Proper time
In relativity, proper time along a timelike world line is defined as the time as measured by a clock following that line. It is thus independent of coordinates, and is a Lorentz scalar.^{[1]} The proper time interval between two events on a world line is the change in proper time. This interval is the quantity of interest, since proper time itself is fixed only up to an arbitrary additive constant, namely the setting of the clock at some event along the world line. The proper time interval between two events depends not only on the events but also the world line connecting them, and hence on the motion of the clock between the events. It is expressed as an integral over the world line. An accelerated clock will measure a smaller elapsed time between two events than that measured by a nonaccelerated (inertial) clock between the same two events. The twin paradox is an example of this effect.^{[2]}
In terms of fourdimensional spacetime, proper time is analogous to arc length in threedimensional (Euclidean) space. By convention, proper time is usually represented by the Greek letter τ (tau) to distinguish it from coordinate time represented by t.
By contrast, coordinate time is the time between two events as measured by an observer using that observer's own method of assigning a time to an event. In the special case of an inertial observer in special relativity, the time is measured using the observer's clock and the observer's definition of simultaneity.
The concept of proper time was introduced by Hermann Minkowski in 1908,^{[3]} and is a feature of Minkowski diagrams.
Mathematical formalism [ edit ]
The formal definition of proper time involves describing the path through spacetime that represents a clock, observer, or test particle, and the metric structure of that spacetime. Proper time is the pseudoRiemannian arc length of world lines in fourdimensional spacetime. From the mathematical point of view, coordinate time is assumed to be predefined and we require an expression for proper time as a function of coordinate time. From the experimental point of view, proper time is what is measured experimentally and then coordinate time is calculated from the proper time of some inertial clocks.
Proper time can only be defined for timelike paths through spacetime which allow for the construction of an accompanying set of physical rulers and clocks. The same formalism for spacelike paths leads to a measurement of proper distance rather than proper time. For lightlike paths, there exists no concept of proper time and it is undefined as the spacetime interval is identically zero. Instead an arbitrary and physically irrelevant affine parameter unrelated to time must be introduced.^{[4]}^{[5]}^{[6]}^{[7]}^{[8]}^{[9]}
In special relativity [ edit ]
Let the Minkowski metric be defined by
and define
for arbitrary Lorentz frames.
Consider an infinitesimal interval between two events:
expressed in any Lorentz frame and here assumed timelike, separating points on a trajectory of a particle (think clock). The same interval can be expressed in coordinates such that at each moment, the particle is at rest. Such a frame is called an instantaneous rest frame, denoted here by the coordinates for each instants. Due to the invariance of the interval (instantaneous rest frames taken at different times are related by Lorentz transformations) one may write
since in the instantaneous rest frame, the particle or the frame itself is at rest, i.e., . Since the interval is assumed timelike, one may take the square root of the above expression;^{[10]}
or
Given this differential expression for τ, the proper time interval is defined as
Here P is the worldline from some initial event to some final event with the ordering of the events fixed by the requirement that the final event occurs later according to the clock than the initial event.
Using (1) and again the invariance of the interval, one may write^{[11]}
where v(t) is the coordinate speed at coordinate time t, and x(t), y(t), and z(t) are space coordinates. The first expression is manifestly Lorentz invariant. They are all Lorentz invariant, since proper time and proper time intervals are coordinateindependent by definition.
If t, x, y, z, are parameterised by a parameter λ, this can be written as
If the motion of the particle is constant, the expression simplifies to
where Δ means the change in coordinates between the initial and final events. The definition in special relativity generalizes straightforwardly to general relativity as follows below.
In general relativity [ edit ]
Proper time is defined in general relativity as follows: Given a pseudoRiemannian manifold with a local coordinates x^{μ} and equipped with a metric tensor g_{μν}, the proper time interval Δτ between two events along a timelike path P is given by the line integral^{[12]}

(4)
This expression is, as it should be, invariant under coordinate changes. It reduces (in appropriate coordinates) to the expression of special relativity in flat spacetime.
