As an example of the statement that Maxwell's equations completely define electromagnetic phenomena, it will be shown that Coulomb's Law may be derived from Gauss' law for electrostatics. Consider a point charge. We can obtain an expression for the electric field surrounding the charge. We surround the charge with a "virtual" sphere of radius , then use Gauss' law in integral form:
We rewrite this as a volume integral in spherical polar coordinates over the "virtual" sphere mentioned above, which has the point charge at its center. Since the electric field is spherically symmetric (by assumption) the electric field is constant over this volume.
Hence
Or
The usual form can then be recovered from the Lorentz force law, noting the absence of magnetic field.
Limitations of coulombs law
from anonymous surfer.... They are equal the only difference is that when the distance of the charge electrons are far so distant from each other, it is much better to apply Gauss's law while Coloumbs law for the other.....
Gauss's law can be used to find the electric field strength within a slab by considering a Gaussian surface that encloses the slab. By applying Gauss's law, which relates the electric flux through a closed surface to the charge enclosed by that surface, one can derive an expression for the electric field strength within the slab.
Describe Gauss's law and its application to planar symmetry
No
Newtons law has to due with mass and ATTRACTION only Coulombs law has to due with charge and ATTRACTION AND REPULSION
Gauss law
gauss law is applicable to certain symmetrical shapes it cannot be used for disk and ring
coulombs law
Obviously. If the Gauss gun shoots pushes something out at the front, this object will push back against the Gauss gun (Newton's Third Law).
Gauss's Law states that the total electric flux through a closed surface is proportional to the total charge enclosed by that surface. In simpler terms, it describes how electric charges create an electric field in space.
Epsilon naught, represented by the symbol , is the permittivity of free space in Gauss's Law. It is a fundamental constant that relates the strength of electric fields to the distribution of electric charges in a given space. This constant plays a crucial role in determining the behavior of electric fields and the interactions between charges in the context of Gauss's Law.