The Maths of General Relativity (3/8) - Geodesics

ScienceClic English
8 Dec 202007:26

Summary

TLDRThis episode of Science Clique explores the mathematics of general relativity through the concept of geodesics. It explains how objects in the universe naturally follow the straightest possible paths, or geodesics, when no external forces are applied. The video delves into the evolution of an object's velocity over time, using the geodesic equation to predict an object's trajectory. It introduces Christoffel symbols, which are crucial for understanding how coordinates behave in the presence of a grid's structure. The analogy of an airplane's flight over the Earth's curved surface illustrates the concept of geodesics and the impact of coordinate systems on perceived motion.

Takeaways

  • 🌌 The video discusses the mathematics of general relativity, focusing on the concept of geodesics.
  • πŸ“ In the absence of external forces, objects in the universe naturally move in straight lines, which are represented as geodesics in spacetime.
  • ⏱️ The evolution of an object's velocity over proper time can predict its trajectory, with the velocity vector remaining constant along the geodesic.
  • πŸ”„ The concept of a geodesic is introduced as the natural path an object follows, which is a straight line in the context of spacetime.
  • 🧭 The velocity vector's derivative with respect to proper time is zero along the geodesic, indicating no acceleration.
  • πŸ“ The velocity vector can be decomposed into components and basis vectors, which can change due to the choice of coordinate system.
  • 🌐 The basis vectors' variation along the trajectory is influenced by the grid or coordinate system used, which can be irregular.
  • πŸ”’ The rate of change of the basis vectors is described by the Christoffel symbols, which are crucial for general relativity as they encode the grid's structure.
  • 🌍 The video uses the Earth's surface with latitude and longitude coordinates as an analogy to explain how geodesics can appear curved due to the coordinate system used.
  • ✈️ An airplane flying in a straight line along a great circle on Earth is given as an example of a geodesic, where the trajectory appears curved on a grid but is actually straight.

Q & A

  • What is the concept of a geodesic in the context of general relativity?

    -A geodesic in general relativity is the natural path that a point mass moves along in spacetime, which is the shortest path between two points in a curved spacetime. It represents the trajectory that an object follows when no force is applied to it.

  • Why do objects in the universe tend to move in straight lines when no force is applied?

    -Objects in the universe tend to move in straight lines when no force is applied due to the symmetry of spacetime. There is no reason for the object to turn one way or the other, so it follows the path of least resistance, which is a straight line in the absence of external influences.

  • What is the significance of the velocity vector in describing the motion of an object?

    -The velocity vector is significant in describing the motion of an object because it indicates the direction and speed at which the object moves through spacetime. It is a fundamental quantity used to predict the trajectory of an object as proper time passes.

  • How does the concept of proper time relate to the motion of objects in spacetime?

    -Proper time is the time measured by a clock moving with an object, and it is the parameter used to describe the motion of objects in spacetime. The evolution of an object's velocity vector is described as proper time passes, allowing for the prediction of the object's trajectory.

  • What is the role of basis vectors in the geodesic equation?

    -Basis vectors play a crucial role in the geodesic equation as they form the coordinate system within which the motion of objects is described. They help in expressing the velocity vector and its components, which are essential for understanding the trajectory of an object.

  • Why do basis vectors change along the trajectory in an irregular coordinate system?

    -Basis vectors change along the trajectory in an irregular coordinate system because the grid or coordinate system itself can be irregular. This means that the basis vectors' components can vary as the object moves through spacetime.

  • What are Christoffel symbols and how are they used in the geodesic equation?

    -Christoffel symbols, denoted by the capital Greek letter gamma (Ξ“), are quantities that encode how a coordinate grid changes along different directions. They are used in the geodesic equation to express the rate of change of the velocity vector components as proper time passes.

  • How does the geodesic equation help in predicting the trajectory of an object?

    -The geodesic equation helps in predicting the trajectory of an object by providing a mathematical framework to calculate the rate of change of each component of the velocity vector as proper time passes. This allows for the prediction of the object's path throughout spacetime.

  • What is the example used in the script to illustrate the concept of geodesics?

