give up his security clearance and walk away from government work. The scene in the movie Oppenheimer is based on true events.


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