Now it remains to be shown that A = B. I'll leave that to you.

In summary, the expression x'^2 + y'^2 _ z'^2 -c^2t'^2 is equal to x^2 + y^2 + z^2 -c^2t^2, which establishes the invariance of the square of s^2.
  • #1
Nitric
21
0
1. Start with the expression x'^2 + y'^2 _ z'^2 -c^2t'^2 and show, with the aid of the Lorentz transofmration, that this quantity is equal to x^2 + y^2 + z^2 -c^2t^2. This result establishes the invariance of s^2 defined by s^2 = x^2 + y^2 + z^2 -c^2t^2



2. s^2 = x^2 + y^2 + z^2 -c^2t^2



3. So far I have y = y' and z = z' because of the transformation law. basically there is no lorentz contraction perpendicular to the motion of X so y = y' and z = z'

how do i really solve this problem? where should I start?
 
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  • #2
So what does the Lorentz transformation look like for x' and t', in terms of x and t?
I mean, what is the correct full expression for

t' = ... t + ... x
x' = ... x + ... t
y' = y
z' = z
 
  • #3
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  • #4
Very nice. It's straightforward algebra then: plug them into
[itex]x^2 - c^2 t^2[/itex]
and show that you can simplify it to
[itex](x')^2 - c^2 (t')^2[/itex].
 
  • #5
CompuChip said:
Very nice. It's straightforward algebra then: plug them into
[itex]x^2 - c^2 t^2[/itex]
and show that you can simplify it to
[itex](x')^2 - c^2 (t')^2[/itex].
so I would have
(x'+vt'/sqrt(1-v^2/c^2)^2 - c^2(t' + vx'/c^2 / sqrt(1-v^2/c^2) and simplify it algebraically to x'^2 - c^2t'^2 ?
 
  • #6
Yes, the expression is a bit unclear, but it looks like what I got,
[tex]\frac{(x' + v t')^2 - (t' + v x' / c^2)^2}{(\sqrt{1 - v^2/c^2)^2}[/tex]
Just work out the multiplication (don't forget the cross-term). Then you'll see some cancellation taking place and you can factor the rest into something[itex]\,{}\times (x'^2 - c^2t'^2)[/itex].
 
  • #7
thanks a lot, i will get on this now :D
 
  • #8
I'm sort of stuck, my algebra isn't as fresh as I thought it would be. But am I on the right track though?

http://img264.imageshack.us/img264/1081/1233176495203dl2.jpg

^ My work
 
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  • #9
You are on the right track, I see two terms cancelling.
Watch the squares however, I see c^2 t'^2 instead of (c^2 t')^2 and v x'^2 instead of (v x')^2...

Also it may help to write everything in one fraction.
 
  • #10
I need a common denominator to start canceling things out right, or can I do it before? This is the part where my algebra isn't as fresh as it should be. To get the common denominator, I have to multiply the left equation by c^4 (top and bottom) and multiple the right equation by 1 (top and bottom) correct?
 
  • #11
Okay I did what I said on the previous post and so far I have:

c^4[x'^2 + (vt')^2] - (c^2t')^2 - (vx'^2) / c^4(1-v^2/c^2)

What can I do now to move forward? I don't see anything else cancel out.
 
  • #12
Okay my way isn't right, still stuck on this :|
 
  • #13
It seems you're having a little problem with the algebra. Let me get you started.

Since y' = y and z' = z, it suffices to show that x'^2 - c^2 t'^2 = x^2 - c^2 t^2.
Plugging it in:

[tex]x^2 - c^2 t^2 = \left( \frac{ x' + v t' }{ \sqrt{1 - v^2 / c^2} } \right)^2 - c^2 \left( \frac{ t' + v x' / c^2 }{ \sqrt{1 - v^2 / c^2} } \right)^2.[/tex]
Let me take the c^2 in the second term inside the brackets (c^2 a^2 = (c a)^2) and take the square root outside ( (a/b)^2 = a^2 / b^2, sqrt(a)^2 = a):
[tex]x^2 - c^2 t^2 = \frac{ \left( x' + v t' \right)^2 - \left( c t' + v x' / c \right)^2 }{ 1 - v^2 / c^2 }.[/tex]
Open up the brackets:
[tex]x^2 - c^2 t^2 = \frac{ x'^2 + 2 x' v t' + v^2 t'^2 - c^2 t'^2 - 2 t' v x' - v^2 x'^2 / c^2 }{ 1 - v^2 / c^2 }.[/tex]

Two terms cancel, after tracing the above steps carefully (make sure you understand which manipulations I did and that I didn't make any sign errors :-p) collect the terms in (x')^2 and (t')^2, i.e. write
[tex]x^2 - c^2 t^2 = \frac{ A x'^2 + B t'^2 }{ 1 - v^2 / c^2 }.[/tex]
 

FAQ: Now it remains to be shown that A = B. I'll leave that to you.

What is a Lorentz Transformation?

A Lorentz Transformation is a mathematical equation used in physics to describe how the measurements of space and time change for an observer moving at a constant velocity relative to another observer.

Who developed the concept of Lorentz Transformation?

The concept of Lorentz Transformation was developed by Dutch physicist Hendrik Lorentz in the late 19th and early 20th century as part of his work on the theory of electromagnetism.

What is the significance of Lorentz Transformation in physics?

Lorentz Transformation is significant in physics because it forms the basis of Einstein's theory of special relativity, which revolutionized our understanding of space and time. It also has practical applications in fields such as particle physics and astrophysics.

How does Lorentz Transformation differ from Galilean Transformation?

Lorentz Transformation differs from Galilean Transformation in that it takes into account the constant speed of light and the relativity of time, whereas Galilean Transformation assumes a constant time and space for all observers. Lorentz Transformation is more accurate and has been experimentally verified, while Galilean Transformation is a simpler approximation that works well for slower speeds.

Can Lorentz Transformation be applied to moving objects in everyday life?

Yes, Lorentz Transformation can be applied to moving objects in everyday life, but its effects are only noticeable at extremely high speeds close to the speed of light. For most daily activities, the differences between Lorentz Transformation and classical Galilean Transformation are negligible.

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