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Proper time

physical science Maturity 9-11 Next article →

In the study of relativity, time is not a single, universal clock ticking for everyone. Instead, scientists use a specific concept called proper time to describe how time passes for a specific object. Proper time is the time measured by a clock that follows a particular path through spacetime. This path is known as a timelike world line.

Proper and coordinate time
Proper and coordinate time

While different observers might assign different numbers to the time between two events, the proper time remains a Lorentz scalar. This means the proper time interval is independent of the coordinate system used to measure it. It provides a fundamental way to understand the duration of a journey through the universe.

To understand how proper time works, we must look at the relationship between motion and the passage of time. An observer uses coordinate time, represented by the letter *t*, to assign time to events based on their own perspective. However, proper time, often represented by the Greek letter *tau* (τ), is measured experimentally by a clock moving along a path. The proper time interval between two events depends on the specific world line connecting them. If a clock moves or accelerates, the time it measures will change. Specifically, an accelerated clock will measure a smaller elapsed time between two events than a non-accelerated, or inertial, clock.

Proper and coordinate time
Proper and coordinate time

This process is mathematically similar to calculating the arc length of a curvy line in geometry.

There are different ways to categorize these paths through spacetime. A timelike path is one that allows for the construction of physical rulers and clocks to measure proper time. In contrast, a spacelike path leads to a measurement of proper distance rather than time. There are also lightlike paths, which are traveled by light. For these paths, the concept of proper time is undefined because the spacetime interval is zero. In these special cases, scientists must use an arbitrary parameter that is not related to time. This distinction helps physicists categorize how different objects, from humans to particles of light, move through the cosmos.

The mathematical foundation of this concept was significantly advanced by Hermann Minkowski. In 1908, Minkowski introduced the concept of proper time to describe the structure of spacetime.

Proper and coordinate time
Proper and coordinate time

His work allowed for the creation of Minkowski diagrams, which are visual tools used to map these paths. In special relativity, the metric used to calculate these intervals is the Minkowski metric. This math shows that proper time is the pseudo-Riemannian arc length of world lines in a four-dimensional spacetime. Minkowski's discovery changed physics by showing that space and time are not separate, but are part of a single fabric.

One of the most famous ways to demonstrate proper time is through the twin paradox. Imagine two twins where observer A stays at rest for 10 years of coordinate time. In this scenario, observer A's proper time is exactly 10 years. Now, imagine twin B travels at a speed of 0.866*c*, which is 86.6% of the speed of light.

Proper and coordinate time
Proper and coordinate time

Twin B travels for 5 years of coordinate time, then accelerates and travels back for another 5 years. When the math is applied, the total proper time for twin B is only about 5.77 years. This shows how high speeds and acceleration cause time dilation, making the traveler age more slowly than the twin who stayed still.

Proper time also behaves predictably in rotating systems, such as a rotating disk. For an observer moving in a circle at a constant distance *r* and angular rate *ω*, the proper time is affected by that rotation. The formula shows that the rotation reduces the amount of proper time experienced compared to an observer standing still at the center. This principle also applies to massive objects like the Earth using the Schwarzschild solution.

Proper and coordinate time
Proper and coordinate time

Because Earth has mass, gravity affects the passage of time. A clock at the North Pole will measure time slightly differently than a clock at the equator. This is because the equator is further from the center and is moving faster due to the Earth's rotation.

Ultimately, proper time connects the local experience of an object to the global structure of the universe. In special relativity, the math works for flat spacetime, but it generalizes into general relativity for curved spacetime. In general relativity, the metric tensor describes how gravity bends the paths of objects.

Proper and coordinate time
Proper and coordinate time

Whether we are looking at the movement of a satellite or the rotation of a planet, proper time is the tool that allows us to calculate the true duration of any journey. It proves that time is deeply connected to both how fast we move and the gravity around us.

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File:Proper and coordinate time.png
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