Lorentz Boost Help: Why Use Hyperbolic Functions?

In summary, the content discusses the use of Lorentz boosts in 4 dimensions, specifically in the context of rotations in the (ct) plane. These transformations use hyperbolic functions instead of trigonometric ones due to the non-Euclidean nature of spacetime. The use of hyperbolic functions allows for the preservation of intervals of constant length and avoids violations of causality. Further explanations and applications of this concept can be found in the provided link.
  • #1
fys iks!
40
0
I was reading a section on lorentz boosts and i need some help understanding what they did:

the book starts off by defining the line element dS where:

(dS)^2 = -(CΔt)^2 + dx^2 + dy^2 + dz^2

then they say: "consider the analogs of rotations in the (ct) plane. These transformations leave y and z unchanged but mix ct and x. The transformations with this character that leave the analogies of rotations of (3.9) but with trig functions replaced by hyperbolic functions because of the non euclidean nature of space time. Specifically

ct= [cosh(theta)]*[ct] - [sinh(theta)]*x
x = [sinh(theta)]*[ct] + {cosh(theta)]*x
y= y
z = z

and 3.9 was

x = cos(gamma)*x - sin(gamma)*y
y = sin(gamma)*x + cos(gamma) * y


So what i don't understand is why did they decide to use the hyperbolic functions in 4 dimensions?
 
Physics news on Phys.org
  • #2
fys iks! said:
So what i don't understand is why did they decide to use the hyperbolic functions in 4 dimensions?

If you use a transformation with an ordinary sin and cos in it, you get a rotation. If you keep on rotating the x-t plane, at some point you'll have rotated it so it's 180 degrees upside-down. At that point you've reversed the direction of time. This violates causality.
 
  • #3
Thanks! That helped out a lot.

So by using hyperbolic sin/cos they were able to create the same shift without violating causality.

Do you have any links that further explain this in more detail?
 
  • #4
So what i don't understand is why did they decide to use the hyperbolic functions in 4 dimensions?
You have not been paying attention, have you. An ordinary rotation in 3D space leaves the length of a vector unchanged, where the length element is [itex]ds^2=dx^2+dy^2+dz^2[/itex]. Rotating this by [itex]\theta[/itex] gives in the xy plane gives

[tex]
ds'^2= (cos(\theta)dx+sin(\theta)dy)^2+(sin(\theta)dx-cos(\theta)dy)^2+dz^2
[/tex]
and because [itex]cos(\theta)^2+sin(\theta)^2=1[/itex] it follows that [itex]ds'=ds[/itex].

In the ct-plane, we wish to preserve [itex]ds^2=dt^2-dx^2-dy^2-dz^2[/itex]. If you do the calculation as above with cosh and sinh instead, you find [itex]ds'=ds[/itex] because [itex]cosh(\theta)^2-sinh(\theta)^2=1[/itex]. The geometry of the cx plane is not Euclidean.

[posted simultaneously with bcrowell]
 
  • #5
fys iks! said:
Thanks! That helped out a lot.

So by using hyperbolic sin/cos they were able to create the same shift without violating causality.

Do you have any links that further explain this in more detail?

http://www.lightandmatter.com/area1book6.html
 
  • #6
In 4 dimensional spacetime intervals of constant length are hyperbolas. Also it is sometimes easier to work with hyperbolic functions

[tex]
tanh(\theta) = v/c
[/tex]

The addition of velocities is reduced to adding hyperbolic functions.
 

1. Why do we need to use hyperbolic functions in Lorentz boosts?

Hyperbolic functions are used in Lorentz boosts because they provide a mathematical framework to describe the effects of relativity on time and space. The equations used in hyperbolic functions are derived from the Lorentz transformation, which is a fundamental concept in special relativity.

2. How do hyperbolic functions differ from trigonometric functions?

Hyperbolic functions are similar to trigonometric functions in that they involve ratios of sides of a right triangle. However, the main difference is that hyperbolic functions use the hyperbola as the underlying geometric shape, while trigonometric functions use the circle.

3. Can you provide an example of a Lorentz boost using hyperbolic functions?

One example of a Lorentz boost using hyperbolic functions is the time dilation formula, which is given by t' = t/cosh(θ), where t' is the time observed in a moving frame of reference, t is the time observed in a stationary frame of reference, and θ is the relative velocity between the frames. This formula shows how time appears to slow down in a moving frame of reference.

4. How do hyperbolic functions help us understand the effects of relativity?

Hyperbolic functions help us understand the effects of relativity by providing a mathematical framework for describing the relationships between time, space, and velocity in moving frames of reference. They allow us to calculate how time, length, and mass change in different reference frames, and how these changes are related to the speed of light.

5. Are there any real-world applications of Lorentz boosts and hyperbolic functions?

Yes, there are many real-world applications of Lorentz boosts and hyperbolic functions, particularly in the fields of physics and engineering. For example, they are used in the design of particle accelerators and in the calculations involved in GPS systems. They are also essential in understanding the behavior of high-speed objects, such as spacecraft and high-speed trains.

Similar threads

  • Special and General Relativity
Replies
2
Views
1K
  • Special and General Relativity
Replies
13
Views
885
  • Special and General Relativity
Replies
33
Views
2K
  • Special and General Relativity
Replies
19
Views
3K
Replies
13
Views
1K
  • Special and General Relativity
2
Replies
61
Views
4K
  • Special and General Relativity
Replies
4
Views
1K
  • Special and General Relativity
Replies
3
Views
984
  • Advanced Physics Homework Help
Replies
8
Views
740
  • Special and General Relativity
Replies
2
Views
1K
Back
Top