Something Strange Happens When You Follow Einstein's Math

Veritasium
29 Apr 202437:02

Summary

TLDRThe video delves into the fascinating world of black holes, white holes, and wormholes through the lens of Einstein's general theory of relativity. It explains the concept of event horizons, the nature of spacetime curvature around massive objects, and how these phenomena challenge our understanding of the universe. The script also touches on historical scientific debates, the limitations of Newtonian gravity, and the potential existence of parallel universes. Despite current scientific skepticism about the reality of white holes and traversable wormholes, the video highlights the evolving nature of scientific discovery and the possibility of future surprises.

Takeaways

  • 🕳️ You can never see anything enter a black hole from an external perspective; objects appear to slow down and freeze at the event horizon.
  • 🚀 Gravity affects time, making it appear as if objects near a black hole slow down and eventually freeze in time from an outside viewpoint.
  • 🌌 The Schwarzschild metric describes how spacetime curves outside a mass, predicting the existence of black holes with a singularity at the center.
  • 🕰️ In the context of a black hole, time freezes at the event horizon for an external observer, but someone falling in would pass through without noticing.
  • 🔄 The Schwarzschild solution includes both black holes and white holes, which are time-reversed black holes ejecting matter instead of consuming it.
  • 🔭 Neutron stars can support themselves against collapse using neutron degeneracy pressure, but they also have a mass limit, leading to the possibility of black holes.
  • 💫 Rotating black holes, described by the Kerr solution, have multiple layers including the ergosphere and two event horizons, allowing complex spacetime behavior.
  • 🌐 Parallel universes and wormholes can be part of the solutions to Einstein's equations, though their physical existence is uncertain due to stability issues.
  • 📉 The existence of white holes, traversable wormholes, and parallel universes is theoretically possible but unlikely based on our current understanding of physics.
  • 🛡️ Exotic matter with negative energy density is theoretically required to stabilize wormholes, but its existence is highly doubtful according to current physical laws.

Q & A

  • What happens to time as an object approaches the event horizon of a black hole?

    -As an object approaches the event horizon of a black hole, from an outside observer's perspective, the object's time appears to slow down. At the exact instant the object crosses the event horizon, it seems to stop completely, frozen in time.

  • What is the significance of the term 'redshift' in the context of black holes?

    -Redshift refers to the phenomenon where light from an object, such as a spaceship near a black hole, gets stretched to longer, redder wavelengths due to the gravitational pull of the black hole. This makes the light dimmer and redder until it fades from view.

  • What is the Schwarzschild solution and how does it relate to black holes?

    -The Schwarzschild solution is the first non-trivial solution to Einstein's field equations of general relativity. It describes how spacetime curves outside of a spherically symmetric, non-rotating mass, which is the theoretical basis for understanding the properties of black holes.

  • What is the role of the Chandrasekhar limit in the context of stellar evolution?

    -The Chandrasekhar limit is the maximum mass that a white dwarf star can have while being supported by electron degeneracy pressure. If a star exceeds this limit, it will continue to collapse, potentially forming a neutron star or a black hole.

  • What is the difference between a black hole and a white hole?

    -A black hole is a region in spacetime where the gravitational pull is so strong that nothing, not even light, can escape from it. In contrast, a white hole is a theoretical concept where matter and light are expelled outwards from a singularity, with the time-reversed properties of a black hole.

  • What is an Einstein-Rosen bridge, and how is it related to wormholes?

    -An Einstein-Rosen bridge, also known as a wormhole, is a hypothetical structure that connects two separate points in spacetime. It is a solution to the general theory of relativity and suggests the possibility of instantaneous travel between these points, potentially across different universes.

  • What is the significance of the Penrose diagram in understanding black holes?

    -The Penrose diagram is a graphical representation of the spacetime of a black hole. It helps visualize the infinite past, infinite distance, and infinite future, as well as the regions inside and outside the event horizon, providing insights into the behavior of objects near a black hole.

  • What is the ergosphere and how does it relate to a rotating black hole?

    -The ergosphere is a region outside the event horizon of a rotating black hole where space is dragged along with the black hole's rotation. Within the ergosphere, it is impossible to remain stationary relative to distant stars due to the frame-dragging effect.

  • What is the concept of an anti-verse as mentioned in the script?

    -An anti-verse is a hypothetical universe where the fundamental properties, such as gravity, are reversed compared to our own universe. In the context of the script, it is suggested that one might end up in an anti-verse by passing through the singularity of a rotating black hole.

  • What are the theoretical requirements for a traversable wormhole according to Einstein's general relativity?

    -According to Einstein's general relativity, a traversable wormhole would require an exotic form of matter with negative energy density to keep it open and stable. This is necessary to prevent the wormhole from collapsing and to allow for the possibility of travel through it.

  • Why might white holes and wormholes not exist in reality according to the script?

    -White holes and wormholes might not exist in reality because they require solutions of Einstein's field equations that describe eternal black holes in an empty universe, which does not account for the formation of such objects. Additionally, the presence of an inner horizon in rotating black holes might seal off the singularity, preventing the existence of white holes and wormholes.

Outlines

00:00

🌌 The Enigma of Black Holes

This paragraph delves into the peculiarities of black holes, explaining how objects falling into them appear to slow down and freeze at the event horizon due to the effects of gravity on time. It discusses the redshift of light and the theoretical images of everything that has fallen captured on the event horizon. The script also touches on Einstein's general theory of relativity, which predicts not only black holes but also their opposites, white holes, and the possibility of parallel universes and wormholes. The limitations of Newtonian gravity are contrasted with Einstein's concept of gravity as mediated by the curvature of spacetime.

05:01

🔍 Unraveling Spacetime with Einstein's Equations

This section explores Einstein's field equations, which describe how matter and energy influence the curvature of spacetime. It explains the complexity of these equations and the challenge they present in finding solutions. The paragraph introduces the concept of a light cone, illustrating how it defines the region of spacetime an observer can interact with. It also discusses the significance of the spacetime interval and how it is affected by the presence of mass, leading to the groundbreaking Schwarzschild solution that describes the curvature of spacetime around a spherically symmetric mass.