    -The script uses the example of an airplane flying on the surface of the Earth, using a latitude-longitude coordinate system. The airplane's trajectory forms a great circle, which is a geodesic, and it demonstrates how a straight path can appear curved when plotted on a grid that does not correspond to straight lines on a sphere.

  • Why does the airplane's trajectory appear curved when plotted on a latitude-longitude coordinate system?

    -The airplane's trajectory appears curved on a latitude-longitude coordinate system because the Earth's surface is a sphere, and the grid of latitude and longitude lines does not represent straight lines on a spherical surface. The geodesic, or the shortest path, appears as a great circle, which is a curve on the surface of the Earth.

  • What do the Christoffel symbols measure in the context of the Earth's surface analogy?

    -In the context of the Earth's surface analogy, the Christoffel symbols measure the extent to which the coordinates deviate from straight lines along the grid. They indicate how the basis vectors change as they are transported along the grid, which is essential for understanding the curvature of the Earth's surface.

Outlines

00:00

🌌 Understanding Geodesics in General Relativity

This paragraph introduces the concept of geodesics in the context of general relativity. It explains that in the absence of external forces, objects in the universe naturally move in straight lines, which are represented as geodesics in the fabric of spacetime. The paragraph discusses how the velocity vector of an object remains constant along its geodesic path, implying that there is no acceleration. It further elaborates on how the basis vectors, which define the coordinate system, can change along the trajectory due to the curvature of spacetime. The christoffel symbols are introduced as a means to quantify how these basis vectors change, which is crucial for understanding the behavior of objects in a gravitational field. The geodesic equation is mentioned as a fundamental tool for predicting the trajectory of objects through spacetime.

05:00

🌍 Geodesics on the Earth's Surface

The second paragraph uses the analogy of the Earth's surface to illustrate the concept of geodesics. It describes how an airplane flying in a straight line follows a great circle route, which is a geodesic on the Earth's surface. The paragraph explains that while the airplane's velocity vector remains constant, the trajectory appears curved when plotted on a latitude-longitude coordinate system due to the spherical shape of the Earth. The christoffel symbols are again discussed, but this time in the context of how they measure the deviation of coordinates from straight lines on a curved surface. The paragraph concludes by emphasizing that the christoffel symbols are essential for understanding the behavior of coordinates and the underlying geometry of spacetime.

Mindmap

Keywords

πŸ’‘General Relativity

General Relativity is a theory of gravitation developed by Albert Einstein, published in 1915. It is the current description of gravity as a geometric property of spacetime caused by the uneven distribution of mass. In the video, General Relativity is the overarching framework for understanding how objects move through spacetime, particularly in the context of geodesics.

πŸ’‘Geodesics

A geodesic is the shortest path between two points in a curved space, such as a great circle on the Earth's surface. In the context of General Relativity, geodesics describe the natural path that a freely moving object will take through spacetime. The video explains that all objects in the universe tend to follow geodesics, which are straight lines in the absence of external forces.

πŸ’‘Proper Time

Proper time is the time measured by a clock moving along with an object, which is the time experienced by that object. It is used to describe the aging of an object under the influence of gravity or acceleration. In the video, the evolution of an object's velocity is described as it passes through proper time, which is key to predicting the object's trajectory.

πŸ’‘Velocity Vector

The velocity vector is a mathematical representation of an object's velocity, indicating both the speed and direction of the object's motion. In the video, the velocity vector is used to describe how an object moves through spacetime, and its constancy along a geodesic implies that the object is in free-fall, experiencing no acceleration.

πŸ’‘Symmetry

Symmetry in physics often refers to the invariance of physical laws under certain transformations. In the video, the concept of symmetry is used to explain why, in the absence of forces, an object's world line through spacetime tends to be straight, as there is no reason for it to deviate from a straight path.

πŸ’‘Basis Vectors

Basis vectors are the fundamental vectors that define a coordinate system. They are used to express any vector in terms of the coordinate system. In the video, basis vectors are used to decompose the velocity vector and to understand how the components of the velocity vector change as the object moves through spacetime.

πŸ’‘Christoffel Symbols

Christoffel symbols, denoted by the Greek letter gamma (Ξ“), are mathematical objects that encode the rate of change of the basis vectors of a coordinate system. They are crucial in General Relativity for describing how the coordinates of spacetime are curved. The video explains that these symbols are essential for understanding how the grid or coordinate system changes along with the object's trajectory.

