FKM Kompass
L3

Relativity of simultaneity

Two events that are simultaneous in one inertial reference frame are generally not simultaneous when viewed from a different frame moving relative to the first, a direct consequence of the finite, constant speed of light — simultaneity is not an absolute, frame-independent fact but depends on the observer's state of motion.

Practise this concept

In everyday experience, "at the same time" seems like an obvious, universal fact: either two events happen simultaneously or they don't, and everyone should agree on which. Special relativity shows this intuition is wrong once the two postulates — the laws of physics are the same in every inertial frame, and the speed of light in vacuum is the same for every inertial observer — are taken seriously.

The classic illustration involves two events separated in space, such as lightning striking both ends of a moving train. An observer standing exactly midway between the two strike points, at rest relative to the train, sees the light from both strikes arrive at the same instant and concludes the strikes were simultaneous. An observer on the platform, watching the same two strikes but moving relative to the train, is at the midpoint of the strike locations only in the platform's own rest frame; because light travels at the same fixed speed for this observer too, and because the train observer's position is moving during the light's travel time, the platform observer generally finds that light from one strike arrives before light from the other, and concludes the strikes were not simultaneous. Both observers are applying the same physics correctly and using the same constant speed of light; they simply disagree about the timing of spatially separated events, and neither is more "correct" than the other.

This is not a perceptual illusion or an artifact of not accounting for light travel time — both observers have already corrected for light-travel delay using their own frame's constant light speed, and they still disagree. Simultaneity for spatially separated events is a frame-dependent notion, not an absolute one, and this relativity of simultaneity is the conceptual root from which effects like time dilation and length contraction can be derived via the Lorentz transformations. The effect exists at every relative speed, not only near the speed of light — it is simply too small to notice at everyday speeds, growing to become dramatic and directly measurable only as relative speeds approach the speed of light.

Key ideas

Requires: Postulates of special relativity, Time dilation

Common misconceptions

  • If two events are simultaneous for one observer, they must be simultaneous for every other observer as well.
  • The relativity of simultaneity is just an illusion caused by the time it takes light to reach an observer, not a real disagreement about when events occurred.
  • Simultaneity disagreements between observers only appear at speeds close to the speed of light, never at everyday speeds.

Resources

Part of these UT courses

This concept is mapped as covering part of the following course(s) in the University of Tartu curriculum.