10:01

💫 The Schwarzschild Solution and Black Holes

This paragraph examines the Schwarzschild solution, which describes the spacetime curvature outside a spherically symmetric mass. It highlights the discovery of singularities within this solution, indicating points where the curvature becomes infinite. The first singularity is at the center of the mass, while the second is at the Schwarzschild radius, where the escape velocity equals the speed of light, suggesting the existence of black holes. The script also touches on the historical debate among astronomers about the end of a star's life and the mechanisms that could prevent a star from collapsing into a black hole.

15:03

🌟 The Life and Death of Stars

This section discusses the life cycle of stars, focusing on what happens when nuclear fuel runs out. It explains the balance between gravity and radiation pressure and how, once the fuel is exhausted, gravity causes the star to collapse. The paragraph introduces Ralph Fowler's theory of electron degeneracy pressure as a support mechanism for white dwarfs, as well as Subrahmanyan Chandrasekhar's realization that there is a limit to this pressure, known as the Chandrasekhar limit. The script also covers the discovery of neutron stars and the eventual acceptance of the possibility of black holes.

20:04

🌀 Black Holes and the Flow of Spacetime

This paragraph explores the concept of space flowing into a black hole, likened to a waterfall. It discusses how photons emitted by an object near a black hole must 'swim' against this flow, which becomes increasingly difficult as the object approaches the event horizon. The script explains that the event horizon is infinitely thin, allowing photons to either escape or fall in, and that inside the horizon, space falls faster than the speed of light, leading everything towards the singularity. It also humorously compares this concept to the frustration of dealing with spam calls.

25:05

🌐 The Geometry of Black Holes and the Universe

This section delves into the geometric representation of black holes and the universe, discussing the transformation of the black hole singularity into a line representing the final moment in time for anything entering a black hole, as depicted in the Kruskal-Szekers diagram. The Penrose diagram is introduced, showing the entire universe, including the infinite past, future, and distant regions, all connected through the black hole's singularity. The script also explores the concept of a white hole, which is the time-reversed counterpart of a black hole, and the possibility of parallel universes connected through black holes.

30:07

🌀 The Complexities of Rotating Black Holes

This paragraph examines the complexities introduced by rotating black holes, as described by the Kerr solution to Einstein's equations. It explains how rotation causes the black hole to bulge at the equator and the resulting structure of multiple layers, including the ergosphere where space is dragged around with the black hole. The script discusses the possibility of entering the inner event horizon and the strange phenomenon of a ring-shaped singularity, suggesting the potential for travel through the singularity into another universe or an anti-verse where gravity pushes instead of pulls.

35:10

🌌 The Theoretical Implications of Black Holes

This section contemplates the theoretical implications of black holes, including the possibility of wormholes and parallel universes. It discusses the Penrose diagram for a spinning black hole and the concept of an infinite number of universes connected through black holes and white holes. The script also addresses the practical challenges and the skepticism around the existence of white holes and traversable wormholes, given the requirement for exotic matter with negative energy density. It concludes by acknowledging the history of being surprised by the universe, suggesting that our understanding may yet evolve.

Mindmap

Keywords

💡Black Hole

A black hole is a region in space where the gravitational pull is so strong that nothing, not even light, can escape from it. In the video, black holes are central to the discussion, illustrating how they distort spacetime and affect the behavior of objects and light around them. The script mentions that black holes can trap light and matter at their event horizon, creating a visual effect where objects appear to slow down and freeze in time as they approach it.

💡Event Horizon

The event horizon is the boundary around a black hole beyond which no information or matter can escape. It is depicted in the script as the point of no return, where objects, including light, are inexorably drawn into the black hole. The concept is crucial for understanding the behavior of a black hole and its interaction with its surroundings.

💡General Theory of Relativity

The general theory of relativity, proposed by Albert Einstein, is the current best theory describing gravity. It underpins the script's discussion on how gravity affects spacetime, leading to phenomena like black holes. The theory is mentioned as the foundation for understanding the curvature of spacetime and the behavior of massive objects like stars and black holes.

💡Spacetime

Spacetime is a concept that combines the three dimensions of space with the one dimension of time into a single four-dimensional continuum. The script uses spacetime to explain how the presence of a massive object like a black hole warps this continuum, affecting the flow of time and the paths of objects moving through it.

💡Singularity

In the context of the video, a singularity refers to a point within a black hole where the density of matter is theoretically infinite, and the laws of physics as we know them break down. The script discusses singularities as problematic points in the equations describing black holes, where certain quantities become infinite, indicating our current understanding of physics may be incomplete.

💡White Hole

A white hole is a hypothetical object that is the time-reverse of a black hole, where matter and light are expelled outwards instead of being drawn in. The script introduces the concept of white holes to illustrate the theoretical possibility of time-reversed solutions to Einstein's field equations, suggesting the existence of regions from which nothing can escape to the outside universe.

💡Wormhole

A wormhole, as discussed in the script, is a hypothetical tunnel-like structure that could provide a shortcut through spacetime, connecting two distant points in the universe or even two separate universes. The concept is part of the video's exploration of the exotic solutions to Einstein's equations and the potential for interstellar or interuniversal travel.

💡Einstein's Field Equations

Einstein's field equations are the core of his general theory of relativity and describe how mass and energy influence the curvature of spacetime. The script refers to these equations as the mathematical foundation for understanding the properties of black holes, white holes, and wormholes, and how they predict the existence of these phenomena.

💡Schwarzschild Solution

The Schwarzschild solution is the first non-trivial solution to Einstein's field equations, describing the spacetime geometry outside a spherically symmetric, non-rotating mass. The script mentions this solution as the starting point for understanding the properties of black holes, including the event horizon and singularity.

💡Kerr Solution

The Kerr solution, found by Roy Kerr, is a solution to Einstein's field equations that describes the geometry of spacetime around a rotating black hole. The script contrasts this with the Schwarzschild solution to highlight the differences between non-rotating and rotating black holes, such as the presence of an ergosphere and a different structure of the singularity.

💡Exotic Matter

Exotic matter, as touched upon in the script, refers to a hypothetical form of matter with negative energy density, which is required to keep wormholes open and stable. The concept is part of the discussion on the theoretical possibility of traversable wormholes and the challenges associated with their existence.

Highlights

Objects appear to slow down as they approach a black hole due to time dilation.

At the event horizon, objects seem to stop, and light becomes too redshifted to see.

General theory of relativity predicts black holes, white holes, and parallel universes.

Newton's gravity theory had a fundamental flaw regarding action at a distance.

