Rad Relativity — 2026
A deep dive into the physics of black holes, from Einstein's relativity to rotating Kerr geometry.
He judges you
A black hole is a region of spacetime where gravity is so overwhelming that nothing — not even light — can escape once it crosses the boundary known as the event horizon.
They are not empty voids. They contain enormous amounts of mass compressed into an incredibly small space, bending spacetime so severely that our ordinary physics breaks down at the centre.
Predicted by Einstein's general theory of relativity in 1916 and first directly photographed in 2019, black holes remain one of the most actively studied objects in all of astrophysics.
Figure 2 — An artist's depiction of a black hole
Rad Relativity Relativity
A completely reliable and accurate description of Einstein's Theory of Relativity.
The Theory of Relativity is one of the most important ideas in modern physics, developed by Albert Einstein in the early 20th century. It explains how space, time, and gravity work — especially when objects move very fast or when gravity is extremely strong.
Einstein's theory explains that space and time are connected through spacetime, that time is relative depending on motion and gravity, and that mass and energy are related. Both special and general relativity have been tested many times. Relativity is not theoretical.
Disclaimer: All of this is simplified for easier reading and understanding, and is as accurate as possible in this form. — The Author
Covers space and time for objects at constant speeds. No gravity involved.
Extends special relativity to include gravity. Mass curves spacetime.
Special relativity (1905) describes how space and time work for objects moving at constant speeds — no gravity involved. It rests on two postulates:
Imagine you are on a sealed train — no windows, no gaps — travelling at a constant speed. You do not know you are moving. You roll a ball on the floor. It drops to the ground and rolls exactly as it would on solid ground.
From inside, you have no way of knowing how fast the train is moving. Physics behaves identically at any constant speed. The laws of physics are the same in all inertial frames.
This means two observers moving at different constant speeds will each measure the same speed of light — not different values, as classical physics would predict. Einstein's insight was that this forces space and time to be flexible instead.
Length contraction happens when something is moving — but it is only significant at speeds approaching the speed of light. Because space and time are interconnected and the speed of light is constant, the relativity of simultaneity means that light from one end of a moving object reaches an observer at a different time than light from the other end. If you measure the distance between the ends using those arrival times, you get a shorter value. This is the observed length contraction.
$$L = L_0\sqrt{1 - \frac{v^2}{c^2}} = \frac{L_0}{\gamma}$$Mass and energy are two forms of the same thing. A tiny bit of mass equals an enormous amount of energy. And because $c$ is the cosmic speed limit, nothing with mass can ever reach it.
Imagine a ruler and two observers: one standing still, the other moving to the right. A football is thrown to the left. Both measure its speed using their own ruler and clock. The stationary observer measures 50 m/s; the moving observer measures 150 m/s. In classical (Newtonian) physics, both are valid — motion is always relative, and each observer considers themselves "at rest."
Logically then, a stationary observer should measure light at $c$, and a moving observer at $c + 50$ m/s. But Einstein said this is wrong. The speed of light in a vacuum is always the same, regardless of the observer's motion.
To explore the consequences, imagine a light clock — a beam of light bouncing between two mirrors. Seen from inside a moving train and from a stationary observer on the ground, the same clock behaves differently.
For the rider, the photon travels straight up and down. For the ground observer, because the clock moves sideways, the photon follows a longer diagonal path — while still moving at exactly the speed of light.
As a result, the ground observer concludes that less time has passed on the moving clock. A moving clock runs more slowly. This is time dilation.
In the ground frame, the resting clock's light travels straight between mirrors at distance $d$. The time between ticks is the proper time, $\Delta t_0$, where $d = c(\Delta t_0/2)$. This distance is perpendicular to the motion, so $d$ is the same in every reference frame.
For the moving clock, the photon traces a diagonal path of length $S = c(\Delta t/2)$, while the clock moves sideways $L = v(\Delta t/2)$. The lengths $d$, $L$, and $S$ form a right triangle. Applying the Pythagorean theorem and solving:
$$\Delta t = \gamma\,\Delta t_0 \qquad \gamma = \frac{1}{\sqrt{1 - v^2/c^2}}$$The moving clock's tick interval $\Delta t$ is longer than the proper time $\Delta t_0$ — the moving clock runs slow. The Lorentz factor $\gamma$ is always $\geq 1$.
Proper time is the time measured by a clock present at both events in the same location — essentially the time in the frame where the clock is at rest. It is always the shortest possible elapsed time between those events.
Muons are created when cosmic rays — high-energy particles from space — strike nuclei in the upper atmosphere. At rest, a muon's average lifetime is about 2.2 microseconds; far too short to travel the ~18 km to sea level before decaying.
Logically, muons should never reach the ground. Yet many are observed at sea level, confirmed by experiments on Mount Washington. Using the time dilation formula, their lifetime as seen from Earth can be about ten times longer than their proper lifetime — enough to travel several kilometres and reach the sensors.
The twin paradox: one twin stays on Earth while the other travels at high speed to a distant star and returns. From Earth's frame, the traveling twin's clock runs slow — the traveler returns younger.
From the traveler's view, Earth seems to move, so Earth's clocks appear slow too. Paradox?
