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APPLICATION OF GAUSS’S LAW
Dr. Nadeem Khalid
AL-AQSA ACADEMY, LAHORE
 Intensity of field inside a Hollow Charged Sphere
• E = 0
 Electric intensity due to an infinite sheet of charge
• E =
𝜎
2ϵ0
 Electric intensity between to oppositely charged Parallel plates
• E =
𝜎
ϵ0
PLAN TO TALK
6/27/2020 2
• 4 steps
1. Gaussian Surface
2. Charged enclosed
3. Total flux
4. Electric intensity
ELECTRIC INTENSITY DUE TO AN
INFINITE SHEET OF CHARGE
6/27/2020 3
•Step 1
• Gaussian surface
ELECTRIC INTENSITY DUE TO AN
INFINITE SHEET OF CHARGE
6/27/2020 4
•Step 2
• Charged enclosed
• To find this first we know about concept of surface charge density(𝜎)
• 𝜎 =
𝑞
𝐴
……..(A)
• From equation …(A)
• q = 𝜎 𝐴
ELECTRIC INTENSITY DUE TO AN
INFINITE SHEET OF CHARGE
6/27/2020 5
•Step 3
• Total flux
1. Right end flat surface
2. Left end flat surface
3. Curved surface
 Right end flat surface
ELECTRIC INTENSITY DUE TO AN
INFINITE SHEET OF CHARGE
6/27/2020 6
 Left end flat surface
 Flux through curved surface
• 𝜑e3 = 0
 Total flux
 𝜑 = 2EA……….(1)
ELECTRIC INTENSITY DUE TO AN
INFINITE SHEET OF CHARGE
6/27/2020 7
•Step 4
• Calculation of electric intensity
• According to gauss’s law
• 𝜑e =
1
ϵ0
(q)…………(2)
• Using 1 & 2
• 2EA = 1
ϵ0
(q)
• 2EA = 1
ϵ0
(𝜎 𝐴)
•E = 𝜎
2ϵ0
ELECTRIC INTENSITY DUE TO AN
INFINITE SHEET OF CHARGE
6/27/2020 8
• 4 steps
1. Gaussian Surface
2. Charged enclosed
3. Total flux
4. Electric intensity
ELECTRIC INTENSITY BETWEEN
TWO OPPOSITELY CHARGED
PARALLEL PLATES
6/27/2020 9
•Step 1
• Gaussian surface
ELECTRIC INTENSITY BETWEEN
TWO OPPOSITELY CHARGED
PARALLEL PLATES
6/27/2020 10
•Step 2
• Charged enclosed
• To find this first we know about concept of surface charge density(𝜎)
• 𝜎 =
𝑞
𝐴
……..(A)
• From equation …(A)
• q = 𝜎 𝐴
ELECTRIC INTENSITY BETWEEN
TWO OPPOSITELY CHARGED
PARALLEL PLATES
6/27/2020 11
• Step 3
•Total flux
1. Flux through sides of box
2. Flux through upper surface of box
3. Flux through lower surface of box
• Flux through sides of box
• 𝜑 = 0
• Flux through upper surface of box
• 𝜑 = 0
ELECTRIC INTENSITY BETWEEN
TWO OPPOSITELY CHARGED
PARALLEL PLATES
6/27/2020 12
• Flux through lower surface of box
• Total flux
• 𝜑 = EA………(1)
ELECTRIC INTENSITY BETWEEN
TWO OPPOSITELY CHARGED
PARALLEL PLATES
6/27/2020 13
• Step 4
• Calculation of electric intensity
• 𝜑e =
1
ϵ0
(q)…………(2)
• Using 1 & 2
• EA = 1
ϵ0
(q)
• EA = 1
ϵ0
(𝜎 𝐴)
•E = 𝜎
ϵ0
ELECTRIC INTENSITY BETWEEN
TWO OPPOSITELY CHARGED
PARALLEL PLATES
6/27/2020 14
6/27/2020 15
ANSWER : D
PRACTICE TEST
6/27/2020 16
ANSWER : C
PRACTICE TEST
6/27/2020 17
6/27/2020 18

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Application of gausses law

