What is the Lorentz Transformation Equation and its Use in Relativity?

ggolu2
Messages
12
Reaction score
0
I really don't understand what it is and what is the use of constant, like in this equation of transformation.
x=k(x' + vt).
The equation can also be good if it is just like this,
x=x' + vt

Thank you.
 
Physics news on Phys.org
So you are saying the $$F=\frac{m_1m_2}{r^2}$$?

That is certainly not true.
Do you believe that ##F=x##?(Hookes law)
Yes this is valid for a elastic constant of 1 but not valid for any other constant.
 
No this is about theory of special relativity. It uses transformation law to derive the equations of Lorentz transformation. And my question is about the use of the constant, I mean how they thought that there must be a constant such that this equation holds good at high speeds.
 
ggolu2 said:
I really don't understand what it is and what is the use of constant, like in this equation of transformation.
x=k(x' + vt).
The equation can also be good if it is just like this,
x=x' + vt

Thank you.

Are you sure there is constant "k"?
Cause I read today Lorentz,and I saw nothing about that?
Also if there is,then what is the value of "k" ?
 
The Lorentz transformation for x is
$$x^\prime = \frac{x - vt}{\sqrt{1 - v^2/c^2}}$$
You should be able to read off the value of k from that equation. (We usually call it ##\gamma##.)
 
Last edited:
OK, so this has bugged me for a while about the equivalence principle and the black hole information paradox. If black holes "evaporate" via Hawking radiation, then they cannot exist forever. So, from my external perspective, watching the person fall in, they slow down, freeze, and redshift to "nothing," but never cross the event horizon. Does the equivalence principle say my perspective is valid? If it does, is it possible that that person really never crossed the event horizon? The...
ASSUMPTIONS 1. Two identical clocks A and B in the same inertial frame are stationary relative to each other a fixed distance L apart. Time passes at the same rate for both. 2. Both clocks are able to send/receive light signals and to write/read the send/receive times into signals. 3. The speed of light is anisotropic. METHOD 1. At time t[A1] and time t[B1], clock A sends a light signal to clock B. The clock B time is unknown to A. 2. Clock B receives the signal from A at time t[B2] and...
From $$0 = \delta(g^{\alpha\mu}g_{\mu\nu}) = g^{\alpha\mu} \delta g_{\mu\nu} + g_{\mu\nu} \delta g^{\alpha\mu}$$ we have $$g^{\alpha\mu} \delta g_{\mu\nu} = -g_{\mu\nu} \delta g^{\alpha\mu} \,\, . $$ Multiply both sides by ##g_{\alpha\beta}## to get $$\delta g_{\beta\nu} = -g_{\alpha\beta} g_{\mu\nu} \delta g^{\alpha\mu} \qquad(*)$$ (This is Dirac's eq. (26.9) in "GTR".) On the other hand, the variation ##\delta g^{\alpha\mu} = \bar{g}^{\alpha\mu} - g^{\alpha\mu}## should be a tensor...
Back
Top