Lorentz transformations on spacetime

In summary, The Lorentz transformations on a spacetime 4-vector can be written as x'μ = (Lμν)*(χν). The matrix L can be obtained by using the standard Lorentz transformation equations with x' y' z' t' on the left and x y z t on the right, in their matrix form.
  • #1
helpcometk
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0

Homework Statement


A3. Show that the Lorentz transformations on a spacetime 4-vector can be written as
x'μ = (Lμν)*(χν)
. Find the matrix L. Prove that (in matrix notation) Lτ gL = g where g is
the Minkowski spacetime metric.

Homework Equations


Any help suggesting at least equations will be appreciated. μ , τ and ν are exponents.

The Attempt at a Solution

 
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  • #2
welcome to pf!

hi helpcometk! welcome to pf! :smile:

(try using the X2 and X2 icons just above the Reply box :wink:)
helpcometk said:
Show that the Lorentz transformations on a spacetime 4-vector can be written as
x'μ = (Lμν)*(χν)

you should be able to write out L just by looking at the standard Lorentz transformation equations

(and btw, they're not exponents, they're superscripts, or just indices :wink:)
 
  • #3


Thanks for the reply Tim.
Specifically which expressions i have to take into account?
 
  • #4
The standard Lorentz equations :rolleyes:

the ones with x' y' z' t' on the left and x y z t on the right!
 
  • #5


The Lorentz transformations are mathematical equations that describe how the coordinates of an event in one inertial reference frame are related to the coordinates of the same event in another inertial reference frame. These transformations are based on the principles of special relativity and are used to account for the effects of time dilation and length contraction.

The equation x'μ = (Lμν)*(χν) represents the transformation of a spacetime 4-vector, where x'μ is the transformed vector, Lμν is the transformation matrix, and χν is the original vector. To find the matrix L, we can use the Lorentz transformation equations:

x'0 = γ(x0 - vt)
x'1 = x1
x'2 = x2
x'3 = x3

where γ is the Lorentz factor and v is the relative velocity between the two reference frames. These equations can be written in matrix form as:

x' = Lx

where x = [x0, x1, x2, x3] and x' = [x'0, x'1, x'2, x'3]. This gives us the following transformation matrix:

L = [γ -γv 0 0;
-γv γ 0 0;
0 0 1 0;
0 0 0 1]

To prove that Lτ gL = g, we can multiply the matrices:

Lτ gL = [γ -γv 0 0;
-γv γ 0 0;
0 0 1 0;
0 0 0 1]
[1 0 0 0;
0 -1 0 0;
0 0 -1 0;
0 0 0 -1]
[γ -γv 0 0;
-γv γ 0 0;
0 0 1 0;
0 0 0 1]

= [γ -γv 0 0;
γv -γ 0 0;
 

What are Lorentz transformations on spacetime?

Lorentz transformations on spacetime are mathematical equations used in Einstein's theory of special relativity to describe how time and space coordinates are related between two reference frames that are moving at constant velocities relative to each other.

What is the significance of Lorentz transformations?

Lorentz transformations are significant because they demonstrate that time and space are not absolute, but are relative to the observer's frame of reference. This is a fundamental principle of special relativity and has far-reaching implications in our understanding of the universe.

How do Lorentz transformations affect the concept of simultaneity?

Lorentz transformations show that simultaneity, or the idea that two events occur at the same time, is relative. This means that events that are simultaneous in one reference frame may not be simultaneous in another reference frame that is moving at a different velocity.

Do Lorentz transformations only apply to objects moving at high speeds?

No, Lorentz transformations apply to all objects in motion, regardless of their speed. However, their effects become more pronounced at high speeds, approaching the speed of light.

What is the difference between a Lorentz transformation and a Galilean transformation?

A Galilean transformation is a simpler mathematical equation used to convert between coordinates in two reference frames that are moving at constant velocities relative to each other. However, it fails to account for the effects of relativity, making it limited to low speeds. A Lorentz transformation is a more complex equation that accounts for the effects of special relativity, making it applicable to all speeds.

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