Apply Gauss' theorem to calculate the electric field due to an infinitely long charged straight wire.
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Amount of Electric flux passing through a closed surface or the surface integral of Electric field intensity is equal to the ratio of the Charge enclosed by the surface and the Permittivity of the free space.
ϕ=Qenclosedε0 ⇒∫E.dS=Qenclosedε0
Electric Field due to a Long Straight Charged Wire:
Consider a long straight wire charge by a linear charge density λ as shown in the figure below.
To find the electric field at a distance from the wire, consider a gaussian surface as shown in the figure.
Let the electric field at the surface is E. Then,
From the definition of gauss law,
∫E.dS=Qenclosedε0⇒E∫dS=Qε0⇒E(2πRL)=Qε0 ⇒ E=12πε0R(QL)⇒ E=λ2πε0R
✌️________✌️
ϕ=Qenclosedε0 ⇒∫E.dS=Qenclosedε0
Electric Field due to a Long Straight Charged Wire:
Consider a long straight wire charge by a linear charge density λ as shown in the figure below.
To find the electric field at a distance from the wire, consider a gaussian surface as shown in the figure.
Let the electric field at the surface is E. Then,
From the definition of gauss law,
∫E.dS=Qenclosedε0⇒E∫dS=Qε0⇒E(2πRL)=Qε0 ⇒ E=12πε0R(QL)⇒ E=λ2πε0R
✌️________✌️
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Answer:
Explanation:
According to the Gauss law, the total flux linked with a closed surface is 1/ε0 times the charge enclosed by the closed surface.
∮E⃗ .d⃗ s=1∈0q .
According to Gauss Law,
Φ = → E.d → A
Φ = Φcurved + Φtop + Φbottom
Φ = → E . d → A = ∫E . dA cos 0 + ∫E . dA cos 90° + ∫E . dA cos 90°
Φ = ∫E . dA × 1
Due to radial symmetry, the curved surface is equidistant from the line of charge and the electric field in the surface has a constant magnitude throughout.
Φ = ∫E . dA = E ∫dA = E . 2πrl
The net charge enclosed by the surface is:
qnet = λ.l
Using Gauss theorem,
Φ = E × 2πrl = qnet/ε0 = λl/ε0
E × 2πrl = λl/ε0
E = λ/2πrε0
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