The longest a ruler ever is is at home.
Each frame carries its own one-metre rod. Whichever frame you are in, the rod in your hand is a full metre. The rod in the other frame, blowing past you, is measured to be only long along the direction of motion.
Setup
Two identical metre-sticks, one in Frame A and one in Frame B, each at rest in its own frame. They’re aligned with the direction of relative motion. Slide β to change the relative speed, and toggle who is "at rest" to feel the symmetry.
Live readouts
- γ
- 1.250
- Proper length L₀ (in rod’s rest frame)
- 1.00 m
- Observed length L = L₀/γ (in the other frame)
- 0.800 m
- Contraction (L₀ − L)
- 0.200 m
The rulers
Where it comes from
To measure the length of a moving rod, you have to mark its endpoints at the same time in your frame. That "at the same time" is the catch — different frames disagree about simultaneity.
Place a rod of proper length at rest in , with ends at and . In (in which the rod moves at ) you measure both ends at the same time . Use the inverse Lorentz boost :
Subtracting:
Solve for the length you measure in your frame:
At your current , , so a one-metre rod measures .
Read the puzzle carefully
A common trap: "if A sees B’s rod contracted, and B sees A’s rod contracted, who is right?" Both. Each statement is a measurement made in that observer’s frame. The contraction is not an "appearance" or a "shrinkage of the atoms"; it is a consequence of how simultaneity is sliced through spacetime, which differs frame to frame.
Lengths perpendicular to the motion don’t contract — only the component along the boost direction does. So a moving cube becomes a flattened slab, not a smaller cube.