Is curvature possible for a 2D metric?

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    2d Curvature Metric
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Discussion Overview

The discussion centers on the possibility of curvature in a two-dimensional metric, specifically examining the properties of the Riemann tensor in 2D spaces. Participants explore theoretical implications, examples, and the nature of curvature in both intrinsic and extrinsic contexts.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that a 2D coordinate system inherently implies flat space, as seen in their derivation of the Riemann tensor yielding zero elements.
  • Others argue that a 2-dimensional manifold, such as a sphere, can exhibit non-zero Riemann curvature, challenging the notion that 2D must be flat.
  • A participant highlights that the Riemann tensor in 2D has four non-zero components, indicating that intrinsic curvature can exist in such spaces.
  • Another participant provides a formula for the Riemann tensor in 2D, suggesting that it can represent varying Gaussian curvature.
  • Some contributions discuss the relationship between curvature and geometric properties, such as the sum of angles in triangles on different surfaces.
  • There is a distinction made between intrinsic curvature and extrinsic curvature, with some participants noting that a 1D curve can only exhibit extrinsic curvature.
  • Participants also explore the implications of curvature in higher dimensions and how it relates to the understanding of 2D spaces.

Areas of Agreement / Disagreement

Participants do not reach a consensus; multiple competing views remain regarding the nature of curvature in 2D metrics, particularly concerning the relationship between curvature and the dimensionality of the space.

Contextual Notes

Some participants reference specific mathematical properties and definitions, indicating that the discussion may depend on particular assumptions about the nature of curvature and the definitions used in different contexts.

  • #31
mal4mac said:
Isn't there still a way to tell the difference? Couldn't an inhabitant of the cylinder walk round the cylinder and get back home? The inhabitant on the infinite plane would never get back home.

How would he know he had gotten back at home, if absolutely everything repeated periodically? He would walk a certain distance and find a house that is exactly like his in every way. Is it his house, or an exact copy?

What I said was that there is no observable difference between Situation A: The universe is an infinite 2D plane in which absolutely everything repeats at regular intervals in one specific direction. Situation B: The universe is a cylinder.
 
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  • #32
stevendaryl said:
How would he know he had gotten back at home, if absolutely everything repeated periodically? He would walk a certain distance and find a house that is exactly like his in every way. Is it his house, or an exact copy?

In reality it could hardly be an exact copy, so your example only holds for a very simple universe, one without life.
 
  • #33
mal4mac said:
In reality it could hardly be an exact copy, so your example only holds for a very simple universe, one without life.

What does "could hardly be an exact copy" mean in mathematics? Periodicity doesn't distinguish whether it's a copy or the same object. Perfect crystal structure is an example to that...
The main point is in Steven's post#30
 
  • #34
A.T. said:
You cannot roll out a common doughnut surface onto a flat plane without any stretching/squeezing. But if the radius of revolution goes to infinity, while the radius of the tube stays constant the intrinsic curvature goes to zero.

Related video presenting another method:

 
  • #35
A.T. said:
For the cylinder it's simple to visualize: You can roll it out onto a flat plane without any stretching/squeezing (no change of the intrinsic distances).

But for a torus it's less obvious: You cannot roll out a common doughnut surface onto a flat plane without any stretching/squeezing. But if the radius of revolution goes to infinity, while the radius of the tube stays constant the intrinsic curvature goes to zero.
The key point here is that while a surface with the topology of a torus does not require curvature, it may have curvature (just as bumps on plane leave the topology unchanged, but add curvature). The follow on point is that any torus embedded in Euclidean 3-space has curvature. However, a torus without curvature can be embedded in Euclidean 4-space. This is similar to the limitation that a Klein bottle (a non-orientable analog of a torus) can only be embedded in Euclidean 4-space not Euclidean 3-space.

[Edit: seeing AT's last post, I am referring to smooth embeddings; curvature is preserved at every point, among other things. Nash also proved a theorem related to the one described in the video on smooth embeddings, that any conceivable manifold can be smoothly embedded in some higher dimensional Euclidean manifold.}
 
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