Einstein's theory of relativity explains gravity through the curvature of spacetime.

Einstein's field equations relate the distribution of matter and energy to spacetime curvature.

The Schwarzschild metric describes spacetime curvature outside a spherically symmetric mass.

The Schwarzschild radius marks the event horizon where not even light can escape.

Astronomers studied star collapse and the role of electron degeneracy pressure.

Chandrasekhar limit defines the maximum mass a white dwarf can have before collapsing.

Neutron stars can support heavier stars than white dwarfs due to neutron degeneracy pressure.

Oppenheimer and Volkoff showed neutron stars have a maximum mass and can lead to black holes.

Einstein initially doubted the existence of black holes due to the freezing of time at the horizon.

The concept of a white hole, the time reverse of a black hole, was introduced.

Penrose diagrams provide a comprehensive map of spacetime, including black holes and white holes.

Einstein-Rosen bridges, or wormholes, hypothetically connect two points in spacetime, potentially across universes.

Rotating black holes, as described by the Kerr solution, have a more complex structure with an ergosphere.

Inside a rotating black hole, there's a theoretical possibility to avoid the singularity and enter another universe.

Theoretical wormholes require exotic matter with negative energy density to remain open.

Current understanding suggests that traversable wormholes and parallel universes are unlikely to exist.

Transcripts

play00:00

- You can never see anything enter a black hole.

play00:03

(bell dings)

play00:04

Imagine you trap your nemesis in a rocket ship

play00:07

and blast him off towards a black hole.

play00:10

He looks back at you shaking his fist at a constant rate.

play00:14

As he zooms in, gravity gets stronger,

play00:17

so you would expect him to speed up,

play00:19

but that is not what you see.

play00:21

Instead, the rocket ship appears to be slowing down.

play00:25

Not only that, he also appears

play00:27

to be shaking his fist slower and slower.

play00:30

That's because from your perspective,

play00:32

his time is slowing down

play00:35

at the very instant when he should cross the event horizon,

play00:38

the point beyond which not even light can escape,

play00:41

he and his rocket ship do not disappear,

play00:45

instead, they seem to stop frozen in time.

play00:51

The light from the spaceship gets dimmer and redder

play00:54

until it completely fades from view.

play00:57

This is how any object would look

play00:59

crossing the event horizon.

play01:01

Light is still coming from the point where he crossed,

play01:04

it's just too redshifted to see,

play01:08

but if you could see that light,

play01:10

then in theory you would see everything

play01:12

that has ever fallen into the black hole

play01:14

frozen on its horizon, including the star that formed it,

play01:19

but in practice, photons are emitted at discreet intervals,

play01:22

so there will be a last photon emitted outside the horizon,

play01:26

and therefore these images will fade after some time.

play01:29

- This is just one of the strange results

play01:32

that comes outta the general theory of relativity,

play01:34

our current best theory of gravity.

play01:36

The first solution of Einstein's equations

play01:38

predicted not only black holes,

play01:40

but also their opposite, white holes.

play01:43

It also implied the existence of parallel universes

play01:46

and even possibly a way to travel between them.

play01:50

This is a video about the real science of black holes,

play01:53

white holes, and wormholes.

play01:56

- The general theory of relativity

play01:58

arose at least in part due to a fundamental flaw

play02:00

in Newtonian gravity.

play02:02

In the 1600s Isaac Newton

play02:04

contemplated how an apple falls to the ground,

play02:06

how the moon orbits the earth and earth orbits the sun

play02:09

and he concluded that every object with mass

play02:12

must attract every other,

play02:14

but Newton was troubled by his own theory.

play02:17

How could masses separated by such vast distances

play02:20

apply a force on each other?

play02:22

He wrote, "That one body may act upon another at a distance

play02:26

through a vacuum without the mediation of anything else

play02:29

is to me, so great and absurdity that I believe no man

play02:33

who has a competent faculty of thinking

play02:34

could ever fall into it."

play02:38

One man who definitely had a competent faculty of thinking,

play02:42

was Albert Einstein and over 200 years later,

play02:45

he figured out how gravity is mediated.

play02:48

Bodies do not exert forces on each other directly.

play02:52

Instead, a mass like the sun curves the spacetime

play02:55

in its immediate vicinity.

play02:58

This, then curves the spacetime around it

play03:00

and so on all the way to the earth.

play03:03

So the earth orbits the sun, because the spacetime

play03:06

earth is passing through is curved.

play03:09

Masses are affected by the local curvature

play03:12

of spacetime, so no action at a distance is required.

play03:16

Mathematically, this is described

play03:18

by Einstein's field equations.

play03:20

Can you write down the Einstein field equation?

play03:23

- This was the the result of Einstein's decade of hard work

play03:26

after special relativity

play03:28

and essentially what we've got in the field equations

play03:30

on one side it says,

play03:32

tell me about the distribution of matter and energy.

play03:34

The other side tells you what the resultant curvature

play03:37

of spacetime is from that distribution

play03:40

of matter and energy and it's a single line.

play03:43

It looks like, oh, this is a simple equation, right?

play03:46

But it's not really one equation.

play03:47

It's a family of equations and to make life more difficult,

play03:51

they're coupled equations, so they depend upon each other

play03:54

and they are differential equations,

play03:56

so it means that there are integrals

play03:58

that have to be done, da, da da.

play04:00

So there's a whole bunch of steps that you need to do

play04:02

to solve the field equations.

play04:04

To see what a solution to these equations would look like,

play04:07

we need a tool to understand spacetime.

play04:11

So imagine your floating around in empty space.

play04:14

A flash of light goes off above your head

play04:16

and spreads out in all directions.

play04:19

Now your entire future, anything that can

play04:22

and will ever happen to you will occur within this bubble

play04:27

because the only way to get out of it

play04:29

would be to travel faster than light.

play04:31

In two dimensions, this bubble is just a growing circle.

play04:35

If we allow time to run up the screen

play04:37

and take snapshots at regular intervals,

play04:39

then this light bubble traces out a cone,

play04:41

your future light cone.

play04:43

By convention, the axes are scaled so that light rays

play04:46

always travel at 45 degrees.

play04:48

This cone reveals the only region of spacetime

play04:51

that you can ever hope to explore and influence.

play04:55

Now imagine that instead of a flash of light

play04:57

above your head, those photons were actually traveling in

play05:00

from all corners of the universe

play05:02

and they met at that instant

play05:03

and then continued traveling on

play05:05

in their separate directions.

