Bending of Space: What, Why, Where, When?

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Discussion Overview

The discussion revolves around the concept of the bending of space, exploring its meaning, implications, and the nature of curvature in both three-dimensional and higher-dimensional contexts. Participants examine theoretical aspects, analogies, and mathematical descriptions related to the bending of space, particularly in relation to gravity and light trajectories.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question the terminology of "bending" and suggest that it may refer more accurately to changes in geometry or intrinsic curvature rather than a literal bending in a higher dimension.
  • One participant describes how light follows the curvature of space near massive objects, which is often referred to as space bending.
  • Another participant introduces an analogy involving a string and the circumference of a circle to illustrate intrinsic curvature, emphasizing that curvature can be understood without invoking higher dimensions.
  • There is a discussion about how intrinsic curvature allows a space to "know" its own properties without external measurements, with some participants providing mathematical formulations to support their points.
  • An analogy involving a ball on a rubber sheet is mentioned as a visualization tool for understanding spatial curvature around massive bodies.
  • One participant proposes a rope analogy to assess curvature based on the relationship between coordinates, questioning the necessity of space for light to bend.

Areas of Agreement / Disagreement

Participants express differing views on the nature of space bending, with some advocating for intrinsic curvature concepts while others maintain that a higher-dimensional perspective is necessary. The discussion remains unresolved, with multiple competing views present.

Contextual Notes

Participants reference various mathematical formulations and analogies, indicating that the understanding of curvature may depend on specific definitions and contexts. Some assumptions about dimensionality and the nature of space are not fully explored.

jobyts
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What exactly is bending of space? Does space bend from position x to position y? If so, what do we call whatever is there in position x (after the bend)? And what was there at position y, before the bend?
 
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jobyts said:
What exactly is bending of space? Does space bend from position x to position y? If so, what do we call whatever is there in position x (after the bend)? And what was there at position y, before the bend?

Hi jobyts! :smile:

Three-dimensional space isn't part of a four-dimensional space.

It doesn't "bend" in or through a fourth dimension … it only changes its own geometry (curvature).
 
tiny-tim said:
Hi jobyts! :smile:

Three-dimensional space isn't part of a four-dimensional space.

It doesn't "bend" in or through a fourth dimension … it only changes its own geometry (curvature).

If I understand you, in a 3D world, it looks like bending, but what actually happening is a change in geometry in the 4-D space. Please correct if I'm wrong.
 
jobyts said:
If I understand you, in a 3D world, it looks like bending, but what actually happening is a change in geometry in the 4-D space. Please correct if I'm wrong.

No, what is actually happening is a change in geometry in the 3-D space.

There is no 4-D space.
 
Hi there,

An example might actually enlighten you on this subject.

Everyone knows that light (photons) travel in a straight line. Ok, nothing so bad up to now. If this light would pass next to a very massive object (super massive star or black hole), the gravitational pull of this object would also affect the light ray trajectory. Therefore, we call it space bending, just because light follows the curvature of space.

Hope this helps a bit. Cheers
 
jobyts said:
What exactly is bending of space? Does space bend from position x to position y? If so, what do we call whatever is there in position x (after the bend)? And what was there at position y, before the bend?

"Bending" is the wrong word, as it usually refers to extrinsic curvature. Intrinsic curvature is a distortion of distances: Imagine you fix one end of a string with the length R at a point in 2d-space, and make a full circle with the other end. If you then find that the circumference of that circle is different from 2*PI*R, you conclude that the 2d-space is curved intrinsically. So you don't need extra dimensions to quantify that curvature. You can extend this example to curved 3d-space containing a sphere with the radius R and a surface area different from 4*PI*R^2.

You can also embed a intrinsically curved manifold into a flat higher dimensional manifold to visualize the distorted distances:
http://www.physics.ucla.edu/demoweb..._and_general_relativity/curved_spacetime.html
 
A.T. said:
"Bending" is the wrong word, as it usually refers to extrinsic curvature. Intrinsic curvature is a distortion of distances: Imagine you fix one end of a string with the length R at a point in 2d-space, and make a full circle with the other end. If you then find that the circumference of that circle is different from 2*PI*R, you conclude that the 2d-space is curved intrinsically. So you don't need extra dimensions to quantify that curvature. You can extend this example to curved 3d-space containing a sphere with the radius R and a surface area different from 4*PI*R^2.

You can also embed a intrinsically curved manifold into a flat higher dimensional manifold to visualize the distorted distances:
http://www.physics.ucla.edu/demoweb..._and_general_relativity/curved_spacetime.html

Think I'm missing something here, would that not still be only possible if the 2d space was "bend" in the 3rd dimension. Otherwise, how can the space "know" it's curved/distorted?
 
Teeril said:
Think I'm missing something here, would that not still be only possible if the 2d space was "bend" in the 3rd dimension. Otherwise, how can the space "know" it's curved/distorted?

Hi Teeril! :smile:

It "knows" it's curved/distorted because it uses its own ruler and finds that (for example) the ratio circumference/diameter of a circle is not π.

Curvature is an intrinsic property of a space …

that means that no outside measurement is required …

the space itself "knows" about its own curvature. :wink:
 
Teeril,
you need some maths to understand intrinsic curvature. You know from that in a 3d Euclidean space the change in distance between two points is given by
ds^2=dx^2+dy^2+dz^2, coordinates are x,y,z.
This is a 'flat' space because the dx^2, dy^2 and dz^2 terms have coefficients that are independent of position. The distances on the surface of a sphere are given by
ds^2=r^2\sin^2(\theta)d\phi^2+r^2d\theta^2, coordinates phi and theta ( r is constant). This 2D space is curved.

As A.T. has said, it's because of distorted distances.
 
  • #10
For the bending of space only, the old analogy of the ball on a rubber sheet works fairly well. In fact, if only consider motion in a plane, the curvature of space around a spherically symmetric, stationary body can be visualized as a Flamm paraboloid embedded in 3 space.

http://en.wikipedia.org/wiki/Schwarzschild_metric#Flamm.27s_paraboloid

This can be used to compute the spatial contribution to the precession of the perihelion of Mercury. Rindler's book does a good job describing this.

The curvature of time contributes the other half to the bending.
 
Last edited:
  • #11
This is my analogy. Please tell me if it makes any sense.

Let's say, I have a rope of known length l and both the end's co-ordinates (x1, y1, z1) and (x2, y2, z2). With co-ordinate (x1, y1, z1) as the center and radius l, I construct a sphere. If the co-ordinate (x2, y2, z2) is part of the sphere, I can confirm the rope is not curved. If not, the rope is curved. (the (x2, y2, z2) must be always inside the sphere; I cannot think of a possibility (x2, y2, z2) is outside the sphere).

What I do not understand, why light has to bend if there's no space?
 

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