Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Four-velocity
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
{{Short description|Analogue of velocity in four-dimensional spacetime}} In [[physics]], in particular in [[special relativity]] and [[general relativity]], a '''four-velocity''' is a [[four-vector]] in four-dimensional [[spacetime]]<ref group=nb>Technically, the four-vector should be thought of as residing in the [[tangent space]] of a point in spacetime, spacetime itself being modeled as a [[smooth manifold]]. This distinction is significant in general relativity.</ref> that represents the relativistic counterpart of [[velocity]], which is a [[Three-dimensional space|three-dimensional]] [[Vector (mathematics and physics)|vector]] in space. Physical [[Event (relativity)|events]] correspond to mathematical points in time and space, the set of all of them together forming a mathematical model of physical four-dimensional spacetime. The history of an object traces a curve in spacetime, called its [[world line]]. If the object has [[Mass in special relativity|mass]], so that its speed is necessarily less than the [[speed of light]], the world line may be [[Parametrization (geometry)|parametrized]] by the [[proper time]] of the object. The four-velocity is the rate of change of [[four-position]] with respect to the proper time along the curve. The velocity, in contrast, is the rate of change of the position in (three-dimensional) space of the object, as seen by an observer, with respect to the observer's time. The value of the [[Magnitude_(mathematics)#Pseudo-Euclidean_space|magnitude]] of an object's four-velocity, i.e. the quantity obtained by applying the [[Metric tensor (general_relativity)|metric tensor]] {{math|''g''}} to the four-velocity {{math|'''U'''}}, that is {{math|1={{norm|'''U'''}}<sup>2</sup> = '''U''' ⋅ '''U''' = ''g''<sub>''μν''</sub>''U''<sup>''ν''</sup>''U''<sup>''μ''</sup>}}, is always equal to {{math|±''c''<sup>2</sup>}}, where {{mvar|c}} is the speed of light. Whether the plus or minus sign applies depends on the choice of [[metric signature]]. For an object at rest its four-velocity is parallel to the direction of the time coordinate with {{math|1=''U''<sup>0</sup> = ''c''}}. A four-velocity is thus the normalized future-directed timelike tangent vector to a world line, and is a [[contravariant vector]]. Though it is a vector, addition of two four-velocities does not yield a four-velocity: the space of four-velocities is not itself a [[vector space]].<ref group=nb>The set of four-velocities is a subset of the tangent space (which ''is'' a vector space) at an event. The label ''four-vector'' stems from the behavior under [[Lorentz transformation]]s, namely under which particular [[Representation theory of the Lorentz group|representation]] they transform.</ref>
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)