The resolution: the traveling twin changes inertial frames at the turnaround — they experience acceleration. The Earth-bound twin does not. When the traveler switches frames, Earth's time coordinate "jumps" forward in the new frame. Over the whole journey, this frame-switching creates a larger total elapsed time for Earth. When they reunite, the traveling twin is much younger.
1915 — Extends special relativity to include gravity. Instead of thinking of gravity as a force pulling objects, mass and energy curve spacetime, and objects move along the curves.
Imagine a single spherically symmetrical object — non-rotating and electrically neutral — alone in an empty universe. Release a ring of stationary particles around it (far away). The particles gradually speed up towards the object until they reach it.
Release more and more streams until you have a uniform flow all accelerating toward the object. Now, instead of particles, think of it as spacetime itself flowing like a river into the object, carrying anything in its path. That is how gravity actually works.
Free fall — like an orbiting planet or a dropped object — is actually the object moving along the "straightest possible path" (a geodesic) in curved spacetime. There is no force pulling it. The path itself is curved by nearby mass.
Every object is already moving through time. Spacetime warping converts that temporal motion into spatial motion — pulling things toward massive objects.
We cannot create a perfectly correct visual for general relativity for one key reason: it includes a fourth dimension. Instead of a spatial dimension, Einstein's theory includes time as the fourth dimension. We can make useful 3D approximations — but they are always approximations.
The sheet visualisation: imagine a perfectly flat, infinitely stretchy sheet with a grid network. Place a large steel ball and a small ping pong ball on it. The steel ball creates a large curve; the ping pong ball rolls toward it, picking up speed.
Now roll the ping pong ball in from the side — it spirals briefly and hits the steel ball. The sheet is spacetime. The steel ball is a planet. The falling ping pong ball is an object under gravity; rolled from the side, it is an orbiting object.
If you shoot the ping pong ball from a massive distance with enormous speed, it whizzes past without orbiting. Control that energy and it enters a stable orbit that decays much more slowly.
A more accurate visualisation uses a full 3D grid or net representing spacetime, pulled and contracted toward the central object — better showing the "river" effect. The full 4D version (including time) cannot yet be perfectly visualised. The most popular 4D approximation is a cube inside a cube with connected vertices.
To look at gravitational time dilation, we look at the Schwarzschild Solution — the spacetime geometry around a single, spherical, non-rotating, uncharged mass. We do not need a big new equation; the time dilation factor is already inside it.
$$ds^2 = -\!\left(1 - \frac{2GM}{c^2 r}\right)c^2\,dt^2 + \left(1 - \frac{2GM}{c^2 r}\right)^{-1}dr^2 + r^2\,d\Omega^2$$The highlighted term $\left(1 - \frac{2GM}{c^2 r}\right)$ appears in the metric's time component. Take its square root to get the gravitational time dilation factor:
$$\text{Grav. TD Factor} = \sqrt{1 - \frac{2GM}{c^2 r}}$$Compare the two time dilation factors side by side:
$$\text{Velocity TD:} \quad \sqrt{1 - \frac{v^2}{c^2}}$$ $$\text{Gravity TD:} \quad \sqrt{1 - \frac{2GM}{c^2 r}}$$Both share the form $\sqrt{1 - (\,\cdot\,)/c^2}$. Equating the inner terms gives:
$$\frac{2GM}{r} = v^2$$This shows that gravitational time dilation and velocity-based time dilation are the same phenomenon, and gives an equation to substitute between them.
Because the speed of light is always constant, time moves more slowly for you to compensate — so the speed of light remains constant from your perspective too. This is why time dilation exists.
Because of this, there is no single "true" time — it is all relative. Some claim the "true" time is measured in a space without any influence from gravity or velocity. This obviously cannot happen in our ever-expanding universe, because everything is under some form of gravitational influence.
Time is relative. Clocks lie. Gravity bends everything — including the passage of time itself. — ME
Rad Relativity History
The history of general relativity
In 1905, Einstein published the special theory of relativity, a theory that would change the world. At the time, it was highly controversial because it contradicted Newtonian laws, and many people thought that was impossible. People were right; almost no one would use this theory at the time. But Einstein, knowing that his theory was correct, realised that Newtonian gravity couldn't be true because it would violate special relativity, so it had to be revised. He concluded that instead of acting immediately, gravitational waves must propagate through space at the speed of light. Einstein used Maxwell's equations of electromagnetism together with mechanics to ensure that Newtonian gravity obeyed the same principle. Einstein performed thought experiments to figure out how gravity actually works. He noticed that he could not derive the solution from his current theory. So he had to work on a completely new theory, one that is more refined and in-depth than the current theory.
Fig. H1 — Einstein's 1905 annus mirabilis papers.
One day, he realises that according to Newtonian gravity, a body in free fall doesn't feel its own weight. Einstein realised that the two things that needed to be equal for this to happen were not a coincidence. He imagined an observer in a sealed box accelerating at a constant rate, realising that there would be no way for the observer to determine if they were in the presence of a large gravitational field or accelerating through outer space. This would be true because they would feel a force pushing them towards the bottom of the box just as gravity would. Einstein called this the equivalence principle. The gravitational force the observer feels is just an authentic homogeneous gravitational field, and the only way for the observer to determine that they are in an authentic gravitational field is to stop accelerating or change the rate of acceleration, and see if they feel anything change. This principle states that physics behaves the same way in all frames of reference in which an observer is accelerating at one constant rate.
