Total volumetric charge distribution of the universe

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Homework Help Overview

The discussion revolves around calculating the total volumetric charge of the universe based on a given charge density function, ρv=(e-2r/r2). Participants are exploring the implications of this problem within the context of electromagnetic theory.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to set up the integral for total charge using spherical coordinates, expressing concerns about the appropriate limits for integration in the context of a spherical universe. Other participants confirm the setup but question how to define the limits of integration, particularly for the angles θ and φ.

Discussion Status

Participants are actively engaging with the problem, with some suggesting that the setup is correct while others are seeking clarification on the limits of integration. There is a recognition of the complexity involved in defining the bounds for a universe modeled as spherical.

Contextual Notes

There is mention of the book suggesting a specific result (6.28[C]), but the participants are unsure how to derive this based on the limits of integration for a spherical coordinate system.

Zee Prime
Greetings! I'm new here and I think about this place as soon as I see what the statement asks.

Homework Statement


Considering the volumetric density ρv=(e-2r/r2), figure the total charge (ℚ) of the universe.

Homework Equations


[/B]
ρv=ΔQ/ΔV -> (ΔQ ∝ ΔV)
ℚ=∫v ρv dxdydz

The Attempt at a Solution


I know you can figure it out ℚ when you've a pack of coordinates (bounds of the volume) in which you can calculate the total charge if you find some kind of symetry or not (i.e: cilindric, spherical coordinates and so on); but my mind just stacked overflow when the book asks the total charge of the universe... I wonder what system of coordinates and values should I use for the triple integral?

I've read that the shape of the universe —or known one— is flat; but I'm pretty sure I haven't the proper knowledge and mathematical understanding to realize that; so I assume for early problems, the shape is spherical, so I would use the following:

ℚ=∫vρv dv = ∫∫∫ρvr2Sin(Φ) drdΦdΘ

Jacobian Determinant.

I've found this problem at the second chapter of the book Electromagnetic Theory - Hayt. I'd appreciate some help with this problem. Thank you for your attention and keep this pantheon of physics alive! Congrats on this forum. :woot:
 
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I think you've set it up properly. Go ahead and put limits on the integrals and evaluate them.
 
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Likes   Reactions: Zee Prime
phyzguy said:
I think you've set it up properly. Go ahead and put limits on the integrals and evaluate them.

But buddy, how would you put the limits of a spherical-universe (some rate of change?) The book suggest 6.28[C] as a result.

Ty for reply! :oldbiggrin:
 
Zee Prime said:
But buddy, how would you put the limits of a spherical-universe (some rate of change?) The book suggest 6.28[C] as a result.
Ty for reply! :oldbiggrin:

Well, r will go from 0 to ∞. What about θ and φ?
 

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