Undergrad Angles between 4-vectors in special relativity?

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The angle between two 4-vectors in special relativity is defined using the dot product, leading to the conclusion that Minkowski spacetime is non-Euclidean. For two unit timelike vectors, the inner product relates to rapidity, which is additive and corresponds to speed, while for unit spacelike vectors, the inner product aligns with the Euclidean definition. The discussion emphasizes that when vectors are of different types, the inner product remains useful but lacks a clear interpretation in terms of angles. Additionally, rapidity and celerity are differentiated, with rapidity being more relevant in special relativity, though its utility diminishes in general relativity. Overall, the complexities of defining angles in relativity highlight the unique nature of spacetime geometry.
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TL;DR
How do we define angles in relativity? do we change the usual euclidean definition or extend it?
How is the angle between two 4-vectors defined in special relativity? Consider two 4-velocity vectors:

$$U^\mu=(1,0), \\ V^\mu=\gamma_{rel}(1,v_{rel})$$

Where the vectors are written in the frame of the particle with ##U^\mu##.

The dot product between these is
$$U^\mu V_\mu=\gamma_{rel}$$

If we define angle ##\theta## between two vectors as:

$$\cos\theta=\frac{U^\mu V_\mu}{\vert U\vert\vert V\vert}$$

then since all velocity vectors have magnitude of ##1##, we get ##\cos\theta= \gamma_{rel}\geq 1##.

But what does this mean?
 
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LightPhoton said:
TL;DR Summary: How do we define angles in relativity? do we change the usual euclidean definition or extend it?

How is the angle between two 4-vectors defined in special relativity? Consider two 4-velocity vectors:

$$U^\mu=(1,0), \\ V^\mu=\gamma_{rel}(1,v_{rel})$$

Where the vectors are written in the frame of the particle with ##U^\mu##.

The dot product between these is
$$U^\mu V_\mu=\gamma_{rel}$$

If we define angle ##\theta## between two vectors as:

$$\cos\theta=\frac{U^\mu V_\mu}{\vert U\vert\vert V\vert}$$

then since all velocity vectors have magnitude of ##1##, we get ##\cos\theta= \gamma_{rel}\geq 1##.

But what does this mean?
It means Minkowski spacetime is manifestly non-Euclidean.
 
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If both ##U## and ##V## are unit and timelike then their inner product is ##\cosh\psi##, where ##\psi## is the rapidity. Rapidity has a one-to-one relationship with speed, and is additive (at least in one dimension). But it's not much used except to reframe the Lorentz transforms as manifestly the Minkowski analogue to Euclidean rotations.

If both ##U## and ##V## are unit and spacelike then their inner product is the Euclidean inner product.

If the vectors are different types the inner product remains useful, but I'm not sure it has a meaningful interpretation in terms of angle-type quantities.
 
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Hornbein said:
I always liked rapidity a.k.a. celerity.
Rapidity and celerity are different things. Rapidity is ##\psi## and ##v=c\tanh\psi##, but celerity is ##dx/d\tau=\gamma v##

I think rapidity is one of those things that isn't particularly useful once you go on to GR, so it's an interesting but fairly niche concept. Celerity is best forgotten about, IMO.
 
velocity = c tanh (rapidity)
celerity = c sinh (rapidity)
time-dilation-factor = cosh (rapidity)
Doppler-factor = exp (rapidity)
 
MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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