I EM Force vs. Gravity: Modeling Spatio-Temporal Curvature

Ontophobe
Messages
60
Reaction score
1
Why is it that the EM force can't be modeled on spatio-temporal curvature the way gravity can be?
 
Physics news on Phys.org
Because the EM force does not obey the equivalence principle. For example, suppose you have three objects, one with a charge of +1, one with a charge of zero, and one with a charge of -1. You start them all off at rest relative to each other at the same point in space in the same EM field. Because of their different charges--or more precisely, their different charge to mass ratios--they will not stay together.

In the case of gravity, by contrast, all three objects would stay together (we start them at the same point in space so tidal gravity won't separate them). Heuristically, this is because gravity acts on the "mass to mass ratio", not the charge to mass ratio, and the mass to mass ratio is the same for all objects. (Usually this is described as inertial mass being the same as gravitational mass.) But observationally, the key fact is that gravity obeys the equivalence principle, whereas the EM force does not.
 
  • Like
Likes martinbn, Vanadium 50 and Dale
Thank you, thank, thank you. That made perfect sense to me. I'm scared to ask questions on this forum because people can be so mean. I really appreciate that you took the time to break it down for me. This encourages me to ask more questions in the future.
 
Ontophobe said:
Why is it that the EM force can't be modeled on spatio-temporal curvature the way gravity can be?

Yes, it can! See Kaluza-Klein theory.
 
haael said:
See Kaluza-Klein theory.

The curvature that models electromagnetism in Kaluza-Klein theory is not spatio-temporal; it's in a dimension other than the 4 spacetime dimensions. So it's not relevant to the OP's question.
 
Thread 'Can this experiment break Lorentz symmetry?'
1. The Big Idea: According to Einstein’s relativity, all motion is relative. You can’t tell if you’re moving at a constant velocity without looking outside. But what if there is a universal “rest frame” (like the old idea of the “ether”)? This experiment tries to find out by looking for tiny, directional differences in how objects move inside a sealed box. 2. How It Works: The Two-Stage Process Imagine a perfectly isolated spacecraft (our lab) moving through space at some unknown speed V...
Does the speed of light change in a gravitational field depending on whether the direction of travel is parallel to the field, or perpendicular to the field? And is it the same in both directions at each orientation? This question could be answered experimentally to some degree of accuracy. Experiment design: Place two identical clocks A and B on the circumference of a wheel at opposite ends of the diameter of length L. The wheel is positioned upright, i.e., perpendicular to the ground...
In Philippe G. Ciarlet's book 'An introduction to differential geometry', He gives the integrability conditions of the differential equations like this: $$ \partial_{i} F_{lj}=L^p_{ij} F_{lp},\,\,\,F_{ij}(x_0)=F^0_{ij}. $$ The integrability conditions for the existence of a global solution ##F_{lj}## is: $$ R^i_{jkl}\equiv\partial_k L^i_{jl}-\partial_l L^i_{jk}+L^h_{jl} L^i_{hk}-L^h_{jk} L^i_{hl}=0 $$ Then from the equation: $$\nabla_b e_a= \Gamma^c_{ab} e_c$$ Using cartesian basis ## e_I...
Back
Top