Four Momentum in General Relativity

Click For Summary
SUMMARY

The discussion clarifies the concept of four momentum in General Relativity (GR) compared to Special Relativity (SR). In SR, the relationship is defined as p^α = mU^α, but this does not hold in curved space, where four momentum is treated as a covector. The time component, p_0 = -E, is valid only in metrics where the 00 component equals -1, which is not always the case in GR. The relationship between vector and covector momentum is expressed as p_μ = g_μν p^ν, emphasizing their fundamental differences despite common conventions.

PREREQUISITES
  • Understanding of Special Relativity (SR) principles
  • Familiarity with General Relativity (GR) concepts
  • Knowledge of covectors and contravariant vectors
  • Basic comprehension of metric tensors in curved spacetime
NEXT STEPS
  • Study the relationship between four momentum and metric tensors in General Relativity
  • Explore the implications of curved spacetime on physical quantities
  • Learn about the Schwarzschild metric and its applications in GR
  • Investigate the conventions of raising and lowering indices in tensor calculus
USEFUL FOR

Students and researchers in theoretical physics, particularly those focusing on General Relativity, as well as anyone seeking to deepen their understanding of the mathematical framework underlying four momentum in curved spacetime.

MrBillyShears
Gold Member
Messages
14
Reaction score
0
Alright, I'm rather new to General Relativity, and I'm getting confused with four momentum. Back in SR, p^α=mU^α, but, this relationship doesn't hold in curved space, does it? Because, now I'm seeing that four momentum is somehow a covector in GR, and p_0=-E, so the time component of the contravariant component can't be E, since the 00 component of the metric isn't always -1. So, is four momentum now redefined in GR, and if the SR relationship between four velocity isn't valid, what is the new relationship to U? Is four momentum naturally a covariant thing?
 
Physics news on Phys.org
MrBillyShears said:
Back in SR, p^α=mU^α, but, this relationship doesn't hold in curved space, does it? Because, now I'm seeing that four momentum is somehow a covector in GR,
I am not sure if this is your concern, but you would probably call both ##p^α=mU^α## and ##p_α=mg_{\mu α}U^{\mu}## "the four momentum". If you need to distinguish between the two verbally you would call one "the four momentum vector" and the other "the four momentum covector".

MrBillyShears said:
and p_0=-E, so the time component of the contravariant component can't be E, since the 00 component of the metric isn't always -1.
##p_0=-E## would only hold in metrics where the 00 component is -1. In GR that won't always be the case. The 00 component may not be the time-time component. In fact, there may not even be a time-time component. Regardless, the definition above will hold, even if the components don't have such a clear interpretation.
 
That's ironic. I'm confused now too. In the introductory book I'm reading on GR, the author defines p_0=-E when discussing trajectories in the Schwarzschild metric, and then he goes to define p^0=g^{00}p_0=(1-{2M}/r)^{-1}E. Why does he do this then? Is this a matter of convention, defining the vector momentum from the covector momentum?
 
Sorry, I was indeed being a little ambiguous (actually a little wrong). What I was thinking and what I should have said is that ##p_0=\pm p^0=\pm E## only in metrics where the 00 component is ##\pm 1##, and even then only if the 0i components are 0 too.

The vector and covector momentum are always related as ##p_{\mu}=g_{\mu\nu}p^{\nu}##, regardless of the metric. The vector and the covector are in some ways fundamentally different quantities, but nevertheless it is a very strong convention to think of them as the same quantity just with raised or lowered indexes.
 
Last edited:

Similar threads

  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 36 ·
2
Replies
36
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 0 ·
Replies
0
Views
1K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 50 ·
2
Replies
50
Views
4K
  • · Replies 67 ·
3
Replies
67
Views
6K
  • · Replies 9 ·
Replies
9
Views
1K
  • · Replies 13 ·
Replies
13
Views
8K