Doing General Relativity with Cartesian coordinates?

In summary, there is a way to do general relativity without using complicated mathematics by using 5-dimensional Euclidean space and constraining it to only points on a 4-dimensional curved hypersurface. This concept is described in George Jones's post and further explained in Marolf's paper. However, the practicality of this approach is questionable as it may still require messy calculations. It is a useful conceptual tool for those familiar with special relativity.
  • #1
kochanskij
44
4
Is it possible to do general relativity but avoid the difficult mathematics of generalized coordinates, tensors, and computing the metric of a space-time manifold by using ordinary cartesian coordinates in a 5 dimensional space?

We can picture a curved 4 dimensional spacetime as being embedded in a Euclidean 5 dimensional space. Cartesian retangular coordinates would work in this Euclidean space. Then you could add a constraint that only points in that 5-D space that fall on the 4-D curved "hypersurface" are allowed.
 
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  • #3
If you have a basic knowledge of SR, there are a few educational papers that describe how you can draw Lorentzian space-time diagrams on a 3D surface to model part of the space-time around a massive nonrotating body (specifically, the R-T plane of Schwarzschild solution to a black hole).

See for instance Marolf's paper at http://arxiv.org/abs/gr-qc/9806123

To actually get any qunatitative results out of this, though, will be messy. Having the embedding diagram doesn't really make it much simpler to calculate geodesic curves, for instance.

The idea is that you just have to draw the normal space-time diagrams of SR on the surface of a curved sheet of paper rather than a flat one is somewhat useful conceptually, though.

This particular embedding isn't a euclidian one, though - if you look at a small, flat piece of the curved paper, the space-time diagram on that flat piece transforms via the Lorentz transform, so it will only be useful to people who understand SR well enough to know what that means.

NOt quite what you asked for, but you might find it interesting.
 

1. What are Cartesian coordinates and how are they used in general relativity?

Cartesian coordinates are a system of three perpendicular axes (x, y, and z) used to describe the position of a point in three-dimensional space. In general relativity, they are often used to describe the geometry of a curved spacetime, where the axes represent the three dimensions of space and time is treated as a fourth dimension.

2. Can Cartesian coordinates be used to describe curved spacetime?

Yes, Cartesian coordinates can be used to describe curved spacetime, but only in a local sense. This means that within a small region of spacetime, the geometry can be approximated as flat and Cartesian coordinates can be used. However, on a larger scale, the curvature of spacetime must be taken into account.

3. How are the laws of physics affected by using Cartesian coordinates in general relativity?

The laws of physics, including the equations of general relativity, are independent of the choice of coordinates. However, using Cartesian coordinates can make the mathematics simpler and more intuitive, especially when working with flat spacetime.

4. What are the limitations of using Cartesian coordinates in general relativity?

Cartesian coordinates have limitations when describing highly curved or non-Euclidean spacetimes, such as those near black holes or in the presence of strong gravitational fields. In these cases, alternative coordinate systems, such as polar coordinates or curved coordinates, may be more appropriate.

5. How do Cartesian coordinates relate to other coordinate systems used in general relativity?

Cartesian coordinates are just one of many coordinate systems used in general relativity. Other common coordinate systems include spherical coordinates, cylindrical coordinates, and Boyer-Lindquist coordinates. Each coordinate system has its own advantages and limitations, and the choice of which to use depends on the specific problem at hand.

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