Ibix
Science Advisor
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"Tidal forces" in general relativity are like the centrifugal force (etc) that emerges in a rotating frame. If you want to pretend that your frame is a simple inertial frame, you need to invoke "inertial" or "fictitious" forces to explain why free-falling particles aren't moving in straight lines.
I think this would be an unusual approach in GR since global inertial frames aren't available anyway. Like centrifugal forces, the obvious application is if you are in a box that is only just big enough to show notable non-inertiality (I'm thinking of a spaceship near a neutron star - with thanks to Larry Niven). But a global view would be that particles are either free-falling with non-zero geodesic deviation, or are being pulled off geodesics by electromagnetic (or other) forces.
I think this would be an unusual approach in GR since global inertial frames aren't available anyway. Like centrifugal forces, the obvious application is if you are in a box that is only just big enough to show notable non-inertiality (I'm thinking of a spaceship near a neutron star - with thanks to Larry Niven). But a global view would be that particles are either free-falling with non-zero geodesic deviation, or are being pulled off geodesics by electromagnetic (or other) forces.