Can Geodesic Deviation in Spacetime Incorporate Non-Causal Relationships?

m4r35n357
Messages
657
Reaction score
148
I've been meaning to ask this for some time, and now I've plucked up the courage! It is puzzling to me that many fundamental relationships in GR are explained in terms of euclidean space. Taking for example the geodesic deviation equation, it occurs to me that if defined in 3+1 spacetime there is at least the possibility that u, v or w could represent something non-causal. What is the basic argument for translating Riemannian concepts to pseudo-Reimannian situations? Is there a sense that we could bake causality into things like geodesic deviation, or is this a non-issue? I don't recall seeing this issue discussed in any of my other investigations . . .
 
Physics news on Phys.org
It's a non-issue. There is certainly nothing non-causal present. We simply have a congruence of time-like geodesics with some associated 4-velocity field and we Lie transport a space-like vector field along this 4-velocity field in order to define infinitesimal spatial displacements between neighboring observers of the geodesic congruence. We then look at the second covariant derivative of this space-like vector field along the geodesic congruence and from that we get the geodesic deviation equation which just measures the second order rate of change of the infinitesimal spatial displacements between the neighboring observers of the congruence. It's a completely local equation.
 
OK, so this has bugged me for a while about the equivalence principle and the black hole information paradox. If black holes "evaporate" via Hawking radiation, then they cannot exist forever. So, from my external perspective, watching the person fall in, they slow down, freeze, and redshift to "nothing," but never cross the event horizon. Does the equivalence principle say my perspective is valid? If it does, is it possible that that person really never crossed the event horizon? The...
In this video I can see a person walking around lines of curvature on a sphere with an arrow strapped to his waist. His task is to keep the arrow pointed in the same direction How does he do this ? Does he use a reference point like the stars? (that only move very slowly) If that is how he keeps the arrow pointing in the same direction, is that equivalent to saying that he orients the arrow wrt the 3d space that the sphere is embedded in? So ,although one refers to intrinsic curvature...
ASSUMPTIONS 1. Two identical clocks A and B in the same inertial frame are stationary relative to each other a fixed distance L apart. Time passes at the same rate for both. 2. Both clocks are able to send/receive light signals and to write/read the send/receive times into signals. 3. The speed of light is anisotropic. METHOD 1. At time t[A1] and time t[B1], clock A sends a light signal to clock B. The clock B time is unknown to A. 2. Clock B receives the signal from A at time t[B2] and...
Back
Top