Special Relativity
Time Dilation, Length Contraction & the Light Cone
Postulate
c is invariant
Speed of light
299,792 km/s
v / c (sim)
0.866
γ (sim)
2.00
Lorentz form
γ = 1/√(1−β²)
At v = 0.99c
γ ≈ 7.09
1. The laws of physics take the same form in every inertial (non-accelerating) frame. There is no privileged stationary observer.
2. The speed of light in vacuum is the same for every observer, regardless of how the source or observer is moving. This single rule forces space and time to mix.
In the simulation, the photon traces the same c in both frames — but the moving clock's photon must travel a longer diagonal. Each tick takes longer, so its clock runs slow.
Atmospheric muons
γ ≈ 30Cosmic-ray muons created ~15 km up have a half-life of just 1.5 μs at rest — far too short to reach the surface. Yet detectors find them in abundance. From our frame their clocks run slow; from theirs the atmosphere is contracted. Either way, they make it.
Particle accelerators
γ ≈ 7500Protons at the LHC are pushed to 0.999999991 c. Their internal clocks tick about 7,500× slower than ours, and short-lived particles produced in collisions live long enough to leave measurable tracks before decaying.
Hafele–Keating experiment
Direct test, 1971In 1971, atomic clocks flown around the world on commercial jets returned tens of nanoseconds out of sync with ground-based clocks — exactly as special and general relativity predict for the combined motional and gravitational effects.
Frame Shift Drive (lore)
ED narrativeED's FSD sidesteps relativistic time dilation by warping spacetime around the ship rather than accelerating through it — the hull never approaches c locally. Without this trick, supercruise across a system would leave the commander decades out of step with the bubble.