In the same way that coordinates can be chosen such that x^{1}, x^{2}, x^{3} = const in special relativity, this can be done in general relativity too. Then, in these coordinates,^{[13]}
This expression generalizes definition (2) and can be taken as the definition. Then using invariance of the interval, equation (4) follows from it in the same way (3) follows from (2), except that here arbitrary coordinate changes are allowed.
Examples in special relativity [ edit ]
Example 1: The twin "paradox" [ edit ]
For a twin paradox scenario, let there be an observer A who moves between the Acoordinates (0,0,0,0) and (10 years, 0, 0, 0) inertially. This means that A stays at for 10 years of Acoordinate time. The proper time interval for A between the two events is then
So being "at rest" in a special relativity coordinate system means that proper time and coordinate time are the same.
Let there now be another observer B who travels in the x direction from (0,0,0,0) for 5 years of Acoordinate time at 0.866c to (5 years, 4.33 lightyears, 0, 0). Once there, B accelerates, and travels in the other spatial direction for another 5 years of Acoordinate time to (10 years, 0, 0, 0). For each leg of the trip, the proper time interval can be calculated using Acoordinates, and is given by
So the total proper time for observer B to go from (0,0,0,0) to (5 years, 4.33 lightyears, 0, 0) and then to (10 years, 0, 0, 0) is 5 years. Thus it is shown that the proper time equation incorporates the time dilation effect. In fact, for an object in a SR spacetime traveling with a velocity of v for a time , the proper time interval experienced is
which is the SR time dilation formula.
Example 2: The rotating disk [ edit ]
An observer rotating around another inertial observer is in an accelerated frame of reference. For such an observer, the incremental () form of the proper time equation is needed, along with a parameterized description of the path being taken, as shown below.
Let there be an observer C on a disk rotating in the xy plane at a coordinate angular rate of and who is at a distance of r from the center of the disk with the center of the disk at x=y=z=0. The path of observer C is given by , where is the current coordinate time. When r and are constant, and . The incremental proper time formula then becomes
So for an observer rotating at a constant distance of r from a given point in spacetime at a constant angular rate of ω between coordinate times and , the proper time experienced will be
as v=rω for a rotating observer. This result is the same as for the linear motion example, and shows the general application of the integral form of the proper time formula.
Examples in general relativity [ edit ]
The difference between SR and general relativity (GR) is that in GR one can use any metric which is a solution of the Einstein field equations, not just the Minkowski metric. Because inertial motion in curved spacetimes lacks the simple expression it has in SR, the line integral form of the proper time equation must always be used.
Example 3: The rotating disk (again) [ edit ]
An appropriate coordinate conversion done against the Minkowski metric creates coordinates where an object on a rotating disk stays in the same spatial coordinate position. The new coordinates are
and
The t and z coordinates remain unchanged. In this new coordinate system, the incremental proper time equation is
With r, θ, and z being constant over time, this simplifies to
which is the same as in Example 2.
Now let there be an object off of the rotating disk and at inertial rest with respect to the center of the disk and at a distance of R from it. This object has a coordinate motion described by dθ = −ω dt, which describes the inertially atrest object of counterrotating in the view of the rotating observer. Now the proper time equation becomes
So for the inertial atrest observer, coordinate time and proper time are once again found to pass at the same rate, as expected and required for the internal selfconsistency of relativity theory.^{[14]}
Example 4: The Schwarzschild solution – time on the Earth [ edit ]
The Schwarzschild solution has an incremental proper time equation of
where
 t is time as calibrated with a clock distant from and at inertial rest with respect to the Earth,
 r is a radial coordinate (which is effectively the distance from the Earth's center),
 ɸ is a colatitudinal coordinate, the angular separation from the north pole in radians.
 θ is a longitudinal coordinate, analogous to the longitude on the Earth's surface but independent of the Earth's rotation. This is also given in radians.
 1=m is the geometrized mass of the Earth, m = GM/c^{2},
 M is the mass of the Earth,
 G is the gravitational constant.
To demonstrate the use of the proper time relationship, several subexamples involving the Earth will be used here.
