# Relativity of simultaneity

In physics, the **relativity of simultaneity** is the concept that *distant simultaneity* – whether two spatially separated events occur at the same time – is not absolute, but depends on the observer's reference frame.

## Description

According to Einstein's special theory of relativity, it is impossible to say in an *absolute* sense that two distinct events occur at the same time if those events are separated in space. If one reference frame assigns precisely the same time to two events that are at different points in space, a reference frame that is moving relative to the first will generally assign different times to the two events (the only exception being when motion is exactly perpendicular to the line connecting the locations of both events).

For example, a car crash in London and another in New York appearing to happen at the same time to an observer on Earth, will appear to have occurred at slightly different times to an observer on an airplane flying between London and New York. Furthermore, if the two events cannot be causally connected (i.e. the time between event A and event B is less than the distance between them divided by the speed of light), depending on the state of motion, the crash in London may appear to occur first in a given frame, and the New York crash may appear to occur first in another. However, if the events are causally connected, precedence order is preserved in all frames of reference.

## History

In 1892 and 1895, Hendrik Lorentz used a mathematical method called "local time" *t' = t – v x/c*^{2} for explaining the negative aether drift experiments.[1] However, Lorentz gave no physical explanation of this effect. This was done by Henri Poincaré who already emphasized in 1898 the conventional nature of simultaneity and who argued that it is convenient to postulate the constancy of the speed of light in all directions. However, this paper does not contain any discussion of Lorentz's theory or the possible difference in defining simultaneity for observers in different states of motion.[2][3]
This was done in 1900, when Poincaré derived local time by assuming that the speed of light is invariant within the aether. Due to the "principle of relative motion", moving observers within the aether also assume that they are at rest and that the speed of light is constant in all directions (only to first order in *v/c*). Therefore, if they synchronize their clocks by using light signals, they will only consider the transit time for the signals, but not their motion in respect to the aether. So the moving clocks are not synchronous and do not indicate the "true" time. Poincaré calculated that this synchronization error corresponds to Lorentz's local time.[4][5]
In 1904, Poincaré emphasized the connection between the principle of relativity, "local time", and light speed invariance; however, the reasoning in that paper was presented in a qualitative and conjectural manner.[6][7]

Albert Einstein used a similar method in 1905 to derive the time transformation for all orders in *v/c*, i.e., the complete Lorentz transformation. Poincaré obtained the full transformation earlier in 1905 but in the papers of that year he did not mention his synchronization procedure. This derivation was completely based on light speed invariance and the relativity principle, so Einstein noted that for the electrodynamics of moving bodies the aether is superfluous. Thus, the separation into "true" and "local" times of Lorentz and Poincaré vanishes – all times are equally valid and therefore the relativity of length and time is a natural consequence.[8][9][10]

In 1908, Hermann Minkowski introduced the concept of a world line of a particle[11] in his model of the cosmos called Minkowski space. In Minkowski's view, the naïve notion of velocity is replaced with rapidity, and the ordinary sense of simultaneity becomes dependent on hyperbolic orthogonality of spatial directions to the worldline associated to the rapidity. Then every inertial frame of reference has a rapidity and a simultaneous hyperplane.

## Thought experiments

### Einstein's train

Einstein's version of the experiment[12] presumed that one observer was sitting midway inside a speeding traincar and another was standing on a platform as the train moved past. As measured by the standing observer, the train is struck by two bolts of lightning simultaneously, but at different positions along the axis of train movement (back and front of the train car). In the inertial frame of the standing observer, there are three events which are spatially dislocated, but simultaneous: standing observer facing the moving observer (i.e., the center of the train), lightning striking the front of the train car, and lightning striking the back of the car.

Since the events are placed along the axis of train movement, their time coordinates become projected to different time coordinates in the moving train's inertial frame. Events which occurred at space coordinates in the direction of train movement happen *earlier* than events at coordinates opposite to the direction of train movement. In the moving train's inertial frame, this means that lightning will strike the front of the train car *before* the two observers align (face each other).

