Do you know that if we know the charge distribution, then we can calculate the electric field due to this charge distribution? This is based on the gauss law of electrostatics.

**Statement**. Total electric flux through any closed surface, is equal to 1/ε times the total charge enclosed by the surface.

Ф_{E}=∫E.dS=q/ε

Where ε is the permittivity of the medium (for free space ε=ε_{0}),

So Ф_{E}=∫E.dS=q/ε_{0}

Where ∫E.dS is surface integral over the closed surface and q is the charge present in the closed surface S

The imaginary closed surface is called Gaussian Surface. If the surface encloses a continuous charge distribution then q is replaced by the intergal ∫ρdV,where ρ is the volume charge density.

**Proof of gauss law of electrostatics:**

Consider a source producing the electric field E is a point charge +q situated at a point O inside a volume enclosed by an arbitrary closed surface S. let us consider a small area element ds around a point P on the surface where the electric field produced by the charge +q is E. if E is along OP and area vector dS is along the outward drawn normal to the area element dS, (Try to make the diagram yourself),

Then the electric flux dФ through the area element dS is given by

dФ=E.dS=EdS cosθ

Where θ is the angle between E and dS and it is zero degree, therefore

dФ = EdS (1)

Since the source producing E at dS is a point charge +q at O, therefore

E=1/4πε_{0} q/(OP)^{2}=1/4πε_{0}q/r^{2} (OP=r)

Substituting this value of E in equation (1),we get

dФ=E.dS=q/4πε_{0}dS/r^{2} (2)

Hence , total electric flux Ф through the entire closed surface S would be

∫dФ=q/4πε_{0} r^{2}∫dS (3)

But ∫dS = 4πr^{2}

Therefore, equation(3) becomes

Ф=∫E.dS= q4πε_{0} r^{2} /4πε_{0} r^{2}

Or Ф=∫E.dS= q/ε_{0 } (4)

Equation (4) represents Gauss law for electrostatics for a single point charge. If the source producing the electric field has more than one point charges such as +q_{1},+q_{2,}+q_{3},-q_{4}.-q_{5},-q_{6………..}etc,then the total flux due to all of them would be the algebric sum of all the fluxes as,

Ф=∫E.dS=1/ε_{0}(q_{1}+q_{2}+q_{3}-q_{4}-q_{5}-q_{6…….})

Or Ф=∫E.dS=∑q/ε_{0}

**Hence proved a charge outside the Gaussian surface would contribute nothing to the electric flux. **

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