Gauss' Law: Discrete vs Continuous Charges

Click For Summary
SUMMARY

Gauss' Law applies to closed surfaces and is crucial for calculating electric fields around charge distributions. A Gaussian surface cannot pass through discrete charges because point charges have no physical size, leading to undefined electric fields at their location. In contrast, continuous charge distributions have defined dimensions, allowing Gaussian surfaces to intersect them. This distinction is essential for accurately applying Gauss' Law in electrostatics.

PREREQUISITES
  • Understanding of Gauss' Law and its mathematical formulation.
  • Familiarity with electric fields and charge distributions.
  • Knowledge of linear charge density and surface charge density concepts.
  • Basic principles of electrostatics and conductors versus dielectrics.
NEXT STEPS
  • Study the mathematical derivation of Gauss' Law in electrostatics.
  • Learn about electric field calculations for continuous charge distributions.
  • Explore the differences between conductors and dielectrics in electrostatics.
  • Investigate applications of Gauss' Law in various geometrical configurations.
USEFUL FOR

Students of physics, electrical engineers, and anyone interested in understanding electrostatics and the application of Gauss' Law in real-world scenarios.

physicsprasanna
Messages
20
Reaction score
0
why is it that a gaussian surface cannot pass through discrete charges ... but can pass through a continuous charge distribution??
 
Physics news on Phys.org
I believe technically, the Gaussian surface must enclose the charges, because Gauss's law applies to the enclosed charge.

http://hyperphysics.phy-astr.gsu.edu/hbase/electric/gaulaw.html#c2

The electric flux through an area is defined as the electric field multiplied by the area of the surface projected in a plane perpendicular to the field. Gauss's Law is a general law applying to any closed surface. It is an important tool since it permits the assessment of the amount of enclosed charge by mapping the field on a surface outside the charge distribution. For geometries of sufficient symmetry, it simplifies the calculation of the electric field.
Hyperphysics

For Gaussian surfaces -
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/gausur.html#c1

One can put a Gassian surface just outside a distributed charge.
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/gausur.html#c3
 
i mean ... yes, the gaussian surface should enclose charges .. but the surface should not pass through a discrete charge... but it can pass through a continuous charge distribution ... why is that?
 
id assume its fairly hard for it to pass through a point charge as you take the "size" of the charge to be 0 and therefore it cannot have anything pass through it, a continuous charge distribution however has a size and then the surface can pass through it
 
may i know what is distribution charge?
 
The electric field of a continuous charge distribution is everywhere defined, while the field of a point charge doesn't exist right at the location of the point charge. I believe that singularity is what invalidates the use of Gauss' law when the surface passes through it.
 
thanks for the replies ... maybe it is due to the fact that the field due to a charge does not exist at the place of the charge.

Thanks once again!
 
lifesfun said:
may i know what is distribution charge?
Simply a collection of charges, but mathematically we treat them as 'uniformly' distributed rather than discrete units.

In a line conductor, the charge is 'linear charge density' or charge/unit length (e.g. C/m).

On a surface conductor, one takes of charge/unit surface (e.g. C/m2) area as though the charges were 'smeared' on the surface. In a conductor, the net charge occurs near the surface because this represents least energy, and the charge units (electrons) are mobile.

In a dielectric, the charges are much less mobile and one can have a volumetric distribution (even non-uniform) of charge.

See - http://hyperphysics.phy-astr.gsu.edu/hbase/electric/elefie.html#c1

http://hyperphysics.phy-astr.gsu.edu/hbase/electric/gaulaw.html#c4
 

Similar threads

  • · Replies 12 ·
Replies
12
Views
1K
  • · Replies 26 ·
Replies
26
Views
3K
  • · Replies 22 ·
Replies
22
Views
3K
  • · Replies 10 ·
Replies
10
Views
2K
Replies
9
Views
747
Replies
10
Views
4K
  • · Replies 5 ·
Replies
5
Views
2K