Gauss theorem and proof
*“Gauss' theorms”: According to this theorem, The net electric flux passing through closed surface which is placed in air/vacuum is 1/Eo times the total charge enclosed by closed surface.
Mathematical form: Φ = q. 1/Eo
Where, q = total charge enclosed by closed surface
Eo = permittivity of free space
* proof :
Let a charge +q be placed at centre 0 of a sphere of radius r . Any point P is placed on the surface of a sphere about this point ,we assuming an element of surface area ds . the solid angle subtended by area ds at the centre 0 be dw.
By the coulumb's Law :
Electric field intensity due to the point charge + q and the distance r is—
E = 1/4πEo × q/r² N/C
Thus the electric flux passing through small surface area ds—
dΦ = E. ds cosθ
Putting the value of E
dΦ = (1/4πEo × q/r²).ds cosθ
Taking surface integration
∫∫dφ = ∫∫ (1/4πEo × q/r²) dscosθ
φ = q/4πEo ∫∫ ds cosθ/r²
we know that
[small solid angle dw = ds cosθ/r²]
∴ φ = q/4πEo ∫∫ dw
φ = q/4πEo ×W
∵ total solid angle W = 4π
∴ φ = q/4πEo × 4π
[ φ = q/Eo ]
HENCE PROVED
Mathematical form: Φ = q. 1/Eo
Where, q = total charge enclosed by closed surface
Eo = permittivity of free space
* proof :
Let a charge +q be placed at centre 0 of a sphere of radius r . Any point P is placed on the surface of a sphere about this point ,we assuming an element of surface area ds . the solid angle subtended by area ds at the centre 0 be dw.
By the coulumb's Law :
Electric field intensity due to the point charge + q and the distance r is—
E = 1/4πEo × q/r² N/C
Thus the electric flux passing through small surface area ds—
dΦ = E. ds cosθ
Putting the value of E
dΦ = (1/4πEo × q/r²).ds cosθ
Taking surface integration
∫∫dφ = ∫∫ (1/4πEo × q/r²) dscosθ
φ = q/4πEo ∫∫ ds cosθ/r²
we know that
[small solid angle dw = ds cosθ/r²]
∴ φ = q/4πEo ∫∫ dw
φ = q/4πEo ×W
∵ total solid angle W = 4π
∴ φ = q/4πEo × 4π
[ φ = q/Eo ]
HENCE PROVED
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