Where was I?
No problem with opposite charge. But you've heard me refer to chirality and topological quantum field theory, which relates to knots. You can tie your shoelaces left-over right to create a knot. Then on the other shoe you can tie your shoelaces right-over left to create an opposite knot. It's a "mirror image" knot, with the opposite chirality, but it isn't really a negative knot.There is no convention I'm aware of in which you can avoid considering some charges as negative. That we take the proton to have positive charge and the electron negative is indeed arbitrary, but that we take them to have opposite signs is not.
As I said the other day, I was referring to curvature in an electromagnetic context, as per Percy Hammond.ctamblyn said:You're talking about extrinsic curvature. The intrinsic curvature of both bent rods is zero (assuming you mean to treat them as one-dimensional manifolds).
Yes we know about this. You can draw a Euclidean triangle on a flat sheet of paper and roll the paper up into a cylinder without deforming the triangle. However the universe is not a sheet.ctamblyn said:1D surfaces are fundamentally different to higher-dimensional surfaces - they are always intrinsically flat. When you go up to 2D, things get more interesting. See the following:
Left to right: Hyperboloid of one sheet, cylinder, and sphere.
[qimg]http://upload.wikimedia.org/wikipedia/commons/4/4a/Gaussian_curvature.PNG[/qimg]
The Gaussian (intrinsic) curvature can be negative (like a hyperboloid of one sheet), zero (like a cylinder) or positive (like a sphere), and there are important qualitative differences between the those cases.
Sure they're opposite. But there's no evidence for any such curvature in the universe. The evidence suggests it isn't curved at all. That squares with my understanding of relativity. What doesn't, is the non-sequitur assertion that the universe must be curved, and that the radius of curvature must be huge.ctamblyn said:Triangles formed from geodesics give the best-known illustration: for a space of negative curvature the internal angles have a sum less than two right-angles, while for a space of positive curvature the sum is greater. To some extent it is conventional which type of space you call negatively-curved and which you call positively-curved, but that they are oppositely-signed holds for any useful definition of intrinsic curvature.