Integral over a region in spacetime

  • Context: Undergrad 
  • Thread starter Thread starter Sandra Conor
  • Start date Start date
  • Tags Tags
    Integral Spacetime
Click For Summary
SUMMARY

The integral under discussion is evaluated over a spacelike 2 surface in spacetime, specifically represented as $$\frac{1}{a_0^2}\int_\Sigma\frac{dy'dz'}{\bigg(y'^2+z'^2+\tfrac{1}{(2a_0)^2}\bigg)^2}$$. The transformation to polar coordinates simplifies the integral to $$\frac{1}{a_0^2}\int_\Sigma\frac{rd\phi dr}{\bigg(r^2+\tfrac{1}{(2a_0)^2}\bigg)^2}$$. The discussion highlights the importance of defining the domain of integration, denoted as $$\Sigma$$, to proceed with the evaluation. Stokes' theorem is also mentioned as a relevant concept in this context.

PREREQUISITES
  • Understanding of spacetime geometry and surfaces
  • Familiarity with polar coordinate transformations
  • Knowledge of Stokes' theorem
  • Basic principles of complex function theory
NEXT STEPS
  • Research the application of Stokes' theorem in evaluating integrals over surfaces
  • Study the properties of spacelike surfaces in general relativity
  • Explore polar coordinate integration techniques in higher dimensions
  • Investigate complex function theory and its applications in integral calculus
USEFUL FOR

Mathematicians, physicists, and students engaged in advanced calculus, particularly those focusing on integrals in spacetime and complex analysis.

Sandra Conor
Messages
9
Reaction score
0
Hello, can anyone show me if this integral can be evaluated?

##\frac{1}{a_0^2}\int_\Sigma\frac{dy'dz'}{\bigg(y'^2+z'^2+\tfrac{1}{(2a_0)^2}\bigg)^2}##
 
Physics news on Phys.org
I am thinking polar coordinates - but what does the summation sign stand for?
 
I have been thinking of polar form too. The summation sign represent a spacelike 2 surface in spacetime.

Initially, I want to evaluate this integral in spacetime.
$$\int_{\Sigma} \frac{dydz}{[a_{o}(y^{2}+z^{2})+2f_{o}y+2g_{o}z+c_{o}]^{2}}$$ where $$a_{o}c_{o}-f_{o}^{2}-g_{0}^{2}=\frac{1}{4}.$$

My way is to define
$$y':=y+\frac{f_0}{a_0},\,z':=z+\frac{g_0}{a_0}$$
Then the quadratic becomes $$a_0(y'^2+z'^2)+c_0-\frac{f_0^2+g_0^2}{a_0}=a_0\bigg(y'^2+z'^2+\tfrac{1}{(2a_0)^2}\bigg).$$

So now, I will need to evaluate$$\frac{1}{a_0^2}\int_\Sigma\frac{dy'dz'}{\bigg(y'^2+z'^2+\tfrac{1}{(2a_0)^2}\bigg)^2}\cdot$$ But this seems complicated. So I am thinking of using polar coordinate and if I do so, it becomes:
$$\frac{1}{a_0^2}\int_\Sigma\frac{dy'dz'}{\bigg(y'^2+z'^2+\tfrac{1}{(2a_0)^2}\bigg)^2} = \frac{1}{a_0^2}\int_\Sigma\frac{rd\phi dr}{\bigg(r^2+\tfrac{1}{(2a_0)^2}\bigg)^2}$$

Since this is in reference to spacetime, I am stuck as to how I should continue. If it is about a disk with radius R then I know what to do but for a spacelike 2 surface, I am still wandering.
 
Hm. This is far outside my area (complex function algebras), but I can throw in some random thoughts and hope it will inspire you.
  • I don't know why, but Stokes' theorem keeps swirling around in my head (https://en.wikipedia.org/wiki/Stokes'_theorem)
  • I have a tendency to think complex variables - have you considered that
  • If I haven't done a blunder, I think \frac{d}{dr}\frac{1}{r^{2}+C}=\frac{-2r}{(r^{2}+C)^{2}}
 
It looks like your main problem is defining the domain of integration in purely geometric terms. You need to explicitly define ##\Sigma##.
 
Thanks Svein for the ideas. I will check these out.

Yes, mathman. The summation sign represent a spacelike 2 surface in spacetime. Its mentioned in the third post. Sorry about that.
 

Similar threads

  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 30 ·
2
Replies
30
Views
1K
  • · Replies 14 ·
Replies
14
Views
4K
  • · Replies 7 ·
Replies
7
Views
392
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 14 ·
Replies
14
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K