Spacetime Diagrams
Spacetime diagrams (Minkowski diagrams) are the geometric language of special relativity. Each point is an event; each particle traces a worldline; light travels at 45°. The causal structure — what can influence what — is encoded in the light cone.
Key Concepts
Key Equations
Reading Proper Time from a Spacetime Diagram
A worldline passes through events and ( m/s). Find the proper time between them.
Convert: m.
Exercises
7 problemsA particle moves at . What is the slope of its worldline (in a vs diagram)?
Events and . Find the proper time (in m/c, or equivalently in units where c=1). .
Is the interval between events and timelike, lightlike, or spacelike? Find .
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Upgrade to Pro →A rocket leaves Earth at at . How far (in ly) from Earth is it when the Earth clock reads yr?
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Upgrade to Pro →Two flashes occur at and m. A third observer sees them at the same time (). At what speed (as fraction of ) must this observer move? .
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Upgrade to Pro →Light from a star 10 ly away was emitted when? Looking at the past light cone, light emitted 10 yr ago arrives now. If the star is now 10 ly away, how many years ago was the light emitted?
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Upgrade to Pro →A spaceship accelerates with proper acceleration m/s² (1g). The Rindler horizon is at distance behind the ship. Find this distance (in light-years). ( m; 1 ly m.)
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Upgrade to Pro →Key Takeaways
- Spacetime diagrams visualize events, worldlines, and causality. Light travels at 45°; massive particles always have |slope| > 1.
- The light cone divides spacetime into timelike future/past (can be influenced/can influence) and spacelike elsewhere (causally disconnected).
- Proper time is the "length" of a worldline: .
- A Lorentz boost tilts the and axes symmetrically toward the light cone — lengths and times change, but the light cone is invariant.