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GUASS’S LAW & ITS APPLICATIONS

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GUASS’S LAW & ITS APPLICATIONS. Lecture No.4 By. Sajid Hussain Qazi. Learning Goals - we will learn: - PowerPoint PPT Presentation
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GUASS’S LAW & ITS APPLICATIONS Lecture No.4 By. Sajid Hussain Qazi
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Page 1: GUASS’S LAW & ITS APPLICATIONS

GUASS’S LAW & ITS APPLICATIONSLecture No.4By. Sajid Hussain Qazi

Page 2: GUASS’S LAW & ITS APPLICATIONS

Learning Goals - we will learn: • How you can determine the amount of

charge within a closed surface by examining the electric field on the surface!• What is meant by electric flux and how

you can calculate it.• How to use Gauss’s Law to calculate the electric field due to a symmetric distribution of charges.

Page 3: GUASS’S LAW & ITS APPLICATIONS

A charge inside a box can be probed with a test charge qo to measure E field

outside the box.

Page 4: GUASS’S LAW & ITS APPLICATIONS

The volume (V) flow rate (dV/dt) of fluid through the wire rectangle (a) is vA when the area of the rectangle is perpendicular to the velocity vector v and (b) is vA cos f when the rectangle is tilted at an angle f. We will next replace the fluid velocity flow vector v with the electric field vector E to get to the concept of electric flux FE.

Volume flow rate through the wire rectangle.

Page 5: GUASS’S LAW & ITS APPLICATIONS

(a) The electric flux through the surface = EA. (b) When the area vector makes an angle f with the vector E, the area projected onto a plane oriented perpendicular to the flow is A perp.   = A cos f.  The flux is zero when f = 90o because the rectangle lies in a plane parallel to the flow and no fluid flows through the rectangle

A flat surface in a uniform electric field.

Page 6: GUASS’S LAW & ITS APPLICATIONS

FE = ò E . dA = ò E dA cos f

= ò  E dA = E ò dA = E (4p R2)

= (1/4p eo) q /R2) (4p R2)

= q / eo. So the electric flux 

FE = q / eo. 

Now we can write Gauss's Law:

FE = ò E . dA = ò |EdA| cos f =Qencl /eo

Electric FLUX through a sphere centered on a point charge q.

Page 7: GUASS’S LAW & ITS APPLICATIONS

The projection of an element of area dA of

a sphere of radius R UP onto a concentric

sphere of radius 2R. The projection

multiplies each linear dimension by 2, so the area element on the

larger sphere is 4 dA.

The same number of lines of flux pass thru each area element.

Flux FE from a point charge q.

Page 8: GUASS’S LAW & ITS APPLICATIONS

Flux through an irregular surface.

The projection of the area element dA onto

the spherical surface is dA cos f.

Page 9: GUASS’S LAW & ITS APPLICATIONS

Spherical Gaussian surfaces around (a) positive and (b) negative point charge.

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Gauss’s Law can be used to calculate the magnitude of the E field vector:

C 2012 J. F. Becker

Page 11: GUASS’S LAW & ITS APPLICATIONS

Use the following recipe for Gauss’s Law problems:

Page 12: GUASS’S LAW & ITS APPLICATIONS

Use the following recipe for Gauss’s Law problems:

1. Carefully draw a figure - location of all charges, direction of electric field vectors E

Page 13: GUASS’S LAW & ITS APPLICATIONS

Use the following recipe for Gauss’s Law problems:

1. Carefully draw a figure - location of all charges, direction of electric field vectors E2. Draw an imaginary closed Gaussian surface so that the value of the magnitude of the electric field is constant on the surface and the surface contains the point at which you want to calculate the field. 

Page 14: GUASS’S LAW & ITS APPLICATIONS

Use the following recipe for Gauss’s Law problems:

1. Carefully draw a figure - location of all charges, direction of electric field vectors E2. Draw an imaginary closed Gaussian surface so that the value of the magnitude of the electric field is constant on the surface and the surface contains the point at which you want to calculate the field.  3. Write Gauss Law and perform dot product E o dA

Page 15: GUASS’S LAW & ITS APPLICATIONS

Use the following recipe for Gauss’s Law problems:

1. Carefully draw a figure - location of all charges, direction of electric field vectors E2. Draw an imaginary closed Gaussian surface so that the value of the magnitude of the electric field is constant on the surface and the surface contains the point at which you want to calculate the field.  3. Write Gauss Law and perform dot product E o dA 4. Since you drew the surface in such a way that the magnitude of the E is constant on the surface, you can factor the |E| out of the integral.

Page 16: GUASS’S LAW & ITS APPLICATIONS

Use the following recipe for Gauss’s Law problems:

1. Carefully draw a figure - location of all charges, direction of electric field vectors E2. Draw an imaginary closed Gaussian surface so that the value of the magnitude of the electric field is constant on the surface and the surface contains the point at which you want to calculate the field.  3. Write Gauss Law and perform dot product E . dA 4. Since you drew the surface in such a way that the magnitude of the E is constant on the surface, you can factor the |E| out of the integral.5. Determine the value of Qencl from your figure and insert it into Gauss's equation.

Page 17: GUASS’S LAW & ITS APPLICATIONS

Use the following recipe for Gauss’s Law problems:

1. Carefully draw a figure - location of all charges, and direction of electric field vectors E2. Draw an imaginary closed Gaussian surface so that the value of the magnitude of the electric field is constant on the surface and the surface contains the point at which you want to calculate the field.  3. Write Gauss Law and perform dot product E o dA 4. Since you drew the surface in such a way that the magnitude of the E is constant on the surface, you can factor the |E| out of the integral.5. Determine the value of Qencl from your figure and insert it into Gauss's equation. 6. Solve the equation for the magnitude of E.

C 2012 J. F. Becker

Page 18: GUASS’S LAW & ITS APPLICATIONS

Under electrostatic conditions, any excess charge resides entirely on the surface of a

solid conductor.

Gaussian

surface

Page 19: GUASS’S LAW & ITS APPLICATIONS

A coaxial cylindrical Gaussian surface is used to find the electric field outside an

infinitely long charged wire.

Page 20: GUASS’S LAW & ITS APPLICATIONS

A cylindrical Gaussian surface is used to find the electric field of an

infinite plane sheet of charge.

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The solution of this problem lies in the fact that the electric field inside a conductor is zero and if we place our Gaussian surface inside the conductor (where the field is zero), the charge enclosed must be zero (+ q – q) = 0. Find the electric charge q on surface of

a hole in the charged conductor.

+q


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