Rad Relativity — 2026

BLACK
HOLES

A deep dive into the physics of black holes, from Einstein's relativity to rotating Kerr geometry.

Est. black holes 10⁸
First photographed 2019
Largest known TON 618
Escape velocity c
The half scottish Roan Connor
The fishy fishy Avish Panthee
he looks at you

He judges you

Introduction

WHAT IS A
BLACK HOLE?

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.

  • Governed entirely by Einstein's general theory of relativity
  • Detected via gravitational waves, X-ray emissions, and light bending
  • First photographed by the Event Horizon Telescope in 2019
  • Predicted to slowly evaporate over cosmic timescales via Hawking radiation
absolute Cinima

Figure 2 — An artist's depiction of a black hole

Rad Relativity Relativity

EINSTEIN
BROKE PHYSICS
AND BROKE IT A FEW
MORE TIMES
AND THEN HE EXPLAINED IT

A completely reliable and accurate description of Einstein's Theory of Relativity.

Overview

SPACE, TIME, A LITTLE SALT
AND THE AUDACITY
OF ALBERT EINSTEIN

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
01 1905

SPECIAL
RELATIVITY

Covers space and time for objects at constant speeds. No gravity involved.

02 1915

GENERAL
RELATIVITY

Extends special relativity to include gravity. Mass curves spacetime.

Effects from Special Relativity
  • Time dilation — moving clocks run slower
  • Length contraction — fast-moving objects appear shorter
  • Nothing can go faster than light
  • $E = mc^2$ — mass and energy are one thing
Act One

SPECIAL
RELATIVITY

The First Postulate Inertial Frames

YOU'RE ALREADY
MOVING —
YOU JUST DON'T
KNOW IT

Special relativity (1905) describes how space and time work for objects moving at constant speeds — no gravity involved. It rests on two postulates:

  • The laws of physics are the same for all inertial frames (non-accelerating).
  • The speed of light in a vacuum is always $c \approx 3.0 \times 10^8$ m/s — no matter how fast the observer is moving.
Speed of light$c \approx 3.0 \times 10^8 \text{ m/s}$
Same for all observers?Yes. Always.
Can you exceed it?No (theoretically impossible)
Thought Experiment

THE SEALED TRAIN

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.

Special Relativity — Effect 01 ✦ cue the game show music ✦

OBJECTS LIE
ABOUT THEIR SIZE

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.

$$L = L_0\sqrt{1 - \frac{v^2}{c^2}} = \frac{L_0}{\gamma}$$
Eq. 1Length Contraction Formula
$L_0$ — Proper LengthLength in the object's own rest frame
$L$ — Contracted LengthShorter length seen by a moving observer
$v$ — VelocitySpeed of the object relative to observer
$c$ — Speed of LightUniversal speed limit ($\approx3\times10^8$ m/s)
$\gamma$ — Lorentz Factor$\gamma = 1\,/\,\sqrt{1 - v^2/c^2}$
Also from Special Relativity

MASS IS JUST
LAZY ENERGY

$$E = mc^2$$
Eq. 2Mass–Energy Equivalence

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.

Special Relativity — Effect 04 The Big One

CLOCKS ARE
LIARS TOO

THE BALL EXPERIMENT

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.

THE LIGHT CLOCK

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.

a diagram of a light clock
The Maths

THE WORLD'S MOST
INCONVENIENT WATCH

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:

$$\Delta t = \gamma\,\Delta t_0 \qquad \gamma = \frac{1}{\sqrt{1 - v^2/c^2}}$$
Eq. 3Time Dilation Formula

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 — Defined

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.

$\Delta t_0$ — Proper TimeShorter time, in the moving clock's own frame
$\Delta t$ — Dilated TimeLonger time measured by ground observer
$\gamma$ — Lorentz Factor$\gamma \geq 1$ always
At $v = 0$$\gamma = 1$, clocks agree
As $v \to c$$\gamma \to \infty$, moving clock stops
Living Proof

THIS IS REAL AND
IT HAPPENS CONSTANTLY

Example 01

THE IMMORTAL MUON

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.

Example 02

THE VERY YOUNG SIBLING

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.

Part Two

GENERAL
RELATIVITY

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.

The Core Idea

GRAVITY ISN'T
A FORCE,
IT'S A VIBE

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.

Gravitational wavesPredicted & confirmed ✓
Light bending near massPredicted & confirmed ✓
Gravitational time dilationPredicted & confirmed ✓
Black holesPredicted & confirmed ✓
Free Fall & Geodesics

THE STRAIGHTEST POSSIBLE
CROOKED PATH

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.

Visualisation A classic — with known caveats

THE UNIVERSE
AS A BOUNCY CASTLE

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.

the sheet visualisation and the path of light and mass
Known Limitations of the Sheet
  • Objects sit on top of spacetime in the visual. Not accurate — objects exist within it.
  • The sheet is 2D. Spacetime is 4D (three spatial dimensions + time).
  • It explains gravity using gravity — the sheet only curves because of a separate gravitational pull.
  • It has no time component; the "spacetime" in the visual is really just "space."
A Better Version

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.

