Transformation of velocity exceeding light speed

[sweet springs]

In discussion with my friend, we reached a conclusion that transformation formula of velosity v to another IFR moving V, i.e.
v'=\frac{v+V}{1+vV/c^2}
is valid even if v is hypothetical velocity,i,e,
v=\frac{x_2-x_1}{t_2-t_1}
v'=\frac{x'_2-x'_1}{t'_2-t'_1}
where interval of $(t_1,x_1)\rightarrow (t'_1,x'_1)$ and $(t_2,x_2)\rightarrow (t_2',x_2')$ are time-like, space-lile, null, it doen't matter.
For example when $t_2-t_1=0$ ,$v=\pm \infty$ is trandformed to
\pm \infty \rightarrow \frac{\pm \infty + V}{1+\pm \infty V/c^2}=\frac{c^2}{V}
Of course it is over c but it seems to work describing change of synchronicity.
I have never thought of such an application of the law so appreciate your comment whether it is OK or No Good.

 

[PeterDonis]

i,e,

$$
v=\frac{x_2-x_1}{t_2-t_1}
$$
$$
v'=\frac{x'_2-x'_1}{t'_2-t'_1}
$$

where interval of $(t_1,x_1)\rightarrow (t'_1,x'_1)$ and $(t_2,x_2)\rightarrow (t_2',x_2')$ are time-like, space-lile, null, it doen't matter.

There are two problems here. First, "velocity" is $dx / dt$, not $(x_2 - x_1) / (t_2 - t_1)$. It's a derivative, not a ratio.

Second, the Lorentz transformation, which is where you're getting all this from, is only valid if $dx / dt < 1$ (or $c$ in conventional units). There is no such thing as a Lorentz transformation with $v \ge 1$, because there is no such thing as an inertial frame with a null or spacelike "time axis".

 

[sweet springs]

Thanks. I will give some more details of the discussion.

----------------------
A stationary wave
\Psi/A=sin[\omega t]sin[k z]=\frac{1}{2} cos[kz-\omega t]-\frac{1}{2} cos[-kz-\omega t]
is transfomed to moving IFR of velocity v in z direction
\Psi/A=\Psi&#039;/A&#039;= sin[\omega \gamma (t&#039;+vz&#039;/c^2)]sin[k \gamma(z&#039;+vt&#039;)]=\frac{1}{2} cos[\gamma(k-\omega v/c^2)z&#039;-\gamma(\omega-kv)t&#039;]-\frac{1}{2} cos[-\gamma(k+\omega v/c^2)z&#039;-\gamma(\omega+kv)t&#039;]
where
dispersion relation \omega=u k,
for a wave going out
\omega&#039;_1=\gamma(\omega-kv)
k&#039;_1=\gamma(k-\omega v/c^2)　
for a wave coming in
\omega&#039;_2=\gamma(\omega+kv)
k&#039;_2=-\gamma(k+\omega v/c^2)
-------------------

We can easily confirm that velocity $\omega'_1/k'_1$ $\omega'_2/k'_2$ follow the addition rule.
Furthermore as for $sin[\omega t]$ where $sin[0\cdot z + \omega t]$ means velocity $-\omega/0=\pm\infty$ ,and $sin[\omega \gamma (t'+vz'/c^2)]$ where velocity is $c^2/v > c$, these "velocities" seem satisfying the addition rule as mentioned in OP.
Is the velocity addition rule applicable also for such velocities exceeding c?

More clearly, as for the formula
x&#039;=\frac{x+V}{1+xV/c^2}
where x' is a quantity in moving IFR by velocity V, which corresponds to x in the original IFR, it is sure that this formula stands for x of ordinary velocity <c so this formula becomes the velocity addition rule in that case.
I am suggested that this formula also stands for x of extraordinary velocities exceeding c or even infinity as exemplified above. Is it all right?

PS The formula suggest that in all the IFRs, -c< ordinary speed <c and |extraordinary speed |>c . They are in the different regions and no contamination take place.

 

[PeterDonis]

Is the velocity addition rule applicable also for such velocities exceeding c?

I've already answered this--the answer is no--and explained why.

 

[sweet springs]

There are two problems here. First, "velocity" is dx/dt, not (x2−x1)/(t2−t1). It's a derivative, not a ratio.

As for the ratio , say, two events
A(t_A,z_A),B(t_B,z_A) be expressed as A(t&#039;_A,z&#039;_A),B(t&#039;_B,z&#039;_A) in change of IFRs where
t&#039;_A=\gamma(t_A+Vz_A/c^2), z&#039;_A=\gamma(z_A+Vt_A)
t&#039;_B=\gamma(t_B+Vz_B/c^2), z&#039;_B=\gamma(z_B+Vt_B)
Let us see how the ratio would be transformed
\frac{z&#039;_B-z&#039;_A}{t&#039;_B-t&#039;_A}=\frac{\gamma(z_B-z_A)+\gamma V(t_B-t_A)}{\gamma(t_B-t_A)+\gamma V(z_A-z_B)/c^2}=\frac{\frac{z_B-z_A}{t_B-t_A}+V}{1+V/c^2 \frac{z_B-z_A}{t_B-t_A}}
It is same as the velocity addition rule. There is no condition put between A and B, e.g. interval is time-like, space-like or null.

This includes the case if we take both A and B is on the same world line and very close to infinity zero then the ratio turns out to be velocity dz/dt.

 

[PeterDonis]

There is no condition put between A and B, e.g. interval is time-like, space-like or null.

You are incorrect. The transformation you are using is a Lorentz transformation, which is only valid if the relative velocity is less than the speed of light. I have already explained why.

Since your question has been answered and you are simply repeating incorrect statements at this point, this thread is closed.