Is Gauss' Law Accurate for Point Charge Divergence in Electrostatics?

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SUMMARY

The discussion centers on the application of Gauss' Law in electrostatics, specifically regarding the divergence of the electric field (E-field) for point charges. Participants clarify that while the differential form of Gauss' Law indicates the divergence at a point is proportional to the charge density at that point, it does not imply independence from charge distributions elsewhere. The divergence of the E-field is influenced by the entire charge distribution in space, not just local charge density. This understanding is crucial for accurately applying Maxwell's equations in electrostatics.

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  • Understanding of Gauss' Law in electrostatics
  • Familiarity with Maxwell's equations
  • Knowledge of vector calculus, particularly divergence
  • Basic concepts of electric fields and charge density
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Jame
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I've "derived" the first Maxwell equation of the divergence of the E-field starting at the Coulomb force of a point charge using Gauss law and even the Dirac delta function to justify the divergence at the origin.

Now I'm wondering: when you state the law in differential form, i.e. not specifying a volume over which the relation is to hold, I take it for being valid as a first order approximation in the neighborhood of a point. Reasonable?

Also, does it make sense to think of the divergence at that point as independent of the charge density outside the local neighborhood? Just as Gauss law says. If so, given the electric field in a volume of space, the charge density at the same point is

\rho(\vec{r}) \propto \nabla \cdot \vec{E}.

Or am I missing something here? (Apart from the permitivity constant)
 
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You are missing something here. =P

The differential forms of the Maxwell equations are point form equation; i.e. their validity prevails at all points in space with no reference to bounds. The differential form of Gauss' law does NOT say "the divergence at that point as independent of the charge density outside the local neighborhood." It does, however, say exactly the equation you have written.

On the left side, you have a charge (density) distribution throughout space. On the right side is a spatial derivative. In one dimension, the derivative depends on points ahead and behind of the specific point in question; this generalizes to three dimensions. Therefore, the right side depends not just on the charge at a specific point but rather on the charge distribution throughout space.

As a simple example, think of the field distribution of an isolated charge and its associated divergence. Now place a second charge at an arbitrary distance away from the first and think qualitatively of how the field distribution changes. The second charge, being arbitrarily placed, could be considered "outside the local neighborhood," but in general will affect the divergence.
 
cmos said:
The second charge, being arbitrarily placed, could be considered "outside the local neighborhood," but in general will affect the divergence.

No, it wont.

Gauss' law says that the divergence of the electric field at any given point is proportional to the charge density at that point. It doesn't matter if another charge is placed somewhere else or not. In general, the electric field will change, but the divergence will not. The divergence of E at any point depends only on the charge density at that point and nothing else.
 
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