play05:08

Well, in that case then into the past,

play05:10

these photons also reveal a light cone,

play05:13

your past light cone.

play05:15

Only events that happened inside this cone

play05:17

could have affected you up to the present moment.

play05:21

We can simplify this diagram even further

play05:23

by plotting just one spatial and one time dimension.

play05:26

This is the spacetime diagram of empty space.

play05:29

If you want to measure how far apart

play05:31

two events are in spacetime, you use something called

play05:34

the spacetime interval.

play05:36

The interval squared is equal to minus dt squared,

play05:39

plus dx squared, since spacetime is flat,

play05:43

the geometry is the same everywhere

play05:45

and so this formula holds throughout the entire diagram,

play05:48

which makes it really easy to measure the separation

play05:50

between any two events, but around a mass,

play05:54

spacetime is curved and therefore you need to modify

play05:57

the equation to take into account the geometry.

play06:00

This is what solutions to Einstein's equations are like.

play06:04

They tell you how spacetime curves

play06:06

and how to measure the separation between two events

play06:09

in that curved geometry.

play06:12

Einstein published his equations in 1915

play06:15

during the First World War,

play06:16

but he couldn't find an exact solution.

play06:19

Luckily, a copy of his paper made its way

play06:22

to the eastern front where Germany was fighting Russia,

play06:25

stationed there was one of the best astrophysicists

play06:27

of the time, Karl Schwarzschild.

play06:30

Despite being 41 years old, he had volunteered

play06:33

to calculate artillery trajectories for the German army.

play06:36

At least until a greater challenge caught his attention,

play06:40

how to solve Einstein's field equations.

play06:45

Schwarzschild did the standard physicist thing

play06:47

and imagined the simplest possible scenario,

play06:49

an eternal static universe with nothing in it

play06:52

except a single spherically symmetric point mass.

play06:55

This mass was electrically neutral and not rotating.

play06:59

Since this was the only feature of his universe,

play07:01

he measured everything using spherical coordinates

play07:04

relative to this center of this mass.

play07:06

So r is the radius and theta and phi give the angles.

play07:10

For his time coordinate, he chose time as being measured

play07:13

by someone far away from the mass,

play07:15

where spacetime is essentially flat.

play07:18

Using this approach, Schwarzschild found the first

play07:20

non-trivial solution to Einstein's equations,

play07:23

which nowadays we write like this.

play07:26

This Schwarzschild metric describes how spacetime curves

play07:30

outside of the mass.

play07:32

It's pretty simple and makes intuitive sense,

play07:34

far away from the mass spacetime is nearly flat,

play07:37

but as you get closer and closer to it,

play07:39

spacetime becomes more and more curved,

play07:41

it attracts objects in and time runs slower.

play07:45

(gunshots firing)

play07:47

Schwarzschild sent his solution to Einstein,

play07:49

concluding with, "The war treated me kindly enough

play07:52

in spite of the heavy gunfire

play07:54

to allow me to get away from it all

play07:55

and take this walk in the land of your ideas."

play08:00

Einstein replied, "I have read your paper

play08:02

with the utmost interest, I had not expected

play08:04

that one could formulate the exact solution to the problem

play08:06

in such a simple way."

play08:12

But what seemed at first quite simple,

play08:15

soon became more complicated.

play08:17

Shortly after Schwarzschild solution was published,

play08:19

people noticed two problem spots.

play08:22

At the center of the mass, at r equals zero,

play08:25

this term is divided by zero, so it blows up to infinity

play08:30

and therefore this equation breaks down

play08:32

and it can no longer describe what's physically happening.

play08:35

This is what's called a singularity.

play08:38

Maybe that point could be excused,

play08:40

because it's in the middle of the mass,

play08:42

but there's another problem spot outside of it

play08:45

at a special distance from the center

play08:47

known as the Schwarzschild radius, this term blows up.

play08:50

So there is a second singularity. What is going on here?

play08:57

Well, at the Schwarzschild radius,

play09:00

the spacetime curvature becomes so steep

play09:02

that the escape velocity, the speed that anything would need

play09:06

to leave there is the speed of light

play09:10

and that would mean that inside the Schwarzschild radius,

play09:13

nothing, not even light would be able to escape.

play09:17

So you'd have this dark object

play09:18

that swallows up matter and light,

play09:22

a black hole, if you will,

play09:26

but most scientists doubted that such an object could exist,

play09:29

because it would require a lot of mass

play09:31

to collapse down into a tiny space.

play09:35

How could that possibly ever happen?

play09:39

(thrilling music)

play09:40

Astronomers at the time were studying

play09:42

what happens at the end of a star's life.

play09:44

During its lifetime the inward force of gravity is balanced

play09:47

by the outward radiation pressure

play09:49

created by the energy released through nuclear fusion,

play09:52

but when the fuel runs out, the radiation pressure drops.

play09:55

So gravity pulls all the star material inwards, but how far?

play10:01

Most astronomers believed some physical process

play10:04

would hold it up and in 1926,

play10:07

Ralph Fowler came up with a possible mechanism.

play10:10

Pauli's exclusion principles states that,

play10:11

"Fermions like electrons cannot occupy the same state,

play10:15

so as matter gets pushed closer and closer together,

play10:18

the electrons each occupy their own tiny volumes,"

play10:21

but Heisenberg's uncertainty principle says that,

play10:23

"You can't know the position and momentum of a particle

play10:26

with absolute certainty, so as the particles become

play10:29

more and more constrained in space,

play10:32

the uncertainty in their momentum,

play10:34

and hence their velocity must go up."

play10:37

So the more a star is compressed,

play10:39

the faster electrons will wiggle around

play10:41

and that creates an outward pressure.

play10:44

This electron degeneracy pressure would prevent the star

play10:47

from collapsing completely.

play10:49

Instead, it would form a white dwarf

play10:51

with the density much higher than a normal star

play10:54

and remarkably enough astronomers had observed stars

play10:57

that fit this description.

play10:58

One of them was Sirius B.

play11:04

But the relief from this discovery was short-lived.

play11:06

Four years later, 19-year-old Subrahmanyan Chandrasekhar

play11:09

traveled by boat to England to study with Fowler

play11:12

and Arthur Eddington, one of the most revered scientists

play11:15

of the time.

