Gauss's Law for Line of Charge

In summary, for a line of charge, the E field is assumed to be perpendicular to the sides of a cylindrical Gaussian surface. Therefore, there is no flux through the ends of the cylinder, as the field has no component normal to the surface. This is due to the infinite length of the line charge and the cancelling out of field lines at the ends. This holds true for any points in the field as long as the line charge is infinitely long. The term "radially outward" refers to the direction of the r coordinate, which is perpendicular to the line itself in cylindrical coordinates. In situations with cylindrical symmetry, it means "perpendicularly outwards from the axis of symmetry."
  • #1
mvpshaq32
28
0
Just refreshing on Gauss's Law.

For a line of charge, we choose a cylindrical Gaussian surface. But if the E field is radially outwards, why is there no flux through the ends of the cylinder and only through the sides?

I know that the field is only assumed to be perpendicular to the sides of the cylinder, but isn't there field through the ends as well?

Or is the flux through the ends zero because the line of charge is infinitely long and there are field lines in equal and opposite direction at the ends of the cylinder so they cancel out, hence there is no flux?
 
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  • #2
If the line is straight and infinite then, by symmetry, the E field must be purely radial. Therefore the flux on the ends is zero since the field has no component normal to the surface.
 
  • #3
DaleSpam said:
If the line is straight and infinite then, by symmetry, the E field must be purely radial. Therefore the flux on the ends is zero since the field has no component normal to the surface.

Yes, I understand that, but does radially outward not mean outward in all directions?

That includes going through the ends of the cylinder
 
  • #4
Just think about it from a symmetry point of view. Could there be a net field going one way or the other?
 
  • #5
mvpshaq32 said:
Yes, I understand that, but does radially outward not mean outward in all directions?

That includes going through the ends of the cylinder
An infinite line is axisymmetric, or in other words it can best be represented using cylindrical coordinates. Radially outward here means in the direction of the r coordinate, which is always perpendicular to the line itself.

Consider this. Either the field can be purely in the r direction, or it could tilt a little in the z direction. If it were to tilt in the z direction, how could it choose whether to tilt in the +z or the -z direction? Everything is symmetric, the charge goes out to infinity in both directions. Since there is no way for the field to choose +z or -z then it must be purely r.
 
  • #6
Yes and we can also consider the two infinitesimal point charges where a given point in the field lies on their perpendicular bisector. The field strengthes in the z direction clearly cancel each other out. And this holds true for any points in the field if the line charge is infinitely long so we can say E is radiating on the r direction only.
 
  • #7
mvpshaq32 said:
does radially outward not mean outward in all directions?

It depends on the context. In a situation with spherical symmetry, e.g. a point charge, it means "outwards in all directions from the center." In a situation with cylindrical symmetry, e.g. a line charge, it means "perpendicularly outwards from the axis of symmetry."
 

Related to Gauss's Law for Line of Charge

1. What is Gauss's Law for Line of Charge?

Gauss's Law for Line of Charge is a mathematical equation that relates the electric field created by a charged line to the charge density along that line. It is a special case of Gauss's Law, which is a fundamental principle in electromagnetism.

2. How does Gauss's Law for Line of Charge work?

Gauss's Law for Line of Charge states that the electric field at any point around a charged line is directly proportional to the charge density at that point and inversely proportional to the distance from the line. This means that the closer a point is to the line and the higher the charge density is at that point, the stronger the electric field will be.

3. What is the formula for Gauss's Law for Line of Charge?

The formula for Gauss's Law for Line of Charge is E = λ/2πε0r, where E is the electric field, λ is the charge density, r is the distance from the line, and ε0 is the permittivity of free space.

4. How is Gauss's Law for Line of Charge used in practical applications?

Gauss's Law for Line of Charge is used in various practical applications, such as calculating the electric field created by power lines or transmission cables. It is also used in designing electronic devices and analyzing the behavior of charged particles in electric fields.

5. What is the significance of Gauss's Law for Line of Charge in the study of electromagnetism?

Gauss's Law for Line of Charge is an important concept in the study of electromagnetism as it helps us understand the behavior of electric fields and their relationship to the distribution of charges. It is also a fundamental building block in the study of more complex cases of Gauss's Law, such as Gauss's Law for a closed surface.

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