Length Contraction
A rod moving relative to an observer appears shorter than when at rest — its length is $L=L_0/\gamma$ along the direction of motion. Like time dilation, this is a real physical effect, not an illusion. Transverse dimensions are unaffected. The two effects — time dilation and length contraction — are two sides of the same Lorentz transformation.
Key Concepts
Key Equations
Contracted Length of a Moving Spacecraft
A spacecraft has proper length m. It flies past a space station at . What length does the station measure?
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The spacecraft appears only 300 m long to the station — 40% shorter than its rest length.
Exercises
7 problemsA rod has proper length m and moves at (). Find its length (in m) in the lab frame.
A spacecraft has proper length 500 m and moves at (). Find (in m) in the lab frame.
A moving object appears to have length m. Its proper length is m. Find .
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Upgrade to Pro →At what speed (as fraction of ) is a rod contracted to half its proper length?
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Upgrade to Pro →A proton ( fm) travels at through a detector. Find (to 1 decimal) for .
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Upgrade to Pro →In the barn-ladder paradox, a ladder of proper length m enters a barn of proper length m. At what does the ladder exactly fit?
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Upgrade to Pro →A train of proper length 300 m moves at . A tunnel has proper length 240 m. What is the train's contracted length (in m) in the tunnel frame?
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Upgrade to Pro →Key Takeaways
- Length contraction affects only the dimension parallel to the velocity.
- Proper length is the maximum measured length — in the rest frame.
- Length contraction and time dilation are consistent: both follow from the same Lorentz transformation.
- The ladder/barn paradox is resolved by relativity of simultaneity — different frames disagree about when "fits" means.