This calculator shows how the measured length of a moving object changes when it travels at a significant fraction of the speed of light. You enter the object’s rest length (also called proper length) and its velocity relative to a stationary observer. The tool returns the contracted length that the stationary observer would measure along the direction of motion, according to Einstein’s special theory of relativity.
At everyday speeds, the effect is so tiny that it is completely negligible. At relativistic speeds (a large fraction of the speed of light), the effect becomes dramatic. This calculator is intended for educational and illustrative physics use, not for precision engineering design.
In special relativity, length is not an absolute quantity. The measured length of an object can depend on the state of motion of the observer. Two ideas are central:
Special relativity predicts that the moving observer will measure a shorter length along the direction of motion. This is the phenomenon of length contraction. It is not that the object is physically squashed in some absolute sense; instead, different observers slice spacetime into space and time in different ways, leading to different length measurements.
The amount of contraction is governed by the Lorentz factor, denoted by the Greek letter gamma, γ. It depends on the object’s speed v relative to the observer and the speed of light c in vacuum (approximately 299,792,458 m/s).
The Lorentz factor is defined as:
γ =
Using this factor, the relation between the proper length L0 and the contracted length L is:
Both expressions are mathematically equivalent. The square-root form makes it clear that as v approaches c, the factor under the square root becomes small, and therefore the measured length L becomes much smaller than L0.
Internally, the tool uses the physical constant c = 299,792,458 m/s. You do not need to enter the speed of light; it is built into the calculation.
The output length L represents the distance between the front and back of the object measured in the observer’s frame who sees the object moving. Several points help interpret this:
Suppose a spacecraft has a proper length L0 = 100 m when measured at rest in the ship’s own frame. It passes by Earth at a speed of v = 0.8c relative to Earth.
An observer on Earth therefore measures the spacecraft’s length along the direction of travel as 60 m, even though crew members on board still measure 100 m. Both measurements are consistent within the framework of special relativity.
The table below shows how the contracted length L compares to the proper length L0 for several representative speeds, using the relation L / L0 = √(1 − v2/c2).
| Speed v (as a fraction of c) | L / L0 | Interpretation |
|---|---|---|
| 0 (at rest) | 1.000 | No motion relative to observer; measured length equals proper length. |
| 0.1c | ≈ 0.995 | Contraction is less than 1%; effectively negligible in most contexts. |
| 0.5c | ≈ 0.866 | Length is about 13.4% shorter than the proper length. |
| 0.8c | 0.600 | Length is 40% shorter, as in the worked example above. |
| 0.9c | ≈ 0.436 | Length is less than half the proper length. |
| 0.99c | ≈ 0.141 | Length is only about 14% of the proper length; contraction is extreme. |
The underlying physics model is the standard special relativistic length contraction formula. For clarity and safe use, the following assumptions and limitations apply:
Within these limits, the tool provides a reliable illustration of how length measurements depend on relative motion in special relativity.
Length contraction is closely related to time dilation, another major prediction of special relativity. Both phenomena arise from the same Lorentz transformation that relates measurements in different inertial frames.
For example, high-energy particles called muons are created in Earth’s upper atmosphere by cosmic rays. Muons have very short lifetimes, so in classical (non-relativistic) physics, most of them should decay long before reaching the ground. In reality, many are detected at the surface. This can be understood in two complementary ways:
Both descriptions are consistent and highlight how space and time are intertwined in special relativity. A length contraction calculator like this one helps build intuition about that relationship by quantifying how large the effect can be at different speeds.