Special Relativity · 03 / 06

Spacetime Interval

Observers can disagree about spatial distance and elapsed coordinate time while agreeing on one deeper quantity: the spacetime interval between the same two events.

The learner question

If observers disagree about space and time, what can they still agree on?

Lorentz transformations reshuffle the spatial and temporal parts of an event separation. The interval stays invariant, giving every inertial observer the same causal classification of the pair.

Invariant interval · one spatial dimension
Δs2=c2Δt2Δx2\Delta s^2=c^2\Delta t^2-\Delta x^2

The lab uses c=1c=1, so time is measured in seconds and distance in light-seconds.

Invariant-geometry lab

Move the second event, then boost the observer.

γ = 1.120
ct
x
solid = original coordinates · outline = boosted coordinates
Δs² original
3.800
Δs² boosted
3.800
Δt′
1.98
Δx′
0.36
Coordinate-time separation Δt2.40 s
Spatial separation Δx1.40 light-s
Boost speed v0.45 c
timelikeΔs² > 0

A slower-than-light causal influence can connect the events. Some frame places both events at the same position.

lightlikeΔs² = 0

Only a light-speed signal connects the events. Every inertial observer keeps them on the light cone.

spacelikeΔs² < 0

No subluminal causal signal can connect the events. Different frames may disagree about their time order.

invariant idea
The interval is invariant

Change the frame speed. Δt′ and Δx′ move, but their Minkowski combination stays the same apart from numerical rounding.

invariant idea
Causality is geometric

Timelike, lightlike, and spacelike are not observer opinions. The interval fixes the causal class for every inertial frame.

invariant idea
Proper quantities come from the interval

For this timelike pair, the proper-time magnitude is 1.95 s.

Transfer check

Two events are separated by 2 seconds and 3 light-seconds. What kind of spacetime separation do they have?

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