Chapter 1: Negative Charge B

System Configuration and Geometry

  • System components:

    • Positive charge AA

    • Negative charge BB

  • Bounded regional evaluation surfaces:

    • Closed surface AA

    • Closed surface BB

    • Closed surface CC

    • Closed surface DD

Core Principles of Electric Flux and Gauss's Law

  • Gauss's Law defines the relationship between total electric flux ΦE\Phi_E passing through any closed surface and the net charge QencQ_{\text{enc}} enclosed within that volume: ΦE=EdA=Qencε0\Phi_E = \oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{\text{enc}}}{\varepsilon_0}

    • ΦE\Phi_E: Net electric flux through the closed surface.

    • E\mathbf{E}: Electric field vector.

    • dAd\mathbf{A}: Differential area vector directed orthogonally outward from the closed surface.

    • QencQ_{\text{enc}}: Net algebraic charge enclosed inside the surface boundary.

    • ε0\varepsilon_0: Vacuum permittivity constant.

Electric Flux Calculations Across Closed Surfaces

  • Closed Surface AA:

    • Encloses positive charge AA

    • Net enclosed charge: Qenc=+qAQ_{\text{enc}} = +q_A

    • Net flux through surface AA is positive (directed outward): ΦE,A=+qAε0\Phi_{E, A} = \frac{+q_A}{\varepsilon_0}

  • Closed Surface BB:

    • Encloses negative charge BB

    • Net enclosed charge: Qenc=qBQ_{\text{enc}} = -q_B

    • Net flux through surface BB is negative (directed inward): ΦE,B=qBε0\Phi_{E, B} = \frac{-q_B}{\varepsilon_0}

  • Closed Surface CC:

    • Encloses both positive charge AA and negative charge BB

    • Net enclosed charge: Qenc=qA+qB=qAqBQ_{\text{enc}} = q_A + q_B = q_A - |q_B|

    • If charges are equal in magnitude (qA=qB|q_A| = |q_B|), the net enclosed charge Qenc=0Q_{\text{enc}} = 0

    • Resulting electric flux through surface CC: ΦE,C=0\Phi_{E, C} = 0

  • Closed Surface DD:

    • Encloses zero charges (Qenc=0Q_{\text{enc}} = 0

    • Net electric flux through surface DD: ΦE,D=0\Phi_{E, D} = 0


System Configuration and Geometry
  • System components:

    • Positive charge AA

    • Negative charge BB

  • Bounded regional evaluation surfaces:

    • Closed surface AA

    • Closed surface BB

    • Closed surface CC

    • Closed surface DD

Core Principles of Electric Flux and Gauss's Law
  • Gauss's Law defines the relationship between total electric flux  Phi<em>E\ Phi<em>E passing through any closed surface and the net charge Q</em>encQ</em>{\text{enc}} enclosed within that volume: Φ<em>E=EdA=Q</em>encε0\Phi<em>E = \oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q</em>{\text{enc}}}{\varepsilon_0}

    • ΦE\Phi_E: Net electric flux through the closed surface.

    • E\mathbf{E}: Electric field vector.

    • dAd\mathbf{A}: Differential area vector directed orthogonally outward from the closed surface.

    • QencQ_{\text{enc}}: Net algebraic charge enclosed inside the surface boundary.

    • ε<em>0\varepsilon<em>0: Vacuum permittivity constant (ε</em>08.854×1012C2N1m2\varepsilon</em>0 \approx 8.854 \times 10^{-12}\,C^2\,N^{-1}\,m^{-2}).

Electric Flux Calculations Across Closed Surfaces
  • Closed Surface AA:

    • Encloses positive charge AA

    • Net enclosed charge: Q<em>enc=+q</em>AQ<em>{\text{enc}} = +q</em>A

    • Net flux through surface AA is positive (directed outward):
      Φ<em>E,A=+q</em>Aε0\Phi<em>{E, A} = \frac{+q</em>A}{\varepsilon_0}

  • Closed Surface BB:

    • Encloses negative charge BB

    • Net enclosed charge: Q<em>enc=q</em>BQ<em>{\text{enc}} = -q</em>B

    • Net flux through surface BB is negative (directed inward):
      Φ<em>E,B=q</em>Bε0\Phi<em>{E, B} = \frac{-q</em>B}{\varepsilon_0}

  • Closed Surface CC:

    • Encloses both positive charge AA and negative charge BB

    • Net enclosed charge: Q<em>enc=q</em>A+q<em>B=q</em>AqBQ<em>{\text{enc}} = q</em>A + q<em>B = q</em>A - |q_B|

    • If charges are equal in magnitude (q<em>A=q</em>B|q<em>A| = |q</em>B|), the net enclosed charge Qenc=0Q_{\text{enc}} = 0

    • Resulting electric flux through surface CC:
      ΦE,C=0\Phi_{E, C} = 0

  • Closed Surface DD:

    • Encloses zero charges (Qenc=0Q_{\text{enc}} = 0)

    • Net electric flux through surface DD:
      ΦE,D=0\Phi_{E, D} = 0

Example Problems
Problem 1: Calculating Flux for a Single Enclosed Charge
  • Question: A point charge q<em>A=+5.00×109Cq<em>A = +5.00 \times 10^{-9}\,C is enclosed inside Surface AA. Calculate the net electric flux Φ</em>E,A\Phi</em>{E, A} passing through Surface A$.

  • Solution:

    1. Apply Gauss's Law:
      \Phi{E, A} = \frac{Q{\text{enc}}}{\varepsilon_0}</p></li><li><p>Substitutethevalues</p></li><li><p>Substitute the valuesQ{\text{enc}} = +5.00 \times 10^{-9}\,Candand\varepsilon0 = 8.854 \times 10^{-12}\,C^2\,N^{-1}\,m^{-2}:<br>:<br>\Phi{E, A} = \frac{5.00 \times 10^{-9}\,C}{8.854 \times 10^{-12}\,C^2\,N^{-1}\,m^{-2}}\Phi{E, A} \approx 5.65 \times 10^2\,N\,m^2\,C^{-1}</p></li></ol></li></ul><h6>Problem2:CalculatingFluxforMultipleEnclosedCharges</h6><ul><li><p><strong>Question:</strong>Surface</p></li></ol></li></ul><h6>Problem 2: Calculating Flux for Multiple Enclosed Charges</h6><ul><li><p><strong>Question:</strong> SurfaceCenclosestwocharges:encloses two charges:qA = +3.00 \times 10^{-9}\,CandandqB = -7.00 \times 10^{-9}\,C.Determinethenetelectricflux. Determine the net electric flux\Phi_{E, C}throughSurfacethrough SurfaceC$.

    2. Solution:

      1. Find the net enclosed charge Q<em>encQ<em>{\text{enc}}: Q</em>enc=q<em>A+q</em>BQ</em>{\text{enc}} = q<em>A + q</em>B
        Qenc=(3.00×109C)+(7.00×109C)=4.00×109CQ_{\text{enc}} = (3.00 \times 10^{-9}\,C) + (-7.00 \times 10^{-9}\,C) = -4.00 \times 10^{-9}\,C

      2. Calculate the electric flux:
        Φ<em>E,C=4.00×109C8.854×1012C2N1m2\Phi<em>{E, C} = \frac{-4.00 \times 10^{-9}\,C}{8.854 \times 10^{-12}\,C^2\,N^{-1}\,m^{-2}} Φ</em>E,C4.52×102Nm2C1\Phi</em>{E, C} \approx -4.52 \times 10^2\,N\,m^2\,C^{-1}