Finding Current Flux Through Closed Surface

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Homework Help Overview

The problem involves calculating the total current flux through a closed surface surrounding a cubic volume, given a specific current density vector in Cartesian coordinates. The context is rooted in electromagnetism, particularly focusing on current density and flux.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the use of symmetry in evaluating the flux through the surface integrals, with one suggesting to start with a single surface integral instead. There is also mention of relating the problem to electric flux concepts, although uncertainty about the correct approach persists.

Discussion Status

The discussion is ongoing, with participants exploring different methods to approach the problem. Some guidance has been offered regarding the use of symmetry and focusing on specific surface integrals, but no consensus has been reached on a definitive method or solution.

Contextual Notes

Participants note that the direction of the current density vector is constant and that the magnitude varies, which may influence the setup of the integrals. There is also mention of certain surfaces where the current density is zero, which could affect the overall calculation.

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Homework Statement



Let J=xy^2(\hat{x}+\hat{y}+\hat{z}) A/m^2 denote the electrical current density filed -i.e, current flux per unit area - in a region of space represented in Cartesian coordinates. A current density of J=xy^2(\hat{x}+\hat{y}+\hat{z}) A/m^2 implies the flow of electrical current in the direction J/abs(J)= (\hat{x}+\hat{y}+\hat{z})/\sqrt{3} with a magnitude of abs(J) = xy^2\sqrt{3} Amperes (A) per unit area.

Calculate the total current flux J*Ds through a closed surface S enclosing a cubic volume V = 1m^3 with vertices at (x,y,z,) = (0,0,0) and (1,1,1) m.


Homework Equations





The Attempt at a Solution



I believe that I can use a fair amount of symmetry for this problem because this flux should be the sum of six surface integrals. I have done a fair amount of things with electric flux in the past..and I feel that this should be very similar however my mind seems to believe drawing a blank is the best solution. I tried to start with the integral of abs(J)*(\hat{z})dxdy=total current enclosed/eo. Is that kind of the right idea? Or should I be trying to set it up differently.
 
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Postpone the symmetry idea and start with one of the six surface integrals. Direction of J is a constant (unit vector) and so is ##d\vec S##. Only thing that varies is the magnitude. Write out the integral.
 
∫xy^2(\hat{z})dxdy

I kind of had this before. I then was thinking along the lines well okay for when I did electric flux if I had a electric field E and I needed to find the charge enclosed and I was given a charge density I would start:

E*2*π*r^2=ρ*π*r^2/εo
then things would cancel and I would get E=ρ/(2*εo)

However, I am unsure how to progress to that point for the current flux. I'm sure its some simple thing I'm not putting together
 
OK, you picked the one where symmetry does come in useful: z=0. Check with the opposite one (z=1) and bingo, two down, four to go.

Note that two of those four have magnitude of J = 0 ( the ones with x or y equal to zero ).

Leaves some work to do, still, but you'll manage !
 

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