play11:17

During his voyage, Chandrasekhar realized

play11:19

that electron degeneracy pressure has its limits.

play11:22

Electrons can wiggle faster and faster,

play11:24

but only up to the speed of light.

play11:27

That means this effect can only support stars

play11:30

up to a certain mass, the Chandrasekhar limit.

play11:33

Beyond this, Chandrasekhar believed,

play11:35

not even electron de degeneracy pressure

play11:37

could prevent a star from collapsing,

play11:40

but Eddington was not impressed.

play11:42

He publicly blasted Chandrasekhar saying,

play11:45

"There should be a law of nature

play11:47

to prevent a star from behaving in this absurd way"

play11:51

and indeed scientists did discover a way

play11:53

that stars heavier than the Chandrasekhar limit

play11:55

could support themselves.

play11:58

When a star collapses beyond a white dwarf,

play12:00

electrons and protons fuse together

play12:02

to form neutrinos and neutrons.

play12:05

These neutrons are also fermions,

play12:07

but with nearly 2000 times the mass an electron,

play12:10

their degeneracy pressure is even stronger.

play12:13

So this is what holds up neutron stars.

play12:16

There was this conviction among scientists

play12:19

that even if we didn't know the mechanism,

play12:21

something would prevent a star from collapsing

play12:23

into a single point and forming a black hole,

play12:28

because black holes were just too preposterous to be real.

play12:34

The big blow to this belief came in the late 1930s

play12:38

when Jay Robert Oppenheimer and George Volkoff

play12:40

found that neutron stars also have a maximum mass.

play12:44

Shortly after Oppenheimer and Hartland Snyder

play12:47

showed that for the heaviest stars,

play12:49

there is nothing left to save them when their fuel runs out,

play12:53

they wrote, "This contraction will continue indefinitely,"

play12:58

but Einstein still couldn't believe it.

play13:00

Oppenheimer was saying that stars can collapse indefinitely,

play13:03

but when Einstein looked at the math,

play13:05

he found that time freezes on the horizon.

play13:08

So it seemed like nothing could ever enter,

play13:11

which suggested that either

play13:12

there's something we don't understand

play13:14

or that black holes can't exist,

play13:17

(star explodes)

play13:21

but Oppenheimer offered a solution to the problem.

play13:23

He said to an outside observer,

play13:26

you could never see anything go in,

play13:27

but if you were traveling across the event horizon,

play13:31

you wouldn't notice anything unusual

play13:33

and you'd go right past it without even knowing it.

play13:37

So how is this possible?

play13:39

We need a spacetime diagram of a black hole.

play13:43

On the left is the singularity at r equals zero.

play13:46

The dotted line at r equals 2M is the event horizon.

play13:49

Since the black hole doesn't move,

play13:51

these lines go straight up in time.

play13:55

Now let's see how ingoing and outgoing light ray travel

play13:58

in this curved geometry.

play14:01

When you're really far away,

play14:02

the future light cones are at the usual 45 degrees,

play14:06

but as you get closer to the horizon,

play14:07

the light cones get narrower and narrower,

play14:11

until right at the event horizon,

play14:13

they're so narrow that they point straight up

play14:16

and inside the horizon, the light cones tip to the left,

play14:22

but something strange happens with ingoing light rays.

play14:26

- They fall in, but they don't get to r equals 2M,

play14:29

they actually asymptote to that value

play14:32

as time goes to infinity,

play14:34

but they don't end at infinity, right?

play14:36

Mathematically they are connected and come back in

play14:41

and they're traveling in this direction

play14:44

and this bothered a lot of people,

play14:46

this bothered people like Einstein,

play14:48

because he looked at these equations and went,

play14:50

"well, if nothing can cross this sort of boundary,

play14:55

then how could there be black holes?

play14:57

How could black holes even form?"

play15:00

- So what is going on here?

play15:02

Well, what's important to recognize

play15:04

is that this diagram is a projection.

play15:06

It's basically a 2D map

play15:08

of four dimensional curved spacetime.

play15:12

It's just like projecting the 3D Earth onto a 2D map.

play15:15

When you do that, you always get distortions.

play15:18

There is no perfectly accurate way

play15:20

to map the earth onto a 2D surface,

play15:22

but different maps can be useful for different purposes.

play15:25

For example, if you wanna keep angles and shapes the same,

play15:28

like if you're sailing across the ocean

play15:30

and you need to find your bearings,

play15:31

you can use the Mercator projection,

play15:33

that's the one Google Maps uses.

play15:35

A downside is that it misrepresent sizes.

play15:39

Africa and Greenland look about the same size,

play15:42

but Africa is actually around 14 times larger.

play15:46

The Gall-Peters projection keeps relative sizes accurate,

play15:49

but as a result, angles and shapes are distorted.

play15:53

In a similar way, we can make different projections

play15:56

of 4D spacetime to study different properties of it.

play16:00

Physical reality doesn't change,

play16:01

but the way the map describes it does.

play16:05

- He had chosen to put a particular coordinate system

play16:07

of a space and have a time coordinate, and off you go.

play16:11

It's the most sensible thing to do, right?

play16:14

- [Derek] People realize that if you choose

play16:15

a different coordinate system

play16:17

by doing a coordinate substitution, then the singularity

play16:20

at the event horizon disappears.

play16:23

- It goes away.

play16:24

That problem goes away and things can actually cross

play16:27

into the black hole.

play16:30

- What this tells us is that there is

play16:32

no real physical singularity at the event horizon.

play16:36

It just resulted from a poor choice of coordinate system.

play16:41

Another way to visualize what's going on

play16:44

is by describing space as flowing in towards the black hole,

play16:48

like a waterfall.

play16:49

As you get closer, space starts flowing in

play16:52

faster and faster.

play16:54

Photons emitted by the spaceship have to swim

play16:56

against this flow, and this becomes harder and harder

play17:00

the closer you get.

play17:02

Photons emitted just outside the horizon

play17:04

can barely make it out, but it takes longer and longer.

play17:09

At the horizon, space falls in

play17:11

as fast as the photons are swimming.

play17:13

So if the horizon had a finite width,

play17:16

then photons would get stuck here,

play17:18

photons from everything that ever fell in,

play17:21

but the horizon is infinitely thin.

play17:23

So in reality, photons either eventually escape or fall in.