πŸ’‘Coordinate System

A coordinate system is a method of specifying points in space by using numbers, often in a grid-like structure. In the video, the coordinate system is used to describe how basis vectors and their changes can be measured, and how these changes relate to the motion of objects along geodesics.

πŸ’‘Non-accelerating

Non-accelerating motion refers to the movement of an object where its velocity does not change over time. In the video, it is mentioned that objects in free-fall follow geodesics and experience non-accelerating motion, meaning their velocity vector does not change direction or magnitude as they move through spacetime.

πŸ’‘Derivative

The derivative in mathematics is a measure of how a function changes as its input changes. In the context of the video, derivatives are used to describe the rate of change of the velocity vector with respect to proper time and how the basis vectors change along the trajectory of an object.

πŸ’‘Great Circle

A great circle is the largest circle that can be drawn on the surface of a sphere, such as the Earth. In the video, the concept of a great circle is used as an analogy to explain geodesics. An airplane flying in a straight line along a great circle is following a geodesic, even though its path appears curved when plotted on a two-dimensional map.

Highlights

Exploring the mathematics of general relativity through the concept of geodesics.

Defining world lines and the motion of objects as proper time progresses.

Understanding velocity as a directional indicator through space-time.

Describing the evolution of velocity to predict the trajectory shape in the universe.

Objects naturally move in straight lines when no force is applied, forming straight world lines.

The concept of geodesics as the natural trajectory formed by transporting velocity along itself.

In a geodesic, the velocity vector does not turn, indicating non-accelerating natural movement.

Deriving the relationship between the change in velocity components and basis vectors.

Basis vectors can vary due to the irregularity of the chosen coordinate system.

Evolution of a basis vector along the world line and its decomposition into coordinate components.

Introducing the new quantity that indicates how the basis vector varies along a coordinate.

The importance of the vector derivative of the basis vector with respect to a coordinate.

Defining Christoffel symbols and their role in general relativity.

Christoffel symbols encode how the grid changes and provide information on coordinate behavior.

Formulating the geodesic equation using Christoffel symbols to predict object trajectories.

Illustrating the concept of geodesics using the surface of the Earth and a latitude-longitude coordinate system.

The geodesic trajectory of an airplane moving in a straight line forms a great circle around the Earth.

Christoffel symbols measure the deviation of coordinates from straight lines on a spherical grid.

Transcripts

play00:01

[Music]

play00:05

welcome back to science clique

play00:07

today the mathematics of general

play00:09

relativity

play00:10

part 3 geodesics

play00:16

in the previous videos we have defined

play00:18

the concepts of world lines

play00:20

motion as proper time goes by and

play00:23

velocity

play00:24

which indicates the direction in which

play00:26

an object moves through space and time

play00:31

we would now like to describe the

play00:33

evolution of this velocity

play00:34

as proper time passes in order to

play00:37

predict the shape of the trajectory

play00:41

in our universe objects naturally move

play00:43

in straight lines

play00:45

when no force is applied world lines

play00:48

tend to be straight

play00:49

through the dimensions of space and time

play00:56

this comes from the symmetry of such

play00:59

trajectory

play01:00

an object has no reason to turn one way

play01:02

or the other

play01:05

this simple consideration gives us a

play01:07

method to predict the trajectory of a

play01:09

body

play01:10

as soon as we know its velocity at a

play01:12

given instant we can just transport the

play01:14

arrow along

play01:15

itself to gradually predict the movement

play01:18

of the object

play01:19

this type of trajectory which is formed

play01:21

by transporting velocity along itself

play01:24

is called a geodesic

play01:26

[Music]

play01:28

in the universe all objects tend to

play01:30

follow geodesics

play01:35

on a geodesic the vector does not turn

play01:38

we can thus write that its derivative

play01:40

with respect to proper time

play01:42

is zero along the trajectory

play01:46

the velocity vector of the apple does

play01:48

not vary

play01:51

this equation simply says that the

play01:53

natural movement of bodies

play01:54

is non-accelerating and therefore that

play01:57

when they experience no

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force objects tend to move straight

