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Gauss's Law

Electronics & Technology
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Gauss's law is a fundamental law in physics that relates the electric flux through a closed surface to the charge enclosed within the surface. It is named after the German mathematician and physicist Carl Friedrich Gauss, who formulated the law in its modern form in 1835.

In its integral form, Gauss's law states that the electric flux through a closed surface is proportional to the charge enclosed within the surface:

∮ S * E · dA = Qenc / ε0

where:

∮ S is the surface integral over a closed surface S

E is the electric field at each point on the surface S
 ·  indicates the dot (or inner) product
dA is the differential area element of the surface
Qenc is the total charge enclosed within the surface
ε0 is the electric constant, also known as the vacuum permittivity.

This equation implies that electric field lines originating from a positive charge and terminating at a negative charge are closed lines, with no beginning or end, and that the total electric flux through any closed surface is proportional to the charge enclosed within the surface. Gauss's law is a powerful tool for calculating electric fields in situations with high symmetry, such as spherical and cylindrical symmetry.

An alternate form of Gauss's law is the differential form, which relates the divergence of the electric field to the charge density at any point in space:

∇ · E = ρ / ε0

where:

∇ represents the divergence operator
 ·  indicates the dot (or inner) product
E represents the electric field vector
ρ represents the charge density at a given point in space
ε0 represents the electric constant or the permittivity of free space.

This equation states that the divergence of the electric field at any point in space is proportional to the charge density at that point. In other words, the electric field "flows" away from regions of high charge density, and "converges" towards regions of low charge density. This form of Gauss's law is particularly useful in situations where the electric field is not uniform, or where the geometry of the charge distribution is complex. It can also be used to derive the integral form of Gauss's law by applying the divergence theorem.


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