Doubt regarding derivation of Lorentz Transformations.

In summary, the conversation discusses the derivation of the Lorentz transformations in the Special Theory of Relativity. The assumptions made and the need for the invariance of the speed of light are explained. It is also noted that the assumptions in Newtonian mechanics lead to the Galilei transformation.
  • #1
Kaguro
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I have just started learning the Special Theory of Relativity. While deriving, I am facing some problems. I obviously have made some kind of mistake while using the equations...
What is wrong if I don't use the time transformation equation in Event #2?
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  • #2
Since y and z aren't involved, let's simplify to just talk about x and t.

Then a Lorentz transformation transforms a pair (x,t) into another pair, (x',t'). We're assuming that ##x' = Ax + Bt## and ##t' = Dx + Et##. Maybe it's clearer if we write them as functions:

##F_{x'}(x,t) = Ax + Bt##
##F_{t'}(x,t) = Dx + Et##

Then we have the assumptions:

Assumption 1: When ##x'=0##, ##x=vt##.

This means that the function ##F_{x'}(x,t)## satisfies ##F_{x'}(vt, t) = 0##. This implies that ##B = -vA##.

Assumption 2: When ##x=0##, ##x'=-vt'##.

This means that the functions ##F_{x'}(x,t)## and ##F_{t'}(x,t)## satisfy:

##F_{x'}(0, t) = -v F_{t'}(0, t)##.

So this implies that ##A\cdot 0 + B t = -v (D \cdot 0 + E t)##. So ##B = -vE##.

So you can conclude that ##E = A## and ##B = -vA##. But you can't conclude that ##D = 0##. To get ##D##, you need another assumption. That's usually the invariance of the speed of light:

Assumption 3: When ##x=ct##, then ##x' = c t'##.

In terms of functions,

##F_{x'}(ct, t) = c F_{t'}(ct, t)##
 
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  • #3
stevendaryl said:
Since y and z aren't involved, let's simplify to just talk about x and t.

Then a Lorentz transformation transforms a pair (x,t) into another pair, (x',t'). We're assuming that ##x' = Ax + Bt## and ##t' = Dx + Et##. Maybe it's clearer if we write them as functions:

##F_{x'}(x,t) = Ax + Bt##
##F_{t'}(x,t) = Dx + Et##

Then we have the assumptions:

Assumption 1: When ##x'=0##, ##x=vt##.

This means that the function ##F_{x'}(x,t)## satisfies ##F_{x'}(vt, t) = 0##. This implies that ##B = -vA##.

Assumption 2: When ##x=0##, ##x'=-vt'##.

This means that the functions ##F_{x'}(x,t)## and ##F_{t'}(x,t)## satisfy:

##F_{x'}(0, t) = -v F_{t'}(0, t)##.

So this implies that ##A\cdot 0 + B t = -v (D \cdot 0 + E t)##. So ##B = -vE##.

So you can conclude that ##E = A## and ##B = -vA##. But you can't conclude that ##D = 0##. To get ##D##, you need another assumption. That's usually the invariance of the speed of light:

Assumption 3: When ##x=ct##, then ##x' = c t'##.

In terms of functions,

##F_{x'}(ct, t) = c F_{t'}(ct, t)##
Wow! Thank you very much! You explained very nicely. I was finally able to derive the Lorentz Transformations.
 
  • #4
stevendaryl said:
So you can conclude that ##E = A## and ##B = -vA##. But you can't conclude that ##D = 0##. To get ##D##, you need another assumption. That's usually the invariance of the speed of light:

Assumption 3: When ##x=ct##, then ##x' = c t'##.

In terms of functions,

##F_{x'}(ct, t) = c F_{t'}(ct, t)##

Just to highlight the difference to Newtonian mechanics. A different assumption (and an incompatible one at that) would be ##t' = t##, which directly would imply that ##D = 0## and ##E = 1## and therefore leads to the Galilei transformation
$$
x' = x - vt, \quad t' = t.
$$
It is important to note that the special principle of relativity is still valid in Newtonian mechanics, what really changes when going to SR is the assumption that the speed of light is invariant replacing the assumption that there is a universal time.
 
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Related to Doubt regarding derivation of Lorentz Transformations.

1. What are the Lorentz Transformations and why are they important in science?

The Lorentz Transformations are a set of mathematical equations that describe how time and space coordinates change between two reference frames that are moving relative to each other at a constant velocity. They are important in science because they form the basis of the theory of special relativity, which explains the behavior of objects moving at high speeds.

2. How were the Lorentz Transformations derived?

The Lorentz Transformations were first derived by Dutch physicist Hendrik Lorentz in the late 19th century. He used a combination of mathematical equations and physical principles to describe the transformation of coordinates between two reference frames that are moving relative to each other at a constant velocity.

3. What is the significance of the speed of light in the Lorentz Transformations?

The speed of light, denoted by the letter 'c', is a fundamental constant in the Lorentz Transformations. It is the maximum speed at which any object can travel in the universe, and it plays a crucial role in the equations that describe the relationship between time and space in special relativity.

4. Are the Lorentz Transformations applicable to all types of motion?

No, the Lorentz Transformations are only applicable to motion that is constant and uniform. They do not accurately describe the behavior of objects that are accelerating or decelerating, or those that are experiencing non-uniform motion.

5. How have the Lorentz Transformations been tested and confirmed?

The Lorentz Transformations have been tested and confirmed through numerous experiments and observations, such as the Michelson-Morley experiment and the measurement of time dilation in high-speed particle accelerators. In addition, they are a fundamental part of the theory of special relativity, which has been extensively tested and validated through various experiments and observations.

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