relative velocity

We begin with relative motion in the classical, (or non-relativistic, or the Newtonian approximation) that all speeds are much less than the speed of light. This limit is associated with the Galilean transformation. The figure shows a man on top of a train, at the back edge. At 1:00 pm he begins to walk forward at a walking speed of 10 km/h (kilometers per hour). The train is moving at 40 km/h. The figure depicts the man and train at two different times: first, when the journey began, and also one hour later at 2:00 pm. The figure suggests that the man is 50 km from the starting point after having traveled (by walking and by train) for one hour. This, by definition, is 50 km/h, which suggests that the prescription for calculating relative velocity in this fashion is to add the two velocities.

The diagram displays clocks and rulers to remind the reader that while the logic behind this calculation seem flawless, it makes false assumptions about how clocks and rulers behave. (See The train-and-platform thought experiment.) To recognize that this classical model of relative motion violates special relativity, we generalize the example into an equation:

:$\backslash underbrace\{\backslash mathbf\; v\_\{M\backslash mid\; E\}\}\_\backslash text\{50\; km/h\}\; =\; \backslash underbrace\{\backslash mathbf\; v\_\{M\backslash mid\; T\}\}\_\backslash text\{10\; km/h\}\; +\; \backslash underbrace\{\backslash mathbf\; v\_\{T\backslash mid\; E\}\}\_\backslash text\{40\; km/h\},$

where:

:$\backslash mathbf\; v\_\{M\backslash mid\; E\}$ is the velocity of the Man relative to Earth,

:$\backslash mathbf\; v\_\{M\backslash mid\; T\}$ is the velocity of the Man relative to the Train,

:$\backslash mathbf\; v\_\{T\backslash mid\; E\}$ is the velocity of the Train relative to Earth.

Fully legitimate expressions for "the velocity of A relative to B" include "the velocity of A with respect to B" and "the velocity of A in the coordinate system where B is always at rest". The violation of special relativity occurs because this equation for relative velocity falsely predicts that different observers will measure different speeds when observing the motion of light. For example, replace the "Man" by a photon traveling at the speed of light.

File:Relative velocity.svg

The figure shows two objects A and B moving at constant velocity. The equations of motion are:

:$\backslash mathbf\; r\_A=\backslash mathbf\; r\_\{Ai\}+\backslash mathbf\; v\_A\; t,$

:$\backslash mathbf\; r\_B=\backslash mathbf\; r\_\{Bi\}+\; \backslash mathbf\; v\_B\; t,$

where the subscript i refers to the initial displacement (at time t equal to zero). The difference between the two displacement vectors, $\backslash mathbf\; r\_B-\backslash mathbf\; r\_A$, represents the location of B as seen from A.

: $\backslash mathbf\; r\_B-\backslash mathbf\; r\_A=\; \backslash underbrace\{\backslash mathbf\; r\_\{Bi\}-\backslash mathbf\; r\_\{Ai\}\}\_\backslash text\{initial\; separation\}\; +\; \backslash underbrace\{(\backslash mathbf\; v\_B-\backslash mathbf\; v\_A\; )\; t\}\_\backslash text\{relative\; velocity\}.$

Hence:

:$\backslash mathbf\; v\_\{B\backslash mid\; A\}=\backslash mathbf\; v\_B-\backslash mathbf\; v\_A.$

After making the substitutions $\backslash mathbf\; v\_\{A|C\}=\backslash mathbf\; v\_A$ and $\backslash mathbf\; v\_\{B|C\}=\backslash mathbf\; v\_B$, we have:

: $\backslash mathbf\; v\_\{B\backslash mid\; A\}\; =\; \backslash mathbf\; v\_\{B\backslash mid\; C\}-\backslash mathbf\; v\_\{A\backslash mid\; C\}\; \backslash Rightarrow$   $\backslash mathbf\; v\_\{B\backslash mid\; C\}=\backslash mathbf\; v\_\{B\backslash mid\; A\}\; +\backslash mathbf\; v\_\{A\backslash mid\; C\}.$

To construct a theory of relative motion consistent with the theory of special relativity, we must adopt a different convention. Continuing to work in the (non-relativistic) Newtonian limit we begin with a Galilean transformation in one dimension:This result is valid if all motion is restricted to the x-axis, but can be easily generalized by replacing the first equation by $\backslash mathbf\; r\backslash ,\text{'}=\backslash mathbf\; r-\backslash mathbf\; vt$