play17:29

Inside the horizon, space falls faster

play17:31

than the speed of light,

play17:33

and so everything falls into the singularity.

play17:36

So Oppenheimer was right.

play17:38

Someone outside a black hole can never see anything enter

play17:42

because the last photons they can see

play17:44

will always be from just outside the horizon,

play17:48

but if you yourself go,

play17:50

you will fall right across the event horizon

play17:52

and into the singularity.

play17:55

Now you can extend the waterfall model

play17:57

to cover all three spatial dimensions,

play17:59

and that gives you this, a real simulation

play18:02

of space flowing into a static black hole

play18:05

made by my friend Alessandro from ScienceClic.

play18:08

Later we'll use this model to see what it's like

play18:10

falling into a rotating black hole.

play18:16

Now, I've never been sucked into a black hole,

play18:18

but sometimes it feels like it when I'm stuck on the phone

play18:20

with a spam collar.

play18:22

Fortunately, today's sponsor Incogni can help.

play18:25

You know, I used to get several spam calls a day,

play18:28

and they frustrated me so much that I wrote a letter

play18:31

to the Do Not Call registry to get my number removed,

play18:33

but that didn't work

play18:35

and so I wanted to go on the offensive.

play18:37

I even contemplated making a video

play18:40

where I just mess with spam callers to get some revenge

play18:43

for all the frustration and lost time,

play18:45

but I no longer have to do that thanks to Incogni.

play18:48

There are a lot of data brokers out there

play18:50

that suck up information about you, a bit like a black hole.

play18:54

They collect things like your name, phone number,

play18:56

email address, and even your social security number

play18:59

and then they sell this information on the open market,

play19:03

which is why we often get calls from people

play19:05

that we've never even given our number to.

play19:08

Incogni battles these data brokers,

play19:11

you simply give them permission and they figure out

play19:13

who out there has your data, which laws apply,

play19:16

and then they send them the right letter,

play19:18

with the correct legal terms to each data broker

play19:21

with the request to remove your information.

play19:23

Now, you could do this yourself,

play19:25

but it's a super tedious process that would take days,

play19:27

weeks, even months,

play19:29

and then you'd have to keep doing it forever.

play19:32

So that's something I definitely don't have the time

play19:35

and energy for, but Incogni makes this really easy.

play19:39

Just sign up and they'll give you a list of companies

play19:41

that have your data, the severity of each claim,

play19:44

and the status of each request.

play19:46

So far, they have filed 126 requests for me,

play19:49

83 of which have been completed saving me over

play19:52

62 hours of work, but the best part is since I signed up,

play19:56

I've hardly gotten any more spam calls.

play19:58

So to try Incogni and fight against the data brokers,

play20:01

visit incog.com/veritasium.

play20:04

You can click that link down in the description

play20:06

or scan the QR code right here

play20:08

and make sure to use the code veritasium to get 60% off.

play20:12

So head over to incog.com/veritasium to get started.

play20:16

I wanna thank Incogni for sponsoring this part of the video

play20:19

and now back to spacetime maps.

play20:22

If you take this map and transform it

play20:25

so that incoming and outgoing light ray

play20:27

all travel at 45 degrees like we're used to,

play20:30

then something fascinating happens.

play20:33

The black hole singularity on the left

play20:35

transforms into a curved line at the top

play20:40

and since the future always points up in this map,

play20:44

it tells us that the singularity is not actually

play20:47

a place in space, instead, it's a moment in time,

play20:52

the very last moment in time for anything

play20:55

that enters a black hole.

play20:58

The map we've just created is a Kruskal-Szekers diagram,

play21:02

but this only represents a portion of the universe,

play21:04

the part inside the black holes event horizon

play21:07

and the part of the universe closest to it,

play21:10

but what we can do is contract the whole universe,

play21:13

the infinite past, infinite distance, and infinite future,

play21:17

and morph it into a single map.

play21:20

It's like using the universe's best fish eye lens.

play21:24

That gives us this penrose diagram.

play21:28

Again, light rays still always go at 45 degrees.

play21:31

So the future always points up.

play21:33

The infinite past is in the bottom of the diagram.

play21:36

The infinite future at the top

play21:39

and the sides on the right are infinitely far away.

play21:42

The black hole singularity is now a straight line

play21:44

at the top, a final moment in time.

play21:49

These lines are all at the same distance

play21:51

from the black hole.

play21:52

So the singularity is at r equals zero,

play21:55

the horizon is at r equals 2M,

play21:57

this line is at r equals 4M,

play21:59

and this is infinitely far away.

play22:02

All of these lines are at the same time.

play22:05

What's great about this map is that it's very easy to see

play22:09

where you can still go and what could have affected you.

play22:12

For example, when you're here, you've got a lot of freedom.

play22:15

You can enter the black hole or fly off to infinity,

play22:19

and you can see and receive information from this area,

play22:23

but if you go beyond the horizon,

play22:25

your only possible future is to meet the singularity.

play22:29

You can still, however, see and receive information

play22:32

from the universe.

play22:33

You just can't send any back out.

play22:36

Now think about being at this point in the map.

play22:39

This is at the event horizon,

play22:41

and now your entire future is within the black hole,

play22:45

but what is the past of this moment?

play22:48

Well, you can draw the past light cone

play22:51

and it reveals this new region.

play22:54

If you're inside this region,

play22:56

you can send signals to the universe,

play22:58

but no matter where you are in the universe,

play23:00

nothing can ever enter this region

play23:02

because it will never be inside your light comb.

play23:06

So things can come out, but never go in.

play23:09

This is the opposite of a black hole, a white hole.

play23:15

What color is a white hole?

play23:18

(Geraint exhales)

play23:19

(Derek laughs)

play23:20

- I mean, it's gonna be the,

play23:22

it's not gonna have a color, right?

play23:24

It's gonna be whatever's being spat out of it.

play23:27

It depends what's in there and gets thrown out,

play23:31

that's what you are going to see.

play23:33

So if it's got light in there, it's got mass in there,

play23:35

it's all gonna be ejected.

play23:36

So the white hole kind of picture

play23:39

is the time reverse picture of a black hole,

play23:42

instead of things falling in, things get expelled outwards

play23:46

and so whilst a black hole has a membrane,

play23:51

the Schwarzschild horizon, which once you cross,

play23:53

you can't get back out, the white hole has the opposite.

