Applying Gauss' Law: Solving Electric Field Problems

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SUMMARY

This discussion focuses on applying Gauss' Law to solve electric field problems, specifically using the equation ∮E.dA = qencl/ϵ0. The calculations demonstrate how to determine the electric field (E) for a cylindrical charge distribution, resulting in E = (Q1 + Q2)/(2πrLϵ0) with specific values leading to E = 0.214 N/C at r = 2.00R2 and E = 0.855 N/C at r = 5.00R1. The direction of the electric field is determined based on the sign of the enclosed charge (qencl), indicating radially inward or outward behavior depending on the charge configuration.

PREREQUISITES
  • Understanding of Gauss' Law and its application in electrostatics
  • Familiarity with electric field calculations and cylindrical symmetry
  • Knowledge of charge density and its relation to electric field strength
  • Basic proficiency in algebra and unit conversions in physics
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  • Study the derivation and applications of Gauss' Law in different geometries
  • Explore electric field calculations for spherical charge distributions
  • Learn about the concept of charge density and its impact on electric fields
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This discussion is beneficial for physics students, educators, and anyone interested in mastering electrostatics and electric field calculations using Gauss' Law.

yohanes vianei
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Homework Statement


upload_2019-2-16_22-26-27.png


Homework Equations


E.dA = qencl/ϵ0

The Attempt at a Solution


(a) magnitude E

we use∮E.dA = qencl/ϵ0For a cylinder:∮E.dA = E(2πrL), thenqencl/ϵ0 = E(2πrL)E = qencl/(2πrLϵ0) E = λ/(2πrϵ0); WITH λ = qencl/L



(a) the magnitude E, qencl = Q1 + Q2 , thenE = (Q1 + Q2)/(2πrLϵ0) Because:

· Q1 + Q2 = +3.40 x 10─12 C +( ─2 x 3.40 x 10─12 C) = ─3.40 x 10─12 C,

· Radius, r = 2.00R2 = 2.00 (10R1) = 20 x 1.3 mm = 26 x 10─3 m

· length L = 11.00 m

then,E = (─3.40 x 10─12 C)/(2π x 26 x 10─3 m x 11.00 m x 8.85 x10-12 C2/Nm2)

E = 0.214 N/C(b) direction (radially inward or outward) of the electric field at radial distance r = 2.00R2 is radially inward since qencl < 0(c) E for r = 5.00R1 = 5.00 x 1.3 mm = 6.5 x 10─3 m, and qencl = Q1 = +3.40 x 10─12 C, thenE = (+3.40 x 10─12 C)/(2π x 6.5 x 10─3 m x 11.00 m x 8.85 x10-12 C2/Nm2)

E = 0.855 N/C(d) the direction at r = 5.00R1 is radially outward since qencl > 0(e) the charge on the interior isQinner = ─ Q1 = ─3.40 x 10─12 C(f) the charge on the exterior surface of the shell is

Qouter = Q2 ─ Qinner = (─2 x 3.40 x 10─12 C) ─ (─3.40 x 10─12 C)

Qouter = ─3.40 x 10─12 C[/B]
 

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Hi johanes vianei and welcome to PF.

Is there a question you wish to ask?
 
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