Lorentz Transformation of relative velocity

In summary, the task is to find the relative velocity and speed of two particles with velocities u and v in frame S, in frame S'. The relative velocity of the frame is represented by s, and the transformation of velocities is given by \vec u' = \frac{1}{1 - \frac{\vec u \cdot \vec s}{c^2}}\left[ \frac{1}{\gamma_s} \vec u - \left( 1 - \frac{\vec u \cdot \vec s }{c^2}\frac{\gamma_s}{1 + \gamma_s} \right) \vec s \right] and \vec v' = \frac{1}{1 - \frac{\vec
  • #1
unscientific
1,734
13

Homework Statement


If two particles have velocities u and v in frame S, find their relative speed in frame S'.
2qbrhj9.png

Homework Equations

The Attempt at a Solution


Isn't it strange that the relative speed doesn't depend on the velocity of the frame, ##\vec s##?

Since the two particles have velocities ##\vec u## and ##\vec v## in some reference frame S, I am to find the relative velocity and speed in frame S'.

Letting the relative velocity of the frame be ## \vec s##, the transformation of velocities are:

[tex]
\vec u' = \frac{1}{1 - \frac{\vec u \cdot \vec s}{c^2}}\left[ \frac{1}{\gamma_s} \vec u - \left( 1 - \frac{\vec u \cdot \vec s }{c^2}\frac{\gamma_s}{1 + \gamma_s} \right) \vec s \right] [/tex]

[tex]
\vec v' = \frac{1}{1 - \frac{\vec v \cdot \vec s}{c^2}}\left[ \frac{1}{\gamma_s} \vec v - \left( 1 - \frac{\vec v \cdot \vec s }{c^2}\frac{\gamma_s}{1 + \gamma_s} \right) \vec s \right] [/tex]

Taking ##\vec u' - \vec v'## only gives me components in ##\vec u, \vec v, \vec s ##. How do I extract the magnitude?
 
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  • #2
Note: the "speed of particle B relative to particle A" is the speed of particle B as measured in the reference frame moving with particle A.

So, what should you choose for primed frame, S'? Hence, what should be the velocity ##\vec{s}##?
 
  • #3
TSny said:
Note: the "speed of particle B relative to particle A" is the speed of particle B as measured in the reference frame moving with particle A.

So, what should you choose for primed frame, S'? Hence, what should be the velocity ##\vec{s}##?

Yes, I misread the question. ##\vec s## is simply ##\vec v##. Then all that remains is to find the magnitude. But it looks very messy due to the ##\gamma_v##

[tex]
\vec w = \frac{1}{1 - \frac{\vec u \cdot \vec v}{c^2}}\left[ \frac{1}{\gamma_v} \vec u - \left( 1 - \frac{\vec u \cdot \vec v }{c^2}\frac{\gamma_v}{1 + \gamma_v} \right) \vec v \right] [/tex]

To find the magnitude I would take ##\sqrt{ \vec w \cdot \vec w}##
 
  • #4
OK, that looks good. Yes, it is messy to deal with all the gamma factors. It will work out.

Another approach is to work out the x and y components of ##\vec{w}##, where the x direction is parallel to ##\vec{v}## and the y direction is perpendicular to ##\vec{v}## such that ##\vec{u}## is in the x-y plane.

There are well-known formulas for calculating these components. See below. These can be derived from your general formula.
 

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  • #5
TSny said:
OK, that looks good. Yes, it is messy to deal with all the gamma factors. It will work out.

Another approach is to work out the x and y components of ##\vec{w}##, where the x direction is parallel to ##\vec{v}## and the y direction is perpendicular to ##\vec{v}## such that ##\vec{u}## is in the x-y plane.

There are well-known formulas for calculating these components. See below. These can be derived from your general formula.

I derived the expression ##
\vec w = \frac{1}{1 - \frac{\vec u \cdot \vec v}{c^2}}\left[ \frac{1}{\gamma_v} \vec u - \left( 1 - \frac{\vec u \cdot \vec v }{c^2}\frac{\gamma_v}{1 + \gamma_v} \right) \vec v \right] ## by using ## u_{||} = \frac{(\vec u \cdot \vec v) \vec v}{|\vec v|^2} ## and ## u_{\perp} = \vec u - \vec u_{||} ##.

I thought it would be easier, because finding the magnitudes of the horizontal and vertical components would involve angles and such.
 
  • #6
unscientific said:
I thought it would be easier, because finding the magnitudes of the horizontal and vertical components would involve angles and such.

If you want to work with the components, you can write ## u_{||} =u \cos \theta## and ## u_{\perp} =u \sin \theta##. Then the velocity-addition formulas for the two components will be fairly easy to work out.
 
  • #7
TSny said:
If you want to work with the components, you can write ## u_{||} =u \cos \theta## and ## u_{\perp} =u \sin \theta##. Then the velocity-addition formulas for the two components will be fairly easy to work out.

So do you reckon it's easier to simply take ##\left[ \frac{u cos \theta - v}{1 - \frac{uv cos\theta}{c^2}} \right]^2 + \left[ \frac{u sin\theta}{\gamma (1- \frac{uv cos \theta}{c^2})} \right]^2 ##?
 
  • #8
unscientific said:
So do you reckon it's easier to simply take ##\left[ \frac{u cos \theta - v}{1 - \frac{uv cos\theta}{c^2}} \right]^2 + \left[ \frac{u sin\theta}{\gamma (1- \frac{uv cos \theta}{c^2})} \right]^2 ##?

Yes. Note that in the denominators you have ##1 - \frac{uv cos\theta}{c^2}## which is part of the answer you want.
 

Related to Lorentz Transformation of relative velocity

1. What is the Lorentz Transformation of relative velocity?

The Lorentz Transformation of relative velocity is a mathematical formula used in special relativity to calculate the velocity of an object in one frame of reference as observed from another frame of reference that is moving at a constant velocity relative to the first frame.

2. What is the difference between relative velocity and absolute velocity?

Relative velocity is the velocity of an object as observed from a specific frame of reference, while absolute velocity is the velocity of an object as measured in an absolute frame of reference, such as the speed of light in a vacuum.

3. How is the Lorentz Transformation of relative velocity derived?

The Lorentz Transformation of relative velocity is derived from the principles of special relativity, particularly the concept of time dilation and length contraction. It is based on the Lorentz factor, which takes into account the relative velocity between two frames of reference.

4. What are the applications of Lorentz Transformation of relative velocity?

The Lorentz Transformation of relative velocity is used in various fields of physics, including astrophysics, particle physics, and nuclear physics. It is also important in practical applications, such as GPS technology and particle accelerators.

5. Can the Lorentz Transformation of relative velocity be applied to all types of motion?

No, the Lorentz Transformation of relative velocity is only applicable to motion that is constant in both speed and direction. It cannot be used for accelerating objects or objects that are changing direction.

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