### The train-and-platform

A popular picture for understanding this idea is provided by a thought experiment similar to those suggested by Daniel Frost Comstock in 1910[13] and Einstein in 1917.[14][12] It also consists of one observer midway inside a speeding traincar and another observer standing on a platform as the train moves past.

A flash of light is given off at the center of the traincar just as the two observers pass each other. For the observer on board the train, the front and back of the traincar are at fixed distances from the light source and as such, according to this observer, the light will reach the front and back of the traincar at the same time.

For the observer standing on the platform, on the other hand, the rear of the traincar is moving (catching up) toward the point at which the flash was given off, and the front of the traincar is moving away from it. As the speed of light is finite and the same in all directions for all observers, the light headed for the back of the train will have less distance to cover than the light headed for the front. Thus, the flashes of light will strike the ends of the traincar at different times.

#### Spacetime diagrams

It may be helpful to visualize this situation using spacetime diagrams. For a given observer, the *t*-axis is defined to be a point traced out in time by the origin of the spatial coordinate *x*, and is drawn vertically. The *x*-axis is defined as the set of all points in space at the time *t* = 0, and is drawn horizontally. The statement that the speed of light is the same for all observers is represented by drawing a light ray as a 45° line, regardless of the speed of the source relative to the speed of the observer.

In the first diagram, the two ends of the train are drawn as grey lines. Because the ends of the train are stationary with respect to the observer on the train, these lines are just vertical lines, showing their motion through time but not space. The flash of light is shown as the 45° red lines. The points at which the two light flashes hit the ends of the train are at the same level in the diagram. This means that the events are simultaneous.

In the second diagram, the two ends of the train moving to the right, are shown by parallel lines. The flash of light is given off at a point exactly halfway between the two ends of the train, and again form two 45° lines, expressing the constancy of the speed of light. In this picture, however, the points at which the light flashes hit the ends of the train are *not* at the same level; they are *not* simultaneous.

## Lorentz transformation

The relativity of simultaneity can be demonstrated using the Lorentz transformation, which relates the coordinates used by one observer to coordinates used by another in uniform relative motion with respect to the first.

Assume that the first observer uses coordinates labeled *t, x, y,* and *z*, while the second observer uses coordinates labeled *t', x', y',* and *z'*. Now suppose that the first observer sees the second moving in the *x*-direction at a velocity *v*. And suppose that the observers' coordinate axes are parallel and that they have the same origin. Then the Lorentz transformation expresses how the coordinates are related:

where *c* is the speed of light. If two events happen at the same time in the frame of the first observer, they will have identical values of the *t*-coordinate. However, if they have different values of the *x*-coordinate (different positions in the *x*-direction), they will have different values of the *t'* coordinate, so they will happen at different times in that frame. The term that accounts for the failure of absolute simultaneity is the *v x/c*^{2}.

The equation *t' *= constant defines a "line of simultaneity" in the (*x', t' *) coordinate system for the second (moving) observer, just as the equation *t* = constant defines the "line of simultaneity" for the first (stationary) observer in the (*x, t*) coordinate system. From the above equations for the Lorentz transform it can be seen that *t'* is constant if and only if *t – v x/c*^{2} = constant. Thus the set of points that make *t* constant are different from the set of points that makes *t' *constant. That is, the set of events which are regarded as simultaneous depends on the frame of reference used to make the comparison.

Graphically, this can be represented on a space-time diagram by the fact that a plot of the set of points regarded as simultaneous generates a line which depends on the observer. In the space-time diagram, the dashed line represents a set of points considered to be simultaneous with the origin by an observer moving with a velocity *v* of one-quarter of the speed of light. The dotted horizontal line represents the set of points regarded as simultaneous with the origin by a stationary observer. This diagram is drawn using the (*x, t*) coordinates of the stationary observer, and is scaled so that the speed of light is one, i.e., so that a ray of light would be represented by a line with a 45° angle from the *x* axis. From our previous analysis, given that *v* = 0.25 and *c* = 1, the equation of the dashed line of simultaneity is *t* – 0.25*x* = 0 and with *v* = 0, the equation of the dotted line of simultaneity is *t* = 0.