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ahead

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but we saw previously that the velocity

play02:07

vector can be written as the sum of its

play02:09

components

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multiplied by the basis vectors

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[Music]

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using this expression and knowing that

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the derivative of a product

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is the sum of each term multiplied by

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the derivative of the other term

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we obtain a relation between on one side

play02:28

the change in the components of the

play02:30

velocity

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and on the other side the change in the

play02:33

basis vectors themselves

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the basis vectors can indeed vary

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throughout the trajectory

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because the grid that we choose as our

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coordinate system can very well be

play02:45

irregular

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although the vector remains the same as

play02:51

a geometric object

play02:53

its components on the grid can vary as

play02:56

the apple moves

play03:08

when we think about it the evolution of

play03:10

a basis vector along the world line

play03:12

can be decomposed as the sum of its

play03:15

evolution

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along each of the two coordinates

play03:19

multiplied by the speed of the apple

play03:22

because the faster the apple moves

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the faster the basis vector will vary

play03:27

[Music]

play03:29

for each coordinate this gives us a new

play03:32

quantity

play03:33

which indicates how the basis vector

play03:35

varies along the coordinate

play03:38

this variation is expressed as a vector

play03:41

that is the derivative of the basis

play03:43

vector with respect to the coordinate in

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question

play03:48

this vector is very interesting because

play03:50

it no longer depends on the trajectory

play03:53

but only on the structure of the grid

play03:55

itself

play03:58

this vector can be expressed through its

play04:00

components

play04:01

denoted by the capital letter gamma

play04:08

in our two-dimensional case these

play04:10

components

play04:11

exist in eight different versions two

play04:13

components

play04:14

for four different vectors these numbers

play04:17

are called christopher symbols the

play04:20

christopher symbols are essential

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quantities for general relativity

play04:24

because they encode how the grid changes

play04:27

along each

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direction they contain crucial

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information

play04:31

on how our coordinates behave

play04:34

[Music]

play04:39

rewriting the previous equation using

play04:41

christopher symbols

play04:44

we finally get to the geodesic equation

play04:49

this very important equation allows us

play04:52

to calculate for

play04:53

each component of the velocity its rate

play04:56

of change

play04:56

as proper time passes

play05:00

the geodesic equation thus allows us to

play05:02

predict the whole trajectory of an

play05:04

object

play05:05

as long as we know its velocity at a

play05:07

given moment

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and the value of each christopher symbol

play05:11

all throughout the grid

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to illustrate all these ideas let's

play05:24

imagine not a space-time

play05:26

but simply the surface of the earth

play05:29

we decide to use a latitude longitude

play05:31

coordinate system

play05:33

which at first glance seems to be a very

play05:35

good fit for the geometry

play05:39

now imagine that an airplane is moving

play05:41

in a straight line

play05:44

when an object moves straight ahead

play05:45

without ever turning

play05:47

its trajectory forms what is called a

play05:50

geodesic

play05:52

in our situation the geodesic is a great

play05:55

circle around the planet

play05:58

on this geodesic trajectory the airplane

play06:00

is always moving straight ahead

play06:03

its velocity vector does not change

play06:05

orientation

play06:08

but when we plot the coordinates the

play06:11

trajectory seems

play06:12

curved the airplane seems to change

play06:15

orientation along the grid

play06:18

in reality its trajectory is perfectly

play06:20

straight

play06:21

the problem does not come from the

play06:23

airplane but from our grid

play06:25

it's our coordinates that are curved

play06:28

their axes do not correspond

play06:30

to straight lines on a sphere compared

play06:34

to real straight lines

play06:35

geodesics they turn

play06:40

starting from a basis vector and

play06:42

transporting it along the grid

play06:44

we can measure how much this vector

play06:46

changes by another vector

play06:49

it's the components of this vector that

play06:52

are called christophel symbols

play06:55

the christopher symbols measure the

play06:57

extent to which our coordinates deviate

play07:00

from straight lines

play07:01

along the grid

play07:18

[Music]

play07:26

you

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Related Tags
General RelativityGeodesicsSpace-TimePhysicsVelocityTrajectoryChristoffel SymbolsCoordinate SystemMathematicsScience Education