:$x\text{'}=x-vt$

:$t\text{'}=t$

where x' is the position as seen by a reference frame that is moving at speed, v, in the "unprimed" (x) reference frame.It is easy to be confused about the minus sign before v, or whether v is defined in the prime or unprimed reference frame. It might help to visualize the fact that if x = vt, then x′ = 0, meaning that a particle that is following the path x = vt is at rest in the primed reference frame. Taking the differential of the first of the two equations above, we have, $dx\text{'}=dx-v\; \backslash ,\; dt$, and what may seem like the obviousKeep in mind that, due to time dilation, dt = dt′ is valid only in the approximation that the speed is much less than that of light. statement that $dt\text{'}=dt$, we have:

:$\backslash frac\{dx\text{'}\}\{dt\text{'}\}=\backslash frac\{dx\}\{dt\}-v$

To recover the previous expressions for relative velocity, we assume that particle A is following the path defined by dx/dt in the unprimed reference (and hence dx′/dt′ in the primed frame). Thus $dx/dt\; =\; v\_\{A\backslash mid\; O\}$ and $dx\text{'}/dt\; =\; v\_\{A\backslash mid\; O\text{'}\}$, where $O$ and $O\text{'}$ refer to motion of A as seen by an observer in the unprimed and primed frame, respectively. Recall that v is the motion of a stationary object in the primed frame, as seen from the unprimed frame. Thus we have $v=v\_\{O\text{'}\backslash mid\; O\}$, and:

:$v\_\{A\backslash mid\; O\text{'}\}=\; v\_\{A\backslash mid\; O\}-v\_\{O\text{'}\backslash mid\; O\}\; \backslash Rightarrow\; v\_\{A\backslash mid\; O\}\; =\; v\_\{A\backslash mid\; O\text{'}\}\; +\; v\_\{O\text{'}\backslash mid\; O\},$

where the latter form has the desired (easily learned) symmetry.

{{further|Special relativity#Composition of velocities{{!}}Special relativity – Composition of velocities|Velocity-addition formula}}

As in classical mechanics, in special relativity the relative velocity $\backslash mathbf\; v\_\backslash mathrm\{B|A\}$ is the velocity of an object or observer B in the rest frame of another object or observer A. However, unlike the case of classical mechanics, in Special Relativity, it is generally not the case that

:$\backslash mathbf\; v\_\backslash mathrm\{B|A\}=-\backslash mathbf\; v\_\backslash mathrm\{A|B\}$

This peculiar lack of symmetry is related to Thomas precession and the fact that two successive Lorentz transformations rotate the coordinate system. This rotation has no effect on the magnitude of a vector, and hence relative speed is symmetrical.

:$\backslash |\backslash mathbf\; v\_\backslash mathrm\{B|A\}\backslash |=\backslash |\backslash mathbf\; v\_\backslash mathrm\{A|B\}\backslash |=v\_\backslash mathrm\{B|A\}=v\_\backslash mathrm\{A|B\}$

In the case where two objects are traveling in parallel directions, the relativistic formula for relative velocity is similar in form to the formula for addition of relativistic velocities.

:$\backslash mathbf\; v\_\backslash mathrm\{B|A\}=\backslash frac\{\backslash mathbf\; v\_\backslash mathrm\{B\}-\backslash mathbf\; v\_\backslash mathrm\{A\}\}\{1-\backslash frac\{\backslash mathbf\; v\_\backslash mathrm\{A\}\backslash mathbf\; v\_\backslash mathrm\{B\}\}\{c^2\}\}$

The relative speed is given by the formula:

:$v\_\backslash mathrm\{B|A\}=\backslash frac\{\backslash left\; |\; \backslash mathbf\; v\_\backslash mathrm\{B\}-\backslash mathbf\; v\_\backslash mathrm\{A\}\backslash right\; |\; \}\{1-\backslash frac\{\backslash mathbf\; v\_\backslash mathrm\{A\}\backslash mathbf\; v\_\backslash mathrm\{B\}\}\{c^2\}\}$

