I've been working though a set of ideas centered around explaining special relativity as rotations in four dimensional space. +Jonah Miller 's excellent post on Minkowski space this week spurred me into finally capturing some of my nascent ideas here. I should caution that what follows are the starting points for directions I intend to explore and are hypothetical thought processes, not (until they're mathematically verified or refuted), necessarily the way things actually work. First though, we'll start out with a little bit of well established background on how special relativity does work.

**Time Dilation and Four Velocity**

Two different sources led to my ideas. First, there's the concept of a four velocity[2]. The first place I saw this concept described was in a Brian Greene book[3]. The basic idea is that everything in the universe moves at a constant speed, the speed of light, in a four dimensional space, (hence the term four velocity), that consists of the three space directions, and the fourth 'direction', time. We can't change our total speed, all we can do is change our direction. So, we can move more quickly in a space direction, but that means we slow down in the time direction. Normally, most of our velocity points in the time direction, so we don't feel like we're moving at the speed of light.

If we steer a significant portion of our velocity into the space direction, we start to see one of the effects of special relativity, time dilation. For us, time slows down. If we speed away at a significant portion of the speed of light, turn around and speed back to our original location, we'll find that more time has passed four our friends that stayed behind than the has passed for us. Why? It's because we slowed our velocity in the time direction when we sped up in the space direction.

This phenomenon is called time dilation. It's often taught in physics courses using something called the twin paradox. More about the paradox and it's resolution in a future post. For now, I'll just leave you with a simplistic diagram of what the twin did when he sped away and returned (picture 1).

**Even Einstein Got it Wrong**

**Hypothesis**

Consider the following three dimensional analog. If a straight line rotated away from you, you'd perceive it as being shorter. If a sphere rotated away from you, you'd still see a perfect sphere.

Given the background sections above, first, that we can think of moving relativistically as 'steering' our speed into and out of the time dimension, and second, the fact that a sphere still looks like a sphere at relativistic speeds, is it possible to describe all of special relativity merely as rotations in a four dimensional space? Physicists already talk about special relativity in terms of Lorentz transforms which are mathematically called rotations. However, as demonstrated by the sphere example above, we stop short of considering these rotations to be common every day rotations as opposed to formal mathematical constructs. If it is possible, what do the mathematical constructs that describe these rotations look like? What simplifications and conceptual enlightenment can be gained from looking at the theory from this perspective?

**References:**

1. http://www.thephysicsmill.com/2013/02/10/a-space-time-cocktail-minkowski-space-and-special-relativity/

2. http://en.wikipedia.org/wiki/Four_velocity

3. Check out pp. 47-48

http://books.google.com/books?id=DNd2K6mxLpIC&printsec=frontcover&dq=brian+greene&hl=en&sa=X&ei=1_4eUdnuLtLy2gWa7YGgBQ&ved=0CDAQ6AEwAA#v=snippet&q=special%20relativity&f=false

4. Invisibility of the Lorentz Contraction

http://prola.aps.org/abstract/PR/v116/i4/p1041_1

Phys. Rev. 116, 1041 (1959) - Invisibility of the Lorentz Contraction http://journals.aps.org/pr/abstract/10.1103/PhysRev.116.1041

5. The apparent shape of a relativistically moving sphere

http://journals.cambridge.org/action/displayAbstract?fromPage=online&aid=2049244

## 2 comments:

Great post! The fact that a sphere always looks the same after Lorentz transform always puzzled me. Thanks for explaining it so nicely!

I didn't explain this in my post on the topic, because I felt it was too technical for my blog, but there's a transformation called a Wick rotation we use to go between Lorentzian and Euclidian spacetimes.

http://en.wikipedia.org/wiki/Wick_rotation

The idea is that you rotate through the complex plane to change the lorentzian signature to a Euclidean one. You've probably seen a matrix for Lorentz transforms that takes the form

[ cosh(phi) -sinh(phi) ]

[ -sinch(phi) cosh(phi) ],

where phi is called the boost parameter, and

phi = cosh^{-1}(gamma).

The secret is that the hyperbolic trig functions are just trig functions of an imaginary angle.

cosh(x) = cos(ix)

sinh(x) = -isin(ix)

So you're absolutely right that Lorentz transforms are a rotation. The secret is that if the norm square of timelike vectors is negative, those vectors are complex. Furthermore, the angle of "rotation" for a Lorentz boost is imaginary.

Thanks Jonah!

I've seen the Wick rotation a lot over on the Casimir side of my work. Both Sommerfeld, in the second volume of his physics course, and Moller have excellent examples where they treat the complex rotation angle as real. In Sommerfeld's case, he shows very nicely how the E and B fields rotate into each other as the velocity of a travelling charge is changed.

Post a Comment