  • 1. APPLICATION OF GAUSS’S LAW Dr. Nadeem Khalid AL-AQSA ACADEMY, LAHORE
  • 2.  Intensity of field inside a Hollow Charged Sphere • E = 0  Electric intensity due to an infinite sheet of charge • E = 𝜎 2ϵ0  Electric intensity between to oppositely charged Parallel plates • E = 𝜎 ϵ0 PLAN TO TALK 6/27/2020 2
  • 3. • 4 steps 1. Gaussian Surface 2. Charged enclosed 3. Total flux 4. Electric intensity ELECTRIC INTENSITY DUE TO AN INFINITE SHEET OF CHARGE 6/27/2020 3
  • 4. •Step 1 • Gaussian surface ELECTRIC INTENSITY DUE TO AN INFINITE SHEET OF CHARGE 6/27/2020 4
  • 5. •Step 2 • Charged enclosed • To find this first we know about concept of surface charge density(𝜎) • 𝜎 = 𝑞 𝐴 ……..(A) • From equation …(A) • q = 𝜎 𝐴 ELECTRIC INTENSITY DUE TO AN INFINITE SHEET OF CHARGE 6/27/2020 5
  • 6. •Step 3 • Total flux 1. Right end flat surface 2. Left end flat surface 3. Curved surface  Right end flat surface ELECTRIC INTENSITY DUE TO AN INFINITE SHEET OF CHARGE 6/27/2020 6
  • 7.  Left end flat surface  Flux through curved surface • 𝜑e3 = 0  Total flux  𝜑 = 2EA……….(1) ELECTRIC INTENSITY DUE TO AN INFINITE SHEET OF CHARGE 6/27/2020 7
  • 8. •Step 4 • Calculation of electric intensity • According to gauss’s law • 𝜑e = 1 ϵ0 (q)…………(2) • Using 1 & 2 • 2EA = 1 ϵ0 (q) • 2EA = 1 ϵ0 (𝜎 𝐴) •E = 𝜎 2ϵ0 ELECTRIC INTENSITY DUE TO AN INFINITE SHEET OF CHARGE 6/27/2020 8
  • 9. • 4 steps 1. Gaussian Surface 2. Charged enclosed 3. Total flux 4. Electric intensity ELECTRIC INTENSITY BETWEEN TWO OPPOSITELY CHARGED PARALLEL PLATES 6/27/2020 9
  • 10. •Step 1 • Gaussian surface ELECTRIC INTENSITY BETWEEN TWO OPPOSITELY CHARGED PARALLEL PLATES 6/27/2020 10
  • 11. •Step 2 • Charged enclosed • To find this first we know about concept of surface charge density(𝜎) • 𝜎 = 𝑞 𝐴 ……..(A) • From equation …(A) • q = 𝜎 𝐴 ELECTRIC INTENSITY BETWEEN TWO OPPOSITELY CHARGED PARALLEL PLATES 6/27/2020 11
  • 12. • Step 3 •Total flux 1. Flux through sides of box 2. Flux through upper surface of box 3. Flux through lower surface of box • Flux through sides of box • 𝜑 = 0 • Flux through upper surface of box • 𝜑 = 0 ELECTRIC INTENSITY BETWEEN TWO OPPOSITELY CHARGED PARALLEL PLATES 6/27/2020 12
  • 13. • Flux through lower surface of box • Total flux • 𝜑 = EA………(1) ELECTRIC INTENSITY BETWEEN TWO OPPOSITELY CHARGED PARALLEL PLATES 6/27/2020 13
  • 14. • Step 4 • Calculation of electric intensity • 𝜑e = 1 ϵ0 (q)…………(2) • Using 1 & 2 • EA = 1 ϵ0 (q) • EA = 1 ϵ0 (𝜎 𝐴) •E = 𝜎 ϵ0 ELECTRIC INTENSITY BETWEEN TWO OPPOSITELY CHARGED PARALLEL PLATES 6/27/2020 14
  • 16. ANSWER : D PRACTICE TEST 6/27/2020 16
  • 17. ANSWER : C PRACTICE TEST 6/27/2020 17