OPH · 64k
V29·Act VI · Spacetime

Curvature as the atlas failing to close

A frame carried around a closed chain of overlapping charts comes back visibly rotated against its ghost.

The relation on screen

Transport a frame around a loop and its failure to return is curvature, measured per unit enclosed area.

Symbols

closed loop in the chart
curvature, the deficit density
transport
chart to chart
only transition maps are used
observer leaves the space
never
closed loop mismatch
48.6°
triangles sampled
12,000
holonomy statistics

the surveyor's definition

Curvature does not need an embedding space. Carry a frame around a closed loop using nothing but the rules for translating between neighbouring charts, and if it comes back rotated the space is curved. On a sphere you can do this with three right-angled turns and end up facing ninety degrees off. Set the curvature slider to zero and the frame returns exactly as it left.

what to look for · The deficit scales with enclosed area, which is what distinguishes curvature from a bookkeeping error.

Consensus to physics

  1. 01carry a frame from chart to chart around a closed chain of overlaps
  2. 02each hop applies that pair's transition map
  3. 03the frame returns rotated relative to its start
  4. 04that holonomy is curvature, measured entirely from inside

In standard physics

Parallel transport and the Riemann tensor

Curvature defined the way a surveyor would define it. No observer steps outside; curvature is an internal consequence of how charts fail to agree globally.

boundary · The chart layout in the picture is illustrative. This is not a measurement of a spacetime Riemann tensor and no metric has been attached.