Barn Pole Paradox Calculator
Explore special-relativity length contraction and compare the pole and barn from both inertial reference frames.
About the barn-pole paradox
Barn-pole paradox examples
The examples compare the same proper lengths at several relativistic speeds.
| Rest lengths and speed | Frame-dependent lengths | Barn-frame outcome |
|---|---|---|
| Pole 20 m, barn 10 m, speed 0.9c | Gamma 2.2942; pole 8.7178 m; barn 4.3589 m | The pole fits in a simultaneous barn-frame snapshot. |
| Pole 20 m, barn 10 m, speed 0.6c | Gamma 1.25; pole 16 m; barn 8 m | The pole is still longer than the barn in the barn frame. |
| Pole 12 m, barn 10 m, speed 0.8c | Gamma 1.6667; pole 7.2 m; barn 6 m | The contracted pole fits, while the pole frame sees a contracted barn. |
How to use the barn-pole paradox calculator
- Enter the pole length measured while the pole is at rest.
- Enter the barn length measured while the barn is at rest.
- Enter relative speed as a decimal fraction of light speed, such as 0.9.
- Select Calculate Relativistic Lengths and compare the two frame-dependent lengths.
- Interpret the fit statement only as simultaneous in the barn's reference frame.
Barn-pole paradox FAQ
Does the pole really fit inside the barn?
In the barn frame, the moving pole can be shorter than the barn at one instant. In the pole frame, the two door-closing events are not simultaneous, so there is no contradictory simultaneous enclosure.
Which measured length is the real length?
Proper length is measured in the object's own rest frame, while moving observers measure a contracted length. Both measurements are physically valid within their specified reference frames.
What resolves the apparent paradox?
Relativity of simultaneity resolves it. Observers moving relative to one another disagree about the timing of spatially separated door events, even though they agree on causal relationships.
Why must speed be less than one?
The input is beta, meaning velocity divided by light speed, and a massive pole cannot reach or exceed light speed. At beta equal to one, the Lorentz factor formula becomes singular.
What happens if a door strikes the pole?
Mechanical stress propagates through the pole at a finite material-dependent speed. The idealized rigid pole is not physically possible, so collision dynamics require a more detailed model.