use Gauss theorem to find the electric field due to a uniformly charged infinite plane sheet
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0
Answer:
Consider an infinite thin plane sheet of positive charge with a uniform surface charge density σ on both sides of the sheet. Let P be the point at a distance a from the sheet at which the electric field is required. Draw a Gaussian cylinder of area of cross-section A through point P.
Explanation:
Consider an infinite plane which carries the uniform charge per unit area σ
Let the plane coincides with the y−z plane.
Let us draw a cylindrical gaussian surface, whose axis is normal to the plane, and which is cut in half by the plane.
Let the cylinder run from x=−a to x=+a, and let its cross-sectional area be A. According to Gauss' law,
2E(a)A=
ϵ
0
σA
,
where E(a)=−E(−a) is the electric field strength at x=+a. Here, the left-hand side represents the electric flux out of the surface.
The only contributions to this flux come from the flat surfaces at the two ends of the cylinder. The right-hand side represents the charge enclosed by the cylindrical surface, divided by ϵ
0
. It follows that
E=
2ϵ
0
σ
.
Answered by
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Answer:
sigma/(2 epsilon0)
Explanation:
Using Gauss theorem derive an expression for electric field due to a uniformly charge infinite plane sheet.?
please see the enclosed attachment for detailed explanation and step by step working.
take an infinitely large charged sheet MNOP of charge density sigma.
Take a point P at the centre of EFGH. To find E at P, construct a Gaussian surface - a cuboid IJKL - EFGH . The electric field and flux lines flow out of the sheet perpendicular to it.
Gauuss's law:
closed Integral over cuboid of E • dA = q/epsilon0.
2 E = sigma/ epsilon0
E = sigma/(2 epsilon0)
Attachments:
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