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Time dilation near a horizon

node

Clocks run slow in a gravitational potential, and near a black hole the effect becomes unbounded. A static clock at radius r ticks slower than a distant one by the square root of one minus the ratio of Schwarzschild radius to r, a factor that goes to zero at the horizon. The consequence is the sharpest asymmetry in the subject: an infalling observer crosses the horizon in finite proper time and notices nothing locally, while a distant observer never sees the crossing at all. What the distant observer sees instead is the infalling object slowing, reddening and fading, its light dimming exponentially on a timescale set by the light-crossing time of the hole - about a ten-thousandth of a second for a ten-solar-mass hole and a matter of hours for M87*. The object does not hover; it becomes unobservable. The two descriptions are not in conflict, because they are answers to different questions asked by observers who can no longer exchange signals. Not a place on Earth.

A node is not a place. Drawing it on a map would assert something about the world that no stored fact supports.

Read in · 1

Evidence · 2
Timeline

No dated observations are stored for this object. Atlas shows what was observed and when — it does not infer a history.

Connections · 1
Assembled narrative · 1

An assembled narrative is available for this object.

Observed changes · 0

No public Signals are attached to this object. Signals show what changed and when it was observed — never a direction or a rank.

Actions

Read the assembled narrativeContinue in StudioOpen TwinTwin does not start a decision from this kind of object.ShareSaveSaved objects are part of the authenticated projection, which is declared and not yet built.

/atlas?object=PHENOMENON_GRAVITATIONAL_TIME_DILATION