Physics
General Relativity
Mass changes the measure of time and of distance. Hang two clocks above a black hole, a neutron star or the Earth and the low one runs slow, so its light arrives stretched. Lay a ruler between two circles and it comes out longer than the circles allow: space itself is curved.
clockslightclock carried downruler
Drag a clock up or down. The bow-ties are light cones: light from that point can only go inside them, and near the mass they flatten, so light barely climbs.
Low clock, timed by the high clock—
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Show
Mass
Numbers
Mass—
Schwarzschild radius rs = 2GM/c²—
r1—
r2—
Clock rate at r1, dτ/dt—
Clock rate at r2, dτ/dt—
Low clock falls behind, per day—
Δr = (C2 − C1)/2π—
Ruler distance r1 to r2—
Radar echo, late against 2Δr/c—
What to observe
- Above a black hole the low clock ticks at about half the rate of the high one. Every flash takes the same time to climb, so they arrive two high ticks apart: light from below is redshifted.
- Carry a clock down, let it wait by the low clock and bring it back. It returns younger than the clock that stayed up, though it ticked normally the whole way.
- In Space, a ruler laid between two circles needs more rungs than the gap their circumferences give. No flat sheet can do that: space is curved too, not just time.
- On Earth, a clock at GPS height gains 45.7 µs a day on the ground from gravity alone. Its orbital speed takes 7.2 back; uncorrected, the net 38.5 µs would shift a GPS fix by 11 km a day.
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