Vedatom Physics
Modern Physics / Special Relativity
The quantum toolkit
β = v/c
γ = 1/√(1 − β²)
c = 3.00×10⁸ m/s
mₑc² = 0.511 MeV
E = γm₀c²
K = (γ − 1)m₀c²
u' = (u+v)/(1+uv/c²)
= (pc)² + (m₀c²)²
Everything hangs on the Lorentz factor γ ≥ 1. It's ≈1 in daily life and blows up as v→c — which is why nothing massive can reach the speed of light.
full reference ↗
Modern Physics · six modules the whole quantum-and-beyond arc
§05

Relativity of simultaneity — who gets hit first

A lamp at the centre of a moving train fires light to both ends. In the train’s own frame both ends light up at the same instant. But to a platform observer the train rushes forward while the light crawls at the same c both ways — so the rear end races to meet its pulse and is struck first. Simultaneity is not absolute; it depends on your frame. Speed the train up and watch the gap open.

Bench · platform frame · flash from the centre
train speed v{{ simBetaPct }}% c
platform frame
rear struck first
Δt = L₀ v· leading clocks lag
In the train’s own frame the flash reaches both ends together — the disagreement is real, not an illusion of signal delay.
§01

The light-clock & the γ dial

Bounce a photon between two mirrors and call each round trip a tick. In the clock's own frame the light goes straight up and down — that's the shortest, proper tick. But to someone watching it fly past, the same photon must travel a longer diagonal at the same speed c, so its tick takes longer: Δt = γΔt₀. Nothing about the clock changed — only the geometry of the path. Slide v toward c and watch the diagonal — and the tick — stretch out.

Bench · Δt = γ·Δt₀
Lorentz factor γ
{{ lcGamma }}
tick Δt / Δt₀
{{ lcGamma }}×
Speed v{{ lcBetaPct }}% of c
1 s proper reads{{ lcObs }} s
Δt = γΔt₀ = Δt₀√(1−β²)
speed v{{ lcBetaPct }}% c
{{ lcVerdict }}