Modern Physics/Addition of Velocities

From Wikibooks, open books for an open world
< Modern Physics(Redirected from Modern Physics:Addition of Velocities)
Jump to: navigation, search

Special Relativity
1 - 2 - 3 - 4 - 5 - 6



In classical physics, velocities simply add. If an object moves with speed u in one reference frame, which is itself moving at v with respect to a second frame, the object moves at speed u+v in that second frame.

This is inconsistant with relativity because it predicts that if the speed of light is c in the first frame it will be v+c in the second.

We need to find an alternative formula for combining velocities. We can do this with the Lorentz transform.

Because the factor v/c will keep recurring we shall call that ratio β.

We are considering three frames; frame O, frame O' which moves at speed u with respect to frame O, and frame O" which moves at speed v with respect to frame O'.

We want to know the speed of O" with respect to frame O,U which would classically be u+v.

The transforms from O to O' and O' to O" can be written as matrix equations,


\begin{pmatrix} x' \\ ct' \end{pmatrix} = 
\gamma \begin{pmatrix} 1 & - \beta \\ -\beta & 1 \end{pmatrix}
\begin{pmatrix} x \\ ct \end{pmatrix} \quad
\begin{pmatrix} x'' \\ t'' \end{pmatrix} = \gamma' 
\begin{pmatrix} 1 & - \beta' \\ -\beta' & 1 \end{pmatrix}
\begin{pmatrix} x' \\ ct' \end{pmatrix}

where we are defining the β's and γ's as

\begin{matrix}
\beta = \frac{u}{c} & \gamma = \frac{1}{\sqrt{1-\beta^2 }} \\
\beta^\prime = \frac{v}{c} & 
\gamma^\prime  = \frac{1}{\sqrt{1-{\beta^\prime}^2 }} 
\end{matrix}

We can combine these to get the relationship between the O and O" coordinates simply by multiplying the matrices, giving


\begin{pmatrix} x'' \\ ct'' \end{pmatrix} = \gamma \gamma^\prime 
\begin{pmatrix} 1+\beta \beta' & - (\beta + \beta') \\
- (\beta + \beta')  & 1+\beta \beta'  \end{pmatrix}
\begin{pmatrix} x \\ ct \end{pmatrix} \quad (1)

This should be the same as the Lorentz transform between the two frames,


\begin{pmatrix} x'' \\ ct'' \end{pmatrix} = 
\gamma'' \begin{pmatrix} 1 & - \beta'' \\ -\beta'' & 1 \end{pmatrix}
\begin{pmatrix} x \\ ct \end{pmatrix} \quad (2) \mbox{  where }
\begin{matrix} \beta'' & = & \frac{U}{c} \\
\gamma'' & = & \frac{1}{\sqrt{1-{\beta''}^2 }} \end{matrix}

These two sets of equations do look similar. We can make them look more similar still by taking a factor of 1+ββ' out of the matrix in (1) giving#


\begin{pmatrix} x'' \\ ct'' \end{pmatrix} = \gamma \gamma' (1+\beta \beta')  
\begin{pmatrix} 1 & - \frac{\beta + \beta'}{1+\beta \beta'} \\
- \frac{\beta + \beta'}{1+\beta \beta'}  & 1+  \end{pmatrix}
\begin{pmatrix} x \\ ct \end{pmatrix}

This will be identical with equation 2 if

\beta''=\frac{\beta + \beta'}{1+\beta \beta'} \mbox{ (3a)   and } 
\gamma'' = \gamma \gamma' (1+\beta \beta')  \mbox{ (3b)}

Since the two equations must give identical results, we know these conditions must be true.

Writing the β's in terms of the velocities equation 3a becomes

\frac{U}{c}=\frac{\frac{u}{c} + \frac{v}{c}}{1+\frac{uv}{c^2}}

which tells us U in terms of u and v.

A little algebra shows that this implies equation 3b is also true

Multiplying by c we can finally write.

U = \frac{u+v}{1+\frac{uv}{c^2}}

Notice that if u or v is much smaller than c the denominator is approximately 1, and the velocities approximately add but if either u or v is c then so is U, just as we expected.