← Special Relativity
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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

Proper Length
L0L_0 is the length of an object measured in its rest frame — the longest measured length. Any other frame measures a shorter value.
Lorentz Contraction
L=L0/γL=L_0/\gamma. Only the dimension parallel to the velocity is contracted; dimensions perpendicular to vv are unchanged. For vcv\ll c, LL0L\approx L_0.
Ladder Paradox
A ladder of proper length L0L_0 fits inside a barn of proper length Lb<L0L_b < L_0. If the ladder moves fast enough, L=L0/γ<LbL=L_0/\gamma<L_b — the ladder fits. Resolved by relativity of simultaneity: the two ends of the ladder enter/exit simultaneously in neither frame.
Penrose-Terrell Rotation
Although a moving sphere is length-contracted, the visual appearance is of a rotated sphere (not a squashed one) due to light travel-time effects. Lorentz contraction is real but visual appearance involves additional optics.

Key Equations

Length contraction
L=L0γ=L01β2L = \frac{L_0}{\gamma} = L_0\sqrt{1-\beta^2}
Length measured in lab frame; L₀ = proper length (rest frame value).
Transverse dimensions
y=y,z=zy' = y, \quad z' = z
Perpendicular dimensions are unchanged by a boost along x.
Proper length from interval
L0=(Δs)2=Δx2c2Δt2L_0 = \sqrt{-(\Delta s)^2} = \sqrt{\Delta x^2 - c^2\Delta t^2}
Spacelike interval between the ends (at the same rest-frame time) gives proper length.
Worked Example

Contracted Length of a Moving Spacecraft

Problem

A spacecraft has proper length L0=500L_0=500 m. It flies past a space station at v=0.80cv=0.80c. What length does the station measure?

Solution

γ=1/10.64=1/0.6=1.667\gamma=1/\sqrt{1-0.64}=1/0.6=1.667.

L=L0γ=5001.667=300 mL = \frac{L_0}{\gamma} = \frac{500}{1.667} = 300\text{ m}

The spacecraft appears only 300 m long to the station — 40% shorter than its rest length.

Answer L = 300 m.
Practice

Exercises

7 problems
1 of 7

A rod has proper length L0=100L_0=100 m and moves at v=0.60cv=0.60c (γ=1.25\gamma=1.25). Find its length LL (in m) in the lab frame.

m
2 of 7

A spacecraft has proper length 500 m and moves at v=0.80cv=0.80c (γ=5/3\gamma=5/3). Find LL (in m) in the lab frame.

m
3 of 7

A moving object appears to have length L=120L=120 m. Its proper length is L0=200L_0=200 m. Find γ\gamma.

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4 of 7

At what speed (as fraction of cc) is a rod contracted to half its proper length?

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5 of 7

A proton (L01.0L_0\approx1.0 fm) travels at β=0.99\beta=0.99 through a detector. Find γ\gamma (to 1 decimal) for β=0.99\beta=0.99.

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6 of 7

In the barn-ladder paradox, a ladder of proper length L0=10L_0=10 m enters a barn of proper length Lb=6L_b=6 m. At what γ\gamma does the ladder exactly fit?

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7 of 7

A train of proper length 300 m moves at v=0.80cv=0.80c. A tunnel has proper length 240 m. What is the train's contracted length (in m) in the tunnel frame?

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Key Takeaways

  • Length contraction L=L0/γL=L_0/\gamma affects only the dimension parallel to the velocity.
  • Proper length L0L_0 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.