- #1
Haorong Wu
- 418
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- TL;DR Summary
- This basic concept in GR has always confused me. I am not sure is my understanding correct.
I imagine there is a isotropic space. Well, I would call it the proper space which will remain unchanged in any cases. And there is another space I call the coordinate space which will be distorted by gravitational field, i.e., metric.
a) Suppose there are two stationary points. Their coordinates will be given in the coordinate space. No matter what kind of gravitational field is imposed on them, their coordinate will remain unchanged. However, due to the metric, their projection to the proper space will be altered. So the proper length between them will be affected by the metric.
b) Consider a light path. Suppose a beam propagates along z axis in the coordinate space. Then it will remain on it. However, due to the gravitational field, the projection of z axis to the proper system may be a curve, so the light actually travel along a curve.
So could I treat the metric like some projection operation from the coordinate space to the proper space?
a) Suppose there are two stationary points. Their coordinates will be given in the coordinate space. No matter what kind of gravitational field is imposed on them, their coordinate will remain unchanged. However, due to the metric, their projection to the proper space will be altered. So the proper length between them will be affected by the metric.
b) Consider a light path. Suppose a beam propagates along z axis in the coordinate space. Then it will remain on it. However, due to the gravitational field, the projection of z axis to the proper system may be a curve, so the light actually travel along a curve.
So could I treat the metric like some projection operation from the coordinate space to the proper space?