Gauss's Law for Line of Charge

Click For Summary
SUMMARY

This discussion focuses on Gauss's Law as it applies to an infinitely long line of charge. Participants clarify that when using a cylindrical Gaussian surface, the electric field (E field) is purely radial and perpendicular to the sides of the cylinder, resulting in zero flux through the ends. The symmetry of the infinite line charge ensures that any potential field components in the z direction cancel out, confirming that the E field is directed only radially outward. Thus, the flux through the ends of the cylinder is indeed zero due to the absence of a normal component of the electric field.

PREREQUISITES
  • Understanding of Gauss's Law
  • Familiarity with electric fields and flux concepts
  • Knowledge of cylindrical coordinates
  • Basic principles of symmetry in physics
NEXT STEPS
  • Study the application of Gauss's Law in different geometries
  • Learn about electric field calculations for various charge distributions
  • Explore the concept of symmetry in electrostatics
  • Investigate the implications of infinite charge distributions on electric fields
USEFUL FOR

Students of physics, educators teaching electromagnetism, and anyone seeking a deeper understanding of electric fields and Gauss's Law in the context of line charges.

mvpshaq32
Messages
28
Reaction score
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?
 
Physics news on Phys.org
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.
 
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
 
Just think about it from a symmetry point of view. Could there be a net field going one way or the other?
 
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.
 
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.
 
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."
 

Similar threads

  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 83 ·
3
Replies
83
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 5 ·
Replies
5
Views
4K
  • · Replies 20 ·
Replies
20
Views
2K
  • · Replies 30 ·
2
Replies
30
Views
3K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K