‹ Figure Out Science Physics · Relativity

The twin paradox

One twin flies to a star and back. On return, she is younger than the sibling who stayed on Earth. Where is the paradox?

Alice stays on Earth; her twin Bob boards a rocket and flies at near-light speed to a distant star, then turns around and comes home. When they meet again, Bob is noticeably younger — his clock, his heart and his cells ticked more slowly throughout the trip. This is no fairy tale, but a measured, real effect of time dilation.

Speed v
0,80 c
γ — Lorentz factor
1,67
Rocket speed0,80 c

Distance to the star: 4 light-years. Both start aged 30. The large number is the age, "+" is the time elapsed during the trip.

Fig. 1 — The traveller’s clock ticks slower, so the rocket twin returns younger.

Where does the asymmetry come from?

On the face of it the situation is symmetric — each sees the other moving away. But it is Bob who accelerates, brakes and turns around; he is the one who changes reference frame. Alice stays the whole time in a single, quiet inertial frame.

That difference breaks the symmetry: the effect is not mutual, and it is the traveller who ages more slowly. The turnaround — the moment of acceleration — is what unambiguously singles Bob out from the pair.

By how much exactly?

The traveller’s time shrinks by a factor of √(1 − v²/c²). This is usually written via the Lorentz factor γ = 1/√(1 − v²/c²) — exactly the γ shown in the animation: it tells how many times slower the traveller’s clock ticks (1.67× at 0.8 c). At 80% of light speed time shrinks to 0.6: if 10 years pass for Alice, only 6 pass for Bob.

The key formula
τ = T · √(1 − v²/c²)
τ — traveller’s time (Bob) · T — time on Earth (Alice) · for v = 0.8 c → τ = 0.6 T; for v = 0.99 c → τ ≈ 0.14 T

Use the speed slider in the animation to see how the gap grows as v rises. The closer to light speed, the more slowly Bob’s clock ticks — and the larger the age difference on return.

A ticket to the future

Travel at near-light speed is a one-way ticket into the future.

Time dilation cannot take you back in time, but it lets you "skip" forward. Returning, Bob arrives at an Earth older by years, though he himself has barely aged. In practice this applies to every astronaut — cosmonauts returning from long missions are fractions of a second younger than us.

Where the model ends

We left out the phases of acceleration and braking, treating the trip as two constant-speed legs. In reality it is precisely the continuous changes of speed and general relativity that describe the full picture — but the final result (the age difference) comes out the same.

A simplificationWe also assumed a perfectly rigid distance and ignored the length contraction Bob observes in his frame. These are two sides of the same coin — and both lead to the same, measurable difference of clocks.

Bibliography (sample)

  1. 1 Einstein, A. — "Zur Elektrodynamik bewegter Körper", Annalen der Physik 17 (1905). 10.1002/andp.19053221004
  2. 2 Langevin, P. — "L’évolution de l’espace et du temps", Scientia 10 (1911) — the first formulation of the paradox. Scientia X, 31
  3. 3 Hafele, J. C. & Keating, R. E. — "Around-the-World Atomic Clocks", Science 177 (1972). 10.1126/science.177.4044.166
Always ad-free

This article is free — and will stay that way

No ads, no paywall. If it helped you understand the topic, support the making of the next one.

Support the magazine Join the newsletter
Next article · Relativity
Einstein’s light clock