Guass's Law over the x axis

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In summary, the homework statement is that a charge is uniformly distributed along the x-axis with density ß. Gauss' Law tells us that the electric field produced by the charge is proportional to this density, and so work is done on a charge moving from y = a to y = b if this field is applied.
  • #1
Colts
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Homework Statement


Charge is uniformly distributed along the x-axis with density ß. Use Gauss' Law to find the electric field it produces, and use this to calculate the work done on a charge Q that moves along the y-axis from y = a to y = b.


Homework Equations



[itex]\phi[/itex]=[itex]\int[/itex][itex]\vec{E}[/itex]*[itex]\hat{n}[/itex]dA

[itex]\phi[/itex]= [itex]\frac{Q}{\epsilon}[/itex]

The Attempt at a Solution



I used a cylinder for my surface since the normal vector will always align with the electrical field. So the first part, the equation ends up
[itex]\phi[/itex]=E[itex]\int[/itex]dA
[itex]\phi[/itex]=E(2∏rh)

(r is the radius from the axis to the edge of the cylinder and h is the length of the cylinder.)

and if I remember right, Q is the density times the are of enclosure.
so Q = β(2∏rh)
I set the two [itex]\phi[/itex] equations equal to each other and get
[itex]\frac{β}{ε}[/itex]=E

I don't think that's right though. What did I do wrong?
 
Last edited:
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  • #2
Since the charge is along the x-axis, then β is a linear charge density.
So, to get the charge enclosed, you multiply β by the length h, and not the volume.
 
  • #3
Hi Colts! :smile:
Colts said:
Charge is uniformly distributed along the x-axis with density ß.

and if I remember right, Q is the density times the are of enclosure.
so Q = β(2∏rh)

No, "density" here means the line density (in coulombs per metre, not per metre3)

So Q = βh. :wink:

(of course, sometimes "density" means surface density, and occasionally it actually means density! :rolleyes:)

EDIT: ap123 beat me to it! :biggrin:
 
  • #4
So the electrical field is

E = [itex]\frac{β}{2πrε}[/itex]
 
Last edited:
  • #5
Is the last question asking me to integrate E from a to b?
 
  • #6
Colts said:
Is the last question asking me to integrate E from a to b?
Integrate the force, FExt, that would need to be exerted on a charge, Q, to move the charge from a to b . (Actually integrate the work the force does.)
 
  • #7
[itex]\int[/itex][itex]\frac{βxdx}{2πrε}[/itex]

x is the distance

does that look right? and the integral would be from a to b
 
  • #8
Colts said:
[itex]\int[/itex][itex]\frac{βxdx}{2πrε}[/itex]

x is the distance

does that look right? and the integral would be from a to b
Not correct.

What is the force on a charge Q located on the y-axis , a distance y from the x-axis ?

You (or some outside agent) must apply what force on Q to move it, at a constant rate, when the charge is located on the y-axis ?

Added in Edit:

Another way to do this is to find the potential difference from y = a to y = b .

To do that, you do integrate -E .
 
Last edited:

Related to Guass's Law over the x axis

1. What is Guass's Law over the x axis?

Guass's Law over the x axis is a mathematical concept in electromagnetism that explains the relationship between the electric field and the electric charge distribution.

2. How is Guass's Law over the x axis different from the traditional Guass's Law?

The traditional Guass's Law applies to any closed surface, while Guass's Law over the x axis specifically applies to a surface that is parallel to the x axis.

3. What is the significance of using Guass's Law over the x axis?

Guass's Law over the x axis allows us to simplify calculations and analyze the electric field in a specific direction, which is useful in many engineering and scientific applications.

4. Can Guass's Law over the x axis be applied to any shape or surface?

Yes, Guass's Law over the x axis can be applied to any surface that is parallel to the x axis, regardless of its shape or size.

5. How is Guass's Law over the x axis used in practical applications?

Guass's Law over the x axis is used in various applications, such as designing electronic circuits, calculating the electric field around wires and conductors, and analyzing the behavior of electromagnetic waves.

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