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Barn-Pole Paradox Calculator — Special Relativity Length Contraction

Enter the rest lengths of the pole and barn, and the speed as a fraction of c. See the Lorentz factor, the contracted lengths in each reference frame, whether the pole "fits" in each frame, and the simultaneity shift that resolves the apparent contradiction.

m

Rest length of the pole (in its own rest frame)

m

Rest length of the barn (in its own rest frame)
Fraction of the speed of light — must be strictly between 0 and 1
Lorentz factor (γ)
1.6667

γ = 1 / √(1 − β²) — all relativistic effects scale with γ

Pole length in barn frame (contracted)
6 m
Barn length in pole frame (contracted)
4.8 m
Pole fits inside barn? (barn frame)
Yes — pole is shorter than barn
Pole fits inside barn? (pole frame)
No — pole exceeds contracted barn length
Simultaneity shift between door events (pole frame)
35.58 ns
Barn frame: contracted pole length6 m
Barn frame: barn rest length8 m
Pole frame: pole rest length10 m
Pole frame: contracted barn length4.8 m
Step by step
  1. 1

    β²

    0.8² = 0.64
  2. 2

    1 − β²

    1 − 0.64 = 0.36
  3. 3

    √(1 − β²)

    √0.36 = 0.6
  4. 4

    Lorentz factor γ

    1 ÷ 0.6 = 1.6667
    All length contractions and time dilations in this scenario scale with γ.
Results are estimates for general information only and are not professional advice — always verify important results independently before relying on them. Read the full disclaimer.
Quick answer

How does this calculator work?

In the barn frame the moving pole contracts to L₀_pole / γ and can fit inside the barn. In the pole frame the barn contracts to L₀_barn / γ and the pole extends beyond it. The paradox resolves via relativity of simultaneity: "both doors closed simultaneously" is frame-dependent. γ = 1/√(1 − β²); L_contracted = L₀ / γ.

Formula
γ = 1 / √(1 − β²) • L_contracted = L₀ / γ • L is contracted for the moving object in each frame
How this is calculated

The barn-pole paradox (also called the ladder paradox) is a thought experiment in special relativity. A long pole moves at relativistic speed v through a barn. In the barn's rest frame, the pole is Lorentz-contracted to L_pole = L₀_pole / γ — so if β = v/c is large enough, the contracted pole fits inside the barn simultaneously. But in the pole's rest frame, it is the barn that is contracted to L_barn = L₀_barn / γ, and the pole remains at its full rest length — apparently too long to fit.

Both descriptions are correct within their respective reference frames. The apparent paradox is resolved by the relativity of simultaneity: the two events — "front door closes on the pole's rear" and "rear door opens for the pole's front" — are simultaneous in the barn frame but are NOT simultaneous in the pole frame. In the pole frame, the rear door opens before the front door closes, so the pole is never fully enclosed. No physical contradiction exists; only the notion of "at the same time" differs between frames.

The simultaneity shift Δt = γ · β · L₀_barn / c gives the time difference in the pole frame between the two door events. For a 8 m barn at β = 0.8 (γ = 5/3), this shift is about 44 ns — too small to perceive but experimentally consistent with time dilation measured in particle accelerators and GPS corrections.

Frequently asked questions

"Fitting" requires two spatially-separated events (front enters, rear enters) to occur simultaneously. Simultaneity is frame-dependent in relativity. In the barn frame both events are simultaneous; in the pole frame they are not. No physical inconsistency exists — it only appears contradictory if you assume simultaneity is absolute, which it is not.

γ = 1/√(1 − β²) quantifies all relativistic effects: time dilation (clocks slow by γ), length contraction (lengths shorten by 1/γ), and relativistic mass increase. At β = 0.8, γ = 5/3 ≈ 1.667; at β = 0.99, γ ≈ 7.09; at β → 1, γ → ∞.

In any real scenario with rigid-seeming materials, the barn doors would either close on the pole (trapping it, in the barn frame) or not (in the pole frame) — but due to simultaneity being relative, both descriptions are consistent. A physical "trapping" requires the doors to remain closed, which introduces forces that must also be analysed relativistically. The paradox is a gedanken (thought) experiment showing that rigid bodies behave differently at relativistic speeds.

APA

TG we-Calculate Editorial Team. (2026). Barn-Pole Paradox Calculator — Special Relativity Length Contraction [Online calculator]. TG we-Calculate. https://we-calculate.com/calculator/barn-pole-paradox-calculator

Chicago

TG we-Calculate Editorial Team. "Barn-Pole Paradox Calculator — Special Relativity Length Contraction." TG we-Calculate. 2026. https://we-calculate.com/calculator/barn-pole-paradox-calculator.

IEEE

TG we-Calculate Editorial Team, "Barn-Pole Paradox Calculator — Special Relativity Length Contraction," TG we-Calculate, 2026. [Online]. Available: https://we-calculate.com/calculator/barn-pole-paradox-calculator

BibTeX

@misc{wecalculate_barn_pole_paradox_calculator, title = {Barn-Pole Paradox Calculator — Special Relativity Length Contraction}, author = {{TG we-Calculate Editorial Team}}, howpublished = {\url{https://we-calculate.com/calculator/barn-pole-paradox-calculator}}, year = {2026}, note = {TG we-Calculate} }

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