In the case where two objects are traveling in perpendicular directions, the relativistic relative velocity $\backslash mathbf\; v\_\backslash mathrm\{B|A\}$ is given by the formula:

:$\backslash mathbf\; v\_\backslash mathrm\{B|A\}=\{\backslash frac\{\backslash mathbf\; v\_\backslash mathrm\{B\}\}\{\backslash gamma\_\backslash mathrm\{A\}\}\}-\backslash mathbf\; v\_\backslash mathrm\{A\}$

where

:$\backslash gamma\_\backslash mathrm\{A\}=\backslash frac\{1\}\{\backslash sqrt\{1\; -\; \backslash left(\; \backslash frac\{v\_\backslash mathrm\{A\}\}\{c\}\; \backslash right)^2\}\}$

The relative speed is given by the formula

:$v\_\backslash mathrm\{B|A\}\; =\; \backslash frac\{\backslash sqrt\{c^4\; -\; \backslash left(c^2-v\_\backslash mathrm\{A\}^2\backslash right)\; \backslash left(c^2\; -v\_\backslash mathrm\{B\}^2\backslash right)\}\}\{c\}$

The general formula for the relative velocity $\backslash mathbf\; v\_\backslash mathrm\{B|A\}$ of an object or observer B in the rest frame of another object or observer A is given by the formula:Fock 1964 The theory of Space Time and Gravitation, retrieved from https://archive.org/details/TheTheoryOfSpaceTimeGravitation

: $$

\mathbf v_\mathrm{B|A} = \frac 1 {\gamma_\mathrm{A} \left(1-\frac{\mathbf v_\mathrm{A}\mathbf v_\mathrm{B}}{c^2} \right )} \left[ \mathbf v_\mathrm{B}-\mathbf v_\mathrm{A}+\mathbf v_\mathrm{A}(\gamma_\mathrm{A}-1) \left( \frac{\mathbf v_\mathrm{A}\cdot \mathbf v_\mathrm{B}}{v_\mathrm{A}^2}-1 \right) \right]

where

: $$

\gamma_\mathrm{A} = \frac{1}{\sqrt{1-\left(\frac{v_\mathrm{A}}{c}\right)^2}}

The relative speed is given by the formula

:$v\_\backslash mathrm\{B|A\}=\backslash sqrt\{1-\backslash frac\{\backslash left(c^2-v\_\backslash mathrm\{A\}^2\backslash right)\backslash left(c^2\; -v\_\backslash mathrm\{B\}^2\backslash right)\}\{\backslash left(c^2-\backslash mathbf\; v\_\backslash mathrm\{A\}\; \backslash cdot\; \backslash mathbf\; v\_\backslash mathrm\{B\}\backslash right)^2\}\}\; \backslash cdot\; c$

• Doppler effect
• {{slink|Non-Euclidean geometry|Kinematic geometries}}
• Peculiar velocity
• Proper motion
• Range rate
• Radial velocity
• Rapidity
• Relativistic speed
• Space velocity (astronomy)

{{reflist|group=note}}

{{Reflist}}

• Alonso & Finn, Fundamental University Physics {{ISBN|0-201-56518-8}}
• Greenwood, Donald T, Principles of Dynamics.
• Goodman and Warner, Dynamics.
• Beer and Johnston, Statics and Dynamics.
• McGraw Hill Dictionary of Physics and Mathematics.
• Rindler, W., Essential Relativity.
• KHURMI R.S., Mechanics, Engineering Mechanics, Statics, Dynamics

• [http://hyperphysics.phy-astr.gsu.edu/Hbase/relmot.html Relative Motion at HyperPhysics]
• [http://physics.bu.edu/~duffy/java/RelV2.html A Java applet illustrating Relative Velocity, by Andrew Duffy]
• [http://www.fizkapu.hu/fizfilm/fizfilm1.html Relatív mozgás (1)...(3)] Relative motion of two train (1)...(3). Videos on the portal [http://www.fizkapu.hu FizKapu]. {{in lang|hu}}
• [http://www.fizkapu.hu/fizfilm/fizfilm1.html Sebességek összegzése] Relative tranquility of trout in creek. Video on the portal [http://www.fizkapu.hu FizKapu]. {{in lang|hu}}

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Category:Physical quantities

Category:Classical mechanics

Velocity

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