For the Earth, M = 5.9742 × 10^{24} kg, meaning that m = 4.4354 × 10^{−3} m. When standing on the north pole, we can assume (meaning that we are neither moving up or down or along the surface of the Earth). In this case, the Schwarzschild solution proper time equation becomes . Then using the polar radius of the Earth as the radial coordinate (or meters), we find that
At the equator, the radius of the Earth is r = 6,378,137 meters. In addition, the rotation of the Earth needs to be taken into account. This imparts on an observer an angular velocity of of 2π divided by the sidereal period of the Earth's rotation, 86162.4 seconds. So . The proper time equation then produces
From a nonrelativistic point of view this should have been the same as the previous result. This example demonstrates how the proper time equation is used, even though the Earth rotates and hence is not spherically symmetric as assumed by the Schwarzschild solution. To describe the effects of rotation more accurately the Kerr metric may be used.
See also [ edit ]
 Lorentz transformation
 Minkowski space
 Proper length
 Proper acceleration
 Proper mass
 Proper velocity
 Clock hypothesis
 Peres metric
Footnotes [ edit ]
 ^ Zwiebach 2004, p. 25
 ^ Hawley, John F.; Holcomb, J Katherine A. (2005). Foundations of Modern Cosmology (illustrated ed.). Oxford University Press. p. 204. ISBN 9780198530961. Extract of page 204
 ^ Minkowski 1908, pp. 53–111
 ^ Lovelock & Rund 1989, pp. 256
 ^ Weinberg 1972, pp. 76
 ^ Poisson 2004, pp. 7
 ^ Landau & Lifshitz 1975, p. 245
 ^ Some authors include lightlike intervals in the definition of proper time, and also include the spacelike proper distances as imaginary proper times e.g Lawden 2012, pp. 17, 116
 ^ Kopeikin, Efroimsky & Kaplan 2011, p. 275
 ^ Zwiebach 2004, p. 25
 ^ Foster & Nightingale 1978, p. 56
 ^ Foster & Nightingale 1978, p. 57
 ^ Landau & Lifshitz 1975, p. 251
 ^ Cook 2004, pp. 214–219
References [ edit ]
 Cook, R. J. (2004). "Physical time and physical space in general relativity" (PDF). Am. J. Phys. 72 (2): 214–219. Bibcode:2004AmJPh..72..214C. doi:10.1119/1.1607338. ISSN 00029505. CS1 maint: ref=harv (link)
 Foster, J.; Nightingale, J.D. (1978). A short course in general relativity. Essex: Longman Scientific and Technical. ISBN 0582441943. CS1 maint: ref=harv (link)
 Kleppner, D.; Kolenkow, R.J. (1978). An introduction to mechanics. McGraw–Hill. ISBN 0070350485. CS1 maint: ref=harv (link)
 Kopeikin, Sergei; Efroimsky, Michael; Kaplan, George (2011). Relativistic Celestial Mechanics of the Solar System. John Wiley & Sons. ISBN 3527408568. CS1 maint: ref=harv (link)
 Landau, L. D.; Lifshitz, E. M. (1975). The classical theory of fields. Course of theoretical physics. 2 (4th ed.). Oxford: Butterworth–Heinemann. ISBN 0750627689. CS1 maint: ref=harv (link)
 Lawden, Derek F. (2012). An Introduction to Tensor Calculus: Relativity and Cosmology. Courier Corporation. ISBN 0486132145. CS1 maint: ref=harv (link)
 Lovelock, David; Rund, Hanno (1989), Tensors, Differential Forms, and Variational Principles, New York: Dover Publications, ISBN 0486658406
 Minkowski, Hermann (1908), "Die Grundgleichungen für die elektromagnetischen Vorgänge in bewegten Körpern", Nachrichten von der Königlichen Gesellschaft der Wissenschaften und der GeorgAugustUniversität zu Göttingen, Göttingen CS1 maint: ref=harv (link) ^{ [permanent dead link] }
 Poisson, Eric (2004), A Relativist's Toolkit: The Mathematics of BlackHole Mechanics, Cambridge University Press, ISBN 9780521537803
 Weinberg, Steven (1972), Gravitation and Cosmology: Principles and Applications of the General Theory of Relativity, New York: John Wiley & Sons, ISBN 9780471925675
 Zwiebach, Barton (2004). A First Course in String Theory (first ed.). Cambridge University Press. ISBN 0521831431. CS1 maint: ref=harv (link)