(The issue behind this question is the possibility of shortening the flight time in space travels. One possibility is great velocity, but I am asking here about another means.)

In the flat space, the relativistic interval

(1) (Δs)2 = (Δx0)2 - (Δx1)2 - (Δx2)2 - (Δx3)2

between two space-separated events, E1 and E2, is proportional to the proper time (Δτ)2 which ellapses between E1 and E2, in a frame in which they occur at the same position,

(2) (Δs)2 = (cΔτ)2.

Let Δτflat denote the proper time in the flat space. I know that If the two events occur in the neighborhood of a big mass M, is Δτ < Δτflat. In other words, in presence of big masses the clock ticks at a slower pace. My questions are:

1) If the events occur in some accelerated region, e.g. in an accelerating rocket, is Δτ different from Δτflat? Let me remind the equivalence principle.

2) If the events occur in the region of strong electromagnetic fields, may Δτ be different from Δτflat? In presence of fields Einstein's Field Equations predict another space-time metrix than in the flat space.

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