Fig. H2 — The equivalence of gravity and acceleration.
Soon after Einstein realised this, Hermann Minkowski coincidentally developed a four-dimensional formulation of special relativity in which space and time were intertwined. Einstein used this spacetime to develop his theory. Einstein had realised the possibility that a mass would curve the spacetime around it, causing objects to follow a 'straight' path in that curved geometry, causing it to move towards the mass. So, Einstein started doing thought experiments in outer space. He imagined a photon travelling in a stationary rocket from one end to the other, and it travelled straight. Then he applied a constant acceleration of 9.8 m/s² and then shot the photon. Einstein realised that the photon would move very slightly downwards from the perspective of someone inside the ship. Then, using the equivalence principle, he concluded that the photon would move the same distance on Earth as well. He concluded that this happened due to the light travelling in a 'straight' path along a curved spacetime. This led him to conclude that masses pull on spacetime, which causes objects travelling through the spacetime to curve towards the masses.
Fig. H3 — Minkowski diagram.
Now all Einstein needed to do was find the correct geometry for this theory and make mathematical equations. When Einstein moved to Zurich, he found that the correct geometry for his new theory was Riemannian geometry, since it applies to curved surfaces rather than to flat ones. To use this, he would have to write his equations to describe motion on curved surfaces. In order to come up with new equations for curved spacetime, he asked Grossmann to help him with the complicated mathematics and said that he would deal with the physics himself. They spent three years working relentlessly until they finished it. This new theory replaced Newton's gravity, and he called it the general theory of relativity.
Fig. H4 — Eienstiens notes.
Even though Einstein had the formulas derived and his theory done, he still couldn't find an exact solution to his equations. But the papers Einstein wrote managed to travel to the war zone during World War I, where they reached Karl Schwarzschild. Schwarzschild was delighted to take a break from the war, and he said, in his note to Einstein, "The war treated me kind enough, despite the heavy gunfire, to allow me to get away from it all and take this walk in the land of your ideas." He worked on Einstein's equations by hyper-simplifying the universe to where there is only one mass in the universe, one that is electrically neutral and spherically symmetric. In a matter of weeks, he developed the formula to solve for any curve in spacetime, given that you know the mass and distance to the object; this was the Schwarzschild solution. This solution consequently created the Schwarzschild radius, or the radius an object must be compressed to for it to become a black hole.
"The war treated me kind enough, despite the heavy gunfire, to allow me to get away from it all and take this walk in the land of your ideas." — Karl Schwarzschild, letter to Einstein, 1916
Fig. H5 — Karl Schwarzschild, who solved Einstein's equations from the front.
After Einstein received the letter from Schwarzschild, he was delighted with the findings, but after the solution was released to the general public, two flaws in his solution were uncovered. When r = rs (when the radius is the Schwarzschild radius), or when r = 0, the escape velocity shoots up to infinity. These points are two very important parts of a black hole: the famous event horizon and the singularity. The main issue here was the event horizon — the event horizon is the point where time stops flowing forward, but inward, the line where time stops. But Einstein thought such a thing could never exist, others thought it went against the laws of "Nature," and there would be a thing stopping that from happening. So began the great research of disproving and proving black holes.
Fig. H6 — Don't know what to put here so here is a sea cucumber.
Now Pauli's exclusion principle states that no two fermions, such as electrons, can occupy the same space. What does this mean? Well, since Heisenberg's Uncertainty Principle states that you cannot know both a particle's momentum and position with absolute certainty, and as each electron gets constrained in space, its uncertainty in momentum would have to increase, therefore causing it to vibrate and wiggle around faster and faster. Because the white dwarf was becoming so condensed, the atoms were vibrating so much that they prevented the star from collapsing any further. This is known as the Chandrasekhar limit, equivalent to about 1.44 solar masses.
Fig. H7 — Electron degeneracy pressure holding up a white dwarf.
Now, as the world breathed a sigh of relief, a scientist by the name Subrahmanyan Chandrasekhar was going to prove that statement wrong. He was an Indian astrophysicist, only 19 years old, and while travelling on a British ship in 1930, he found out that a star can collapse past the white dwarf and pass the Chandrasekhar limit. People discovered that when a huge star passes the Chandrasekhar limit, the atoms cannot vibrate faster than light, and they can not hold the star up, and it collapses further. This causes the protons and electrons to fuse, forming neutrons and neutrinos through neutronization, and collapse into a neutron star. However, there is a limit to neutron stars to prevent them from collapsing as well. The Tolman-Oppenheimer-Volkoff or TOV Limit is approximately 2.17 solar masses.
If the star is past the TOV limit, there is nothing to keep it from collapsing, and it folds inwards on itself. At this point, the radius is below the Schwarzschild radius, and it has become a black hole.
Fig. H8 — Stellar collapse: white dwarf → neutron star → black hole.