Barn Pole Paradox Calculator

Explore special-relativity length contraction and compare the pole and barn from both inertial reference frames.

Relativistic length inputs
Enter proper lengths and relative speed as a fraction of the speed of light.

About the barn-pole paradox

The barn-pole paradox is a thought experiment that reveals why length contraction cannot be understood without the relativity of simultaneity. Imagine a pole whose proper length is greater than a barn's proper length. The pole moves toward the barn at a substantial fraction of the speed of light. An observer standing with the barn measures the moving pole as contracted, so at a sufficiently high speed the entire pole can be between the barn doors at one instant in that observer's frame. The Lorentz factor, commonly called gamma, equals one divided by the square root of one minus speed squared when speed is expressed as a fraction of light speed. A moving object's measured length along the direction of travel is its proper length divided by gamma. The calculator therefore contracts the pole in the barn frame and separately contracts the barn in the pole frame. Only the object moving relative to a chosen frame is contracted in that frame. From the pole's perspective, the barn is even shorter than its rest length, so it appears impossible for the pole to fit. There is no contradiction because the two observers disagree about which spatially separated events occur simultaneously. In the barn frame, closing both doors at the same time can briefly enclose the contracted pole. In the pole frame, the front door closes and opens before the rear door closes. No signal or physical influence must travel faster than light, and every observer agrees on the causal order of events that can influence one another. This calculator displays geometric lengths for both frames but does not simulate door forces or acceleration. A real pole struck by a closing door would transmit stress at the material's finite sound speed, not instantaneously, and changing frames during acceleration requires additional analysis. The classic paradox assumes idealized inertial motion and precisely timed door events to isolate the central lesson. Use proper lengths measured in each object's own rest frame and enter beta, the speed divided by light speed, rather than meters per second. Values close to one produce large Lorentz factors and dramatic contraction. The fit statement applies only to a simultaneous snapshot in the barn frame; it does not claim that both frames agree on simultaneous enclosure. That distinction is exactly what resolves the apparent paradox.

Barn-pole paradox examples

The examples compare the same proper lengths at several relativistic speeds.

Rest lengths and speedFrame-dependent lengthsBarn-frame outcome
Pole 20 m, barn 10 m, speed 0.9cGamma 2.2942; pole 8.7178 m; barn 4.3589 mThe pole fits in a simultaneous barn-frame snapshot.
Pole 20 m, barn 10 m, speed 0.6cGamma 1.25; pole 16 m; barn 8 mThe pole is still longer than the barn in the barn frame.
Pole 12 m, barn 10 m, speed 0.8cGamma 1.6667; pole 7.2 m; barn 6 mThe contracted pole fits, while the pole frame sees a contracted barn.

How to use the barn-pole paradox calculator

  1. Enter the pole length measured while the pole is at rest.
  2. Enter the barn length measured while the barn is at rest.
  3. Enter relative speed as a decimal fraction of light speed, such as 0.9.
  4. Select Calculate Relativistic Lengths and compare the two frame-dependent lengths.
  5. 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.