PlanetPhysics/Velocity

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The velocity of an [[../TrivialGroupoid/|object]] is the time derivative of its [[../Position/|position]]. It is usually denoted by the symbol v or by x˙ (where x stands for position and the dot for the time derivative). Velocity can be considered either as a [[../Vectors/|vector]] quantity or as a [[../Vectors/|scalar]] quantity. If there is more than one spatial dimension and the direction of [[../CosmologicalConstant/|motion]] is important, the vector quantity 𝐯 is used. In the case of one spatial dimension, it is common to view the velocity as a scalar quantity, v (although it is formally a vector with only one component). In both cases, if only the [[../AbsoluteMagnitude/|magnitude]] of the velocity is of importance, the speed can be used, which is defined as the absolute value of the velocity and is also denoted by v, or by |𝐯|.

The SI unit of velocity is m/s (metres per second). Other units of velocity are also used, such as kilometres per hour (km/h) and the [[../CosmologicalConstant/|speed of light]], c=299792458m/s.

The definition of velocity can be written as 𝐯d𝐱dt. In addition to this definition of velocity as the instantaneous rate of change of the position, the average velocity , or the change in position Δ𝐱 over a specified period of time Δt, is also used: 𝐯¯Δ𝐱Δt.

In [[../MathematicalFoundationsOfQuantumTheories/|classical mechanics]], the velocity of an object with [[../Mass/|mass]] m enters into the equations for its [[../Momentum/|momentum]], 𝐩m𝐯 and its [[../KineticEnergy/|kinetic energy]], Ekin12mv2. Notice that this last equation is an example where only the speed of the object, and not the direction of motion, is important.

In special (and general) relativity, there are two distinct [[../PreciseIdea/|concepts]] of velocity. The first, called coordinate velocity , is the rate of change of the position of an object with respect to time as measured by the observer : vμdxμdt. The second, called proper velocity or world velocity , is the derivative of the position of the object with respect to its proper time , τ: uμdxμdτ Only the proper velocity is a vector in the full sense of the word: to express the proper velocity in a different coordinate [[../SimilarityAndAnalogousSystemsDynamicAdjointnessAndTopologicalEquivalence/|system]], all that needs to be done is multiplying the vector on the left by the Jacobian [[../Matrix/|matrix]] of the coordinate transformation (in the case of [[../CosmologicalConstant/|Lorentz transformations]] in [[../SR/|special relativity]], this is just [[../LorentzTransformation/|The Lorentz transformation]] matrix itself). In mathematical terms, this is a consequence of the fact that the proper velocity is a tangent vector to the spacetime [[../NoncommutativeGeometry4/|manifold]]. To express the coordinate velocity in a different coordinate system, on the other hand, the [[../Bijective/|relation]] between coordinate time and proper time in each of the two coordinate systems needs to be taken into account.

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