File:DifferentialAgingAndFalling.JPG

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English: This plot illustrates Epstein's x-cτ-plot argument[1], in his sketches 9-9 and 10-4, for how differential aging causes gravitational acceleration. Note that x-cτ plots are not "global plots of events in space-time" because the cτ axis is specific to each trajectory.

The green trajectories show two siblings who spend the same amount of map-time Δt (line-length) between start (solid circle) and finish (open circles), one up in the attic (dotted-trajectory) and the other down in the basement (dashed-trajectory). Little proper-time (azimuth-angle) is spent by either sibling in changing floors (radial-position). As you can see, a curved x-cτ plot lets us show how the siblings return to the ground floor with less proper-time Δτ having elapsed on (and hence less aging of) the sibling who stayed in the basement.

The red straight and therefore free-float-frame "fly-ball" trajectory shows how spacetime, bent as above to allow differential-aging on the two traveler clocks, as a consequence also requires that an object in free fall experiences a downward acceleration. This is because straight free-fall trajectories naturally change motion always "at lightspeed" through proper time (i.e. when stopped so that cδτ/dt = c) to motion which is also partly through space (i.e. dx/dt ≤ c), and vice versa, when spacetime is curved by gravity's differential aging. Light of course to first order experiences that same motion largely through space and not time, so that dx/dt ≈ c and light trajectories on the plot above will be largely in the radial direction.
Date
Source Own work
Author P. Fraundorf

Further notes[edit]

The figures below illustrate how x-cτ trajectory plots compare to more familiar x-ct spacetime plots[2], and to perhaps less-familiar ρ-cτ extended-simultaneity plots[3], in flat spacetime. The first of these figures shows how these might work for constant-velocity observers e.g. to illustrate time-dilation and length-contraction.

A triad of x-ct, x-cτ and ρ-cτ plots for constant speed time-dilation (green) and length-contraction (blue) in flat spacetime.

The figure below illustrates how these work in flat spacetime to show what happens for a traveler undergoing constant proper-acceleration.

A triad of x-ct, x-cτ and ρ-cτ plots for a constant proper-acceleration visit to our x-ct origin.

In principle these x-cτ plots can also work (schematically at least) to illustrate, again following Epstein, the way that extreme gravitational curvature hinders the far-away observation of events near the event-horizon of a static black hole.

Wrapped schematic-plots of x-cτ through the (open) center of objects of varying mass.

Footnotes[edit]

  1. Epstein, Lewis Carroll (1895/1994). Relativity Visualized, (Insight Press, San Fransisco), ch. 9-12.
  2. Minkowski, Hermann (1907/1915) "Das Relativitätsprinzip", Annalen der Physik 47 352 (15): 927–938, prepared by A. Sommerfeld long after Minkowski's death. link
  3. Carl E. Dolby and Stephen F. Gull (2001) "On radar time and the twin paradox", Amer. J. Phys. 69 (12) 1257-1261 abstract.

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