Lorentz Transformations
The Lorentz transformations replace the Galilean transformations of Newtonian mechanics. They mix space and time coordinates between inertial frames and reduce to the Galilean transform in the limit $v\ll c$. Any physical law that is Lorentz-covariant automatically satisfies the postulates of special relativity.
Key Concepts
Key Equations
Transforming Coordinates Between Frames
Frame moves at relative to . An event occurs at ns, m in . Find and . ( m/s.)
. Note: m.
s ns.
Exercises
7 problemsFind the Lorentz factor for .
Find for .
Frame moves at (). An event at m, in . Find (in m).
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Upgrade to Pro βSame frame (, ). Event at m, . Find (in ns, use m/s).
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Upgrade to Pro βTwo spaceships travel in opposite directions relative to Earth. Ship A moves at and ship B at (in the opposite direction, so relative to Earth). Find ship B's speed as seen from ship A using velocity addition: with and . Express as .
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Upgrade to Pro βA rocket travels at relative to Earth (). A photon is fired forward. Find its speed in the rocket frame (in units of c).
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Upgrade to Pro βA rocket (, ) emits a signal at , in its frame. Find the coordinate in the lab frame using the inverse transform (in m if ).
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Upgrade to Pro βKey Takeaways
- Lorentz boosts mix and : , .
- is always and grows without bound as .
- Velocity addition always gives β the speed limit is self-consistently maintained.
- The Lorentz group is a 6-parameter group (3 boosts + 3 rotations) acting on Minkowski spacetime.