In general the second observer traces out a worldline in the spacetime of the first observer described by *t* = *x*/*v*, and the set of simultaneous events for the second observer (at the origin) is described by the line *t* = *vx*. Note the multiplicative inverse relation of the slopes of the worldline and simultaneous events, in accord with the principle of hyperbolic orthogonality.

## Accelerated observers

The Lorentz-transform calculation above uses a definition of extended-simultaneity (i.e. of when and where events occur *at which you were not present*) that might be referred to as the co-moving or "tangent free-float-frame" definition. This definition is naturally extrapolated to events in gravitationally-curved spacetimes, and to accelerated observers, through use of a radar-time/distance definition that (unlike the tangent free-float-frame definition for accelerated frames) assigns a unique time and position to any event.[15]

The radar-time definition of extended-simultaneity further facilitates visualization of the way that acceleration curves spacetime for travelers in the absence of any gravitating objects. This is illustrated in the figure at right, which shows radar time/position isocontours for events in flat spacetime as experienced by a traveler (red trajectory) taking a constant proper-acceleration roundtrip. One caveat of this approach is that the time and place of remote events are not fully defined until light from such an event is able to reach our traveler.

## See also

## References

- Lorentz, Hendrik Antoon (1895), , Leiden: E.J. Brill
- Poincaré, Henri (1898–1913),
*The foundations of science*, New York: Science Press, pp. 222–234 , - Galison, Peter (2003),
*Einstein's Clocks, Poincaré's Maps: Empires of Time*, New York: W.W. Norton, ISBN 0-393-32604-7 - Poincaré, Henri (1900),
*Archives Néerlandaises des Sciences Exactes et Naturelles*,**5**: 252–278. See also the English translation. , - Darrigol, Olivier (2005), "The Genesis of the theory of relativity" (PDF),
*Séminaire Poincaré*,**1**: 1–22, doi:10.1007/3-7643-7436-5_1, ISBN 978-3-7643-7435-8 - Poincaré, Henri (1904–1906),
*Congress of arts and science, universal exposition, St. Louis, 1904*,**1**, Boston and New York: Houghton, Mifflin and Company, pp. 604–622 , - Holton, Gerald (1988),
*Thematic Origins of Scientific Thought: Kepler to Einstein*, Harvard University Press, ISBN 0-674-87747-0 - Einstein, Albert (1905), "Zur Elektrodynamik bewegter Körper" (PDF),
*Annalen der Physik*,**322**(10): 891–921, Bibcode:1905AnP...322..891E, doi:10.1002/andp.19053221004. See also: English translation. - Miller, Arthur I. (1981),
*Albert Einstein's special theory of relativity. Emergence (1905) and early interpretation (1905–1911)*, Reading: Addison–Wesley, ISBN 0-201-04679-2 - Pais, Abraham (1982),
*Subtle is the Lord: The Science and the Life of Albert Einstein*, New York: Oxford University Press, ISBN 0-19-520438-7 - Minkowski, Hermann (1909),
*Physikalische Zeitschrift*,**10**: 75–88- Various English translations on Wikisource: Space and Time

- Einstein, Albert (2017),
*Relativity - The Special and General Theory*, Samaira Book Publishers, pp. 30–33, ISBN 978-81-935401-7-6, Chapter IX - The thought experiment by Comstock described two platforms in relative motion. See: Comstock, D.F. (1910),
*Science*,**31**(803): 767–772, Bibcode:1910Sci....31..767C, doi:10.1126/science.31.803.767, PMID 17758464. , - Einstein's thought experiment used two light rays starting at both ends of the platform. See: Einstein A. (1917), , Springer
- Dolby, Carl E.; Gull, Stephen F. (December 2001). "On radar time and the twin "paradox"".
*American Journal of Physics*.**69**(12): 1257–1261. arXiv:gr-qc/0104077. Bibcode:2001AmJPh..69.1257D. doi:10.1119/1.1407254.

## External links

Special relativity at Wikibooks