General Relativity — Gravitational Time Dilation

THE EQUATION
THAT DOES IT ALL

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.

$$ds^2 = -\!\left(1 - \frac{2GM}{c^2 r}\right)c^2\,dt^2 + \left(1 - \frac{2GM}{c^2 r}\right)^{-1}dr^2 + r^2\,d\Omega^2$$
Eq. 4Schwarzschild Metric
$$r_s = \frac{2GM}{c^2}$$
Eq. 5Schwarzschild Radius — where light cannot escape

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:

$$\text{Grav. TD Factor} = \sqrt{1 - \frac{2GM}{c^2 r}}$$
Eq. 6Gravitational Time Dilation Factor
$G$Gravitational constant
$M$Mass of the object
$r$Distance away from the object
$c$Speed of light
The Hidden Connection

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:

$$\frac{2GM}{r} = v^2$$
Eq. 7Also known as $\sqrt{2GM/r} = v$

This shows that gravitational time dilation and velocity-based time dilation are the same phenomenon, and gives an equation to substitute between them.

The Conclusion

THERE IS NO
TRUE TIME

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

Einstein: Humanities Savior

The history of general relativity

Act One

THE JOURNEY
TO GENERAL
RELATIVITY

1905 Special Relativity

EINSTEIN BEGINS
THE JOURNEY

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.

fuel source
Key details
  • Special relativity published in 1905
  • Contradicted Newtonian mechanics
  • Gravity must propagate at the speed of light
  • Thought experiments guided the new theory

Fig. H1 — Einstein's 1905 annus mirabilis papers.

1907 The Key Insight

THE EQUIVALENCE
PRINCIPLE

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.

guy wow
Key details
  • Free fall feels weightless
  • Gravity and acceleration are locally indistinguishable
  • Physics behaves the same in accelerating frames
  • Foundation for general relativity

Fig. H2 — The equivalence of gravity and acceleration.

1908–1912 Geometry of Gravity

MASS CURVES
SPACETIME

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.

not guy wow
Key details
  • Space and time are united in Minkowski spacetime
  • Mass curves spacetime, changing particle paths
  • Light appears to bend in accelerating frames
  • Gravity becomes geometry, not a force

Fig. H3 — Minkowski diagram.

1912–1915 The Mathematics

FINDING THE
RIGHT GEOMETRY

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.

CollaboratorMarcel Grossmann — Mathematics
Geometry usedRiemannian (curved surfaces)
ResultGeneral Theory of Relativity
Key details
  • Einstein chose geometry for gravity
  • Riemannian geometry describes curved surfaces
  • Grossmann helped with mathematical form
  • Led directly to general relativity
not guy wow

Fig. H4 — Eienstiens notes.

Act Two

THE SCHWARZSCHILD
SOLUTION

1916 World War I

A LETTER FROM
THE TRENCHES

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
not guy wow

Fig. H5 — Karl Schwarzschild, who solved Einstein's equations from the front.

1916–1930s The Great Debate

THE PROBLEM OF
THE EVENT HORIZON

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.

Event horizon (r = rs)Escape velocity → ∞
Singularity (r = 0)Spacetime curvature → ∞
Einstein's reactionBelieved it impossible
not guy wow

Fig. H6 — Don't know what to put here so here is a sea cucumber.

Act Three

PROOF OF
BLACK HOLES

1925–1930 Quantum Mechanics

THE WHITE DWARF
BARRIER

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.

1.44 M
The Chandrasekhar limit — maximum mass of a white dwarf
not guy wow

Fig. H7 — Electron degeneracy pressure holding up a white dwarf.

1930–1939 The Final Frontier

THE BIRTH OF
BLACK HOLES

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.

Chandrasekhar limit~1.44 M — white dwarf max
TOV limit~2.17 M — neutron star max
Beyond TOVBlack hole — inevitable collapse
not guy wow
Quick recap
  • Chandrasekhar showed collapse beyond white dwarfs
  • Neutron stars have a mass limit too
  • Beyond the TOV limit, collapse continues
  • Black holes form when radius falls below Schwarzschild radius

Fig. H8 — Stellar collapse: white dwarf → neutron star → black hole.

History Summary
Timeline highlights

Relativity history at a glance

  • 1905: special relativity challenges Newton
  • 1907: equivalence principle links gravity and acceleration
  • 1912–1915: curved spacetime and Riemannian geometry
  • 1916: Schwarzschild solution introduces black hole radius
  • 1930s: Chandrasekhar and TOV limits lead to black hole formation
  • 1960s: (A little extra) John Archibald Wheeler popularized the phrase “Black hole” in a interview and it stuck.