Finding Current Flux Through Closed Surface

In summary, we are given the current density J=xy^2(\hat{x}+\hat{y}+\hat{z}) A/m^2 representing the flow of electrical current in a region of space. To calculate the total current flux, we can use symmetry to simplify the problem by breaking it down into six surface integrals. We can start with one of the integrals and use the fact that the direction of J and ##d\vec S## are constant, while the magnitude varies. By setting up the integral and using the given information, we can solve for the magnitude of J and determine the total current flux through a closed surface enclosing a cubic volume.
  • #1
Gee Wiz
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Homework Statement



Let J=xy^2([itex]\hat{x}[/itex]+[itex]\hat{y}[/itex]+[itex]\hat{z}[/itex]) 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([itex]\hat{x}[/itex]+[itex]\hat{y}[/itex]+[itex]\hat{z}[/itex]) A/m^2 implies the flow of electrical current in the direction J/abs(J)= ([itex]\hat{x}[/itex]+[itex]\hat{y}[/itex]+[itex]\hat{z}[/itex])/[itex]\sqrt{3}[/itex] with a magnitude of abs(J) = xy^2[itex]\sqrt{3}[/itex] 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)*([itex]\hat{z}[/itex])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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  • #2
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.
 
  • #3
∫xy^2([itex]\hat{z}[/itex])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
 
  • #4
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 !
 
  • #5


I would approach this problem by first identifying the relevant equations and variables involved. In this case, the relevant equation is the definition of current flux, which is given by J*Ds, where J is the current density and Ds is the surface area. The variables involved are the current density J and the surface area Ds.

Next, I would visualize the problem and identify any symmetries that could simplify the calculation. In this case, the cubic volume and the current density being constant throughout the volume suggest a high degree of symmetry. This means that we can use the symmetry to simplify the calculation.

To calculate the total current flux, we need to integrate the current density over the surface area. Since the current density is constant, we can pull it out of the integral. Then, we can use the symmetry to simplify the integral by breaking it up into six surface integrals, each corresponding to one face of the cube. The surface area for each face can be calculated using basic geometry.

Finally, we can use the given vertices of the cube to set up the limits of integration for each surface integral. Once we have all six surface integrals, we can add them together to get the total current flux through the closed surface.

In summary, to solve this problem, we need to use the definition of current flux, take advantage of the symmetry of the problem, and set up and evaluate six surface integrals to calculate the total current flux through the closed surface.
 

1. What is "Finding Current Flux Through Closed Surface"?

"Finding Current Flux Through Closed Surface" is a mathematical concept used in physics to calculate the flow of an electric field through a closed surface. It is commonly used in the study of electromagnetism and can help determine the amount of charge enclosed within a given surface.

2. How is current flux through a closed surface calculated?

The current flux through a closed surface is calculated by taking the integral of the dot product of the electric field and the surface's normal vector over the entire surface. This can be represented mathematically as Φ = ∫E · dA, where Φ is the current flux, E is the electric field, and dA is the differential area element.

3. What is the significance of finding current flux through a closed surface?

Finding current flux through a closed surface allows us to understand the behavior of electric fields and how charges interact with them. It can also help us determine the strength and direction of the electric field at any point on the surface and the amount of charge enclosed within the surface.

4. Can current flux through a closed surface be negative?

Yes, current flux through a closed surface can be negative. This indicates that the electric field is directed opposite to the normal vector of the surface, meaning that the flow of the electric field is in the opposite direction. This could occur if there is a negatively charged object within the surface, as the electric field would be directed towards the object.

5. How is current flux through a closed surface related to Gauss's Law?

Current flux through a closed surface is directly related to Gauss's Law, which states that the electric flux through a closed surface is equal to the charge enclosed by the surface divided by the permittivity of free space. This means that by calculating the current flux through a closed surface, we can determine the amount of charge enclosed within that surface, and vice versa.

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