play23:56

If you're inside the event horizon, you have to be ejected,

play23:59

so it kicks you out kind of thing, right?

play24:01

Relativity doesn't tell you which way time flows.

play24:04

There's nothing in there that says that, that is the future

play24:08

and that is the past.

play24:10

When you are doing your mathematics

play24:12

and you're working out the behavior of objects,

play24:15

you make a choice about which direction is the future,

play24:19

but mathematically, you could have chosen

play24:21

the other way, right?

play24:22

You could have had time point in the opposite direction.

play24:25

Any solution that you find in relativity,

play24:28

mathematically, you can just flip it

play24:30

and get a time reverse solution

play24:32

and that's also a solution to the equations.

play24:36

- [Derek] Now, we've been showing things

play24:37

being ejected to the right, but they could just as well

play24:40

be ejected to the left.

play24:42

So what's over there?

play24:44

This line is not at infinity,

play24:46

so there should be something beyond it.

play24:49

If we eject things in this direction,

play24:51

you find that they enter a whole new universe,

play24:55

one parallel to our own.

play25:01

- [Geraint] We can fall into this black hole,

play25:03

and somebody in this universe here

play25:05

could fall into this black hole in their universe,

play25:08

and we would find ourselves in the same black hole.

play25:11

(Derek chuckles)

play25:12

- The only downside is that

play25:14

we'd both soon end up in the singularity.

play25:18

I guess I'm just trying to understand

play25:20

where that universe appears

play25:22

in the mathematical part of the solution.

play25:24

Like, can you point to the part of the equation and be like,

play25:27

so that's our universe, and then these terms here,

play25:30

that's the other universe, or do you know what I mean?

play25:32

Like- - Yeah,

play25:33

well, it's coordinates, right?

play25:35

Imagine somebody, right, came up with a coordinate system

play25:40

for the earth, but only the northern hemisphere

play25:43

and you looked at that coordinate system, right?

play25:45

And you looked at it and you said,

play25:47

"Ah, I can see the coordinate system, it looks fine,

play25:50

but mathematically latitudes can be negative, right?

play25:55

You've only got positive latitudes in your solution.

play25:58

What about the negative ones?"

play25:59

And they said to you, (scoffs) "Negative ones?

play26:02

No southern hemisphere, right?"

play26:05

And you've gotta go, "Well, the mathematics says that

play26:08

you can have negative latitudes.

play26:09

Maybe we should go and look over the equator

play26:12

to see if there is something down there"

play26:13

and I know that's a kind of extreme example,

play26:16

because we know we live on a globe,

play26:17

but we don't know the full geometry

play26:20

of what's going on here in the sense that

play26:22

Schwarzschild laid down coordinates

play26:24

over part of the solution.

play26:26

It was like him only laying down coordinates

play26:28

on the northern hemisphere

play26:30

and other people have come along and said,

play26:32

"Hey, there's a southern hemisphere"

play26:34

and more than that, there's two earths.

play26:36

That's why it's called maximal extension.

play26:39

It's like, if I have this mathematical structure,

play26:43

then what is the extent of the coordinates

play26:47

that I can consider?

play26:49

And with the Schwarzschild black hole,

play26:51

you get a second universe

play26:52

that has its own independent set of coordinates

play26:56

from our universe.

play26:57

I want to emphasize right, this is the simplest solution

play27:00

to the Einstein field equations,

play27:02

and it already contains a black hole,

play27:03

white hole and two universes.

play27:05

- [Derek] That's what you get

play27:07

when you push this map to its limits

play27:09

so that every edge ends at a singularity or infinity.

play27:13

- And in fact, there's another little feature in here,

play27:16

which is that, that little point there where they cross,

play27:19

that is an Einstein Rosen Bridge.

play27:24

- To see it, we need to change coordinates.

play27:27

Now this line is at constant crustal time

play27:30

and it connects the space of both universes.

play27:33

You can see what the spacetime is like

play27:35

by following this line from right to left.

play27:38

Far away from the event horizon,

play27:39

spacetime is basically flat,

play27:41

but as you get closer to the event horizon,

play27:43

spacetime starts to curve more and more.

play27:46

At this cross, you are at the event horizon,

play27:49

and if you go beyond it, you end up in the parallel universe

play27:53

that gives you a wormhole that looks like this.

play27:59

- So that is hypothetically how we could use a black hole

play28:04

to travel from one universe to another.

play28:06

- Hypothetically, because these wormholes

play28:08

aren't actually stable in time.

play28:11

- It's a bit like a bridge, but it's a bridge that is long

play28:14

and then becomes shorter and then becomes long again

play28:17

and if you try to traverse this bridge,

play28:19

at some point, the bridge is only very short, right?

play28:21

And you say, "Oh, well, let me just cross this bridge."

play28:23

But as you start crossing the bridge and start running,

play28:25

your speed is finite, right?

play28:27

The speed of light roughly and then the bridge starts,

play28:30

becoming stretching and you never come out the other side.

play28:35

- [Derek] This pinching off always happens too fast

play28:38

for anything to travel through.

play28:40

You can also see this if you look at the Penrose diagram,

play28:43

because when you're inside one universe,

play28:45

there isn't a light cone that can take you

play28:47

to the other universe.

play28:49

The only way to do that

play28:50

would be to travel faster than light,

play28:54

but there might be another way.

play28:57

Schwarzschild solution describes a black hole

play28:59

that doesn't rotate.

play29:00

Yet, every star does rotate

play29:02

and since angular momentum must be conserved,

play29:04

every black hole must also be rotating.

play29:08

While Schwarzschild found his solution within weeks

play29:10

after Einstein published his equations,

play29:12

solving them for a spinning mass

play29:14

turned out to be much harder.

play29:15

Physicists tried, but 10 years after Schwarzschild solution,

play29:19

they still hadn't solved it.

play29:21

10 years turned into 20, which turned into 40

play29:24

and then in 1963, Roy Kerr found the solution

play29:28

to Einstein's equations for a spinning black hole,

play29:32

which is far more complicated than Schwarzschild solution

play29:35

and this comes with a few dramatic changes.

play29:40

The first is that the structure is completely different.

play29:43

The black hole now consists of several layers.

play29:47

It's also not spherically symmetric anymore.

play29:50

This happens because the rotation

play29:52

causes it to bulge around the equator.

play29:54

So it's only symmetric about its axis of spin.

play29:59

Alessandro from science click simulated what happens

play30:02

around this spinning black hole.

play30:07

Space gets dragged around with the black hole

play30:10

taking you and the particles along with it.

play30:13

When you get closer, space gets dragged around

play30:15

faster and faster until it goes around faster

play30:19

than the speed of light,

play30:20

you've now entered into the first new region,

play30:24

the ergosphere.

play30:26

No matter how hard you fire your rockets here,

play30:29

it's impossible to stay still relative to distance stars,

play30:33

but because space doesn't flow directly inward,

play30:36

you can still escape the black hole.

play30:39

When you travel in further, you go through the next layer,

play30:42

the outer horizon, the point of no return.

play30:46

Here you can only go inwards,

play30:49

but as you get dragged in deeper and deeper,

play30:52

something crazy happens, you enter another region,

play30:57

one where you can move around freely again,

play31:00

so you're not doomed to the singularity.

play31:03

You're now inside the inner event horizon.

play31:07

Here you can actually see the singularity

play31:12

- In a normal black hole, it's a point,

play31:13

but it in a rotating black hole,

play31:14

it actually expands out to be a ring

play31:17

and there are weird things happened

play31:19

with spacetime inside the center of a black hole,

play31:22

a rotating black hole,

play31:23

but it's thought that you can actually

play31:24

fly through the singularity.

play31:29

- [Derek] We need a Penrose diagram

play31:31

of a spinning black hole, where before the singularity

play31:35

was a horizontal line at the top

play31:37

here, the singularity lifts up and moves to the sides,

play31:40

revealing this new region inside the inner horizon.

play31:45

Here we can move around freely and avoid the singularity,

play31:49

but these edges aren't at infinity or a singularity,

play31:53

so there must be something beyond them.

play31:55

Well, when you venture further,

play31:57

you could find yourself in a white hole,

play32:00

which would push you out into a whole nother universe.

play32:05

- You can have these pictures whereby

play32:08

you're in one universe, you fall into a rotating black hole,

play32:12

you fly through the singularity,

play32:14

and you pop out into a new universe from a white hole,

play32:18

and then you can just continue playing this game.

play32:21

- Extending this diagram infinitely far.

play32:25

but there is still one thing we haven't done,

play32:27

brave the singularity.

play32:30

So you aim straight towards the center of the ring

play32:33

and head off towards it, but rather than time ending,

play32:37

you now find yourself in universe, a strange universe,

play32:40

one where gravity pushes instead of pulls.

play32:44

This is known as an anti-verse.

play32:48

If that's too weird, you can always jump back

play32:50

across the singularity and return to a universe

play32:53

with normal gravity.

play32:55

- And I know this is basically science fiction, right?

play32:57

But if you take the solutions of relativity at,

play33:02

you know, essentially at face value and add on a little bit,

play33:05

which is what Penrose does here, he says this,

play33:07

"oh look, these shapes are very similar,

play33:10

I can just stick these together."

play33:12

Then this is the conclusion that you get.

play33:14

Now we have effectively an infinite number

play33:17

of universes all connected with black hole, white holes

play33:20

all the way through and you, of you go to explore,

play33:25

but it'll be a very brave person who's the first one

play33:28

who's gonna leap into a rotating black hole

play33:30

to find out if this is correct?

play33:31

(Derek chuckles)

play33:33

- Yeah, I would not sign up for that.

play33:35

So could these maximally extended Schwarzschild

play33:38

and Kerr solutions actually exist in nature?

play33:41

Well, there are some issues.

play33:43

Both the extended Schwarzschild and Kerr solutions

play33:46

are solutions of eternal black holes in an empty universe.

play33:50

- As you say, it's an eternal solution.

play33:52

So it stretches infinitely far into the past

play33:55

and infinitely far into the future

play33:57

and so there's no formation mechanism in there,

play33:59

it's just a static solution

play34:02

and I think that is part of the,

play34:07

part of the reason why black holes

play34:10

are realized in our universe and white holes aren't-

play34:15

- Or might not be.

play34:16

- Or might not be,

play34:16

or I'm reasonably I,

play34:18

personally, I'm reasonably confident

play34:20

that they don't exist, right?

play34:22

- [Derek] For the maximally extended Kerr solution,

play34:24

there's also another problem.

play34:26

If you're an immortal astronaut inside the universe,

play34:28

you can send light into the black hole,

play34:31

but because there's infinite time compressed

play34:34

in this top corner, you can pile up light along this edge,

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which creates an infinite flux of energy

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along the inner horizon.

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This concentration of energy

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then creates its own singularity,

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sealing off the ring singularity and beyond.

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- My suspicion and the suspicion

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of some other people in the field is that

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this inner horizon will become singular

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and you will not be able to go through these second copies.

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- So all the white holes, wormholes, other universes

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and anti universes disappear.

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Does that mean that real wormholes are impossible?

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In 1987, Michael Morris and Kip Thorne looked at wormholes

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that an advanced civilization could use

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for interstellar travel, ones that have no horizons,

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so you can travel back and forth, are stable in time,

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and have some other properties like

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being able to construct them.

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They found several geometries that are allowed

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by Einstein's general relativity.

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In theory, these could connect different parts

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of the universe, making a sort of interstellar highway.

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They might even be able to connect to different universes.

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The only problem is that all these geometries

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require an exotic kind of matter

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with a negative energy density

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to prevent the wormhole from collapsing.

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- This exotic kind of matter,

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is really against the loss of physics, so it's,

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I have the prejudice that it will not exist.

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I'm bothered by the fact that we say that

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the science fiction wormholes are mathematically possible.

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It's true, it's mathematically possible

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in the sense that there's some geometry that can exist,

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but Einstein's theory is not just geometries,

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it's geometries plus field equations.

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If you use the kinds of properties of matter

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that matter actually has, then they're not possible.

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So I feel that the reason they're not possible

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is very strong.

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- So according to our current best understanding,

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it seems likely that white holes, traversable wormholes,

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and these parallel universes don't exist,

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but we also used to think that black holes didn't exist.

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So maybe we'll be surprised again.

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- I mean, we have one universe, right?

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Good, why can't we have two.

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(whimsical music)

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Related Tags
Black HolesWhite HolesWormholesGeneral RelativitySpacetimeEinsteinAstronomySingularityCosmologySci-Fi