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Ch. 27 : GAUSS’ LAW

Ch. 27 : GAUSS’ LAW. Electric Flux. Gauss’ Law. Applications of Gauss’ Law. Conductors. Flux of a Vector Field. rate of flow of a fluid through the surface A:  vA ,.  vA cosØ (when the rectangle is tilted at an angle Ø.). Flux of a Vector Field.

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Ch. 27 : GAUSS’ LAW

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  1. Ch. 27: GAUSS’ LAW • Electric Flux • Gauss’ Law • Applications of Gauss’ Law • Conductors

  2. Flux of a Vector Field rate of flow of a fluid through the surface A:  vA , vA cosØ (when the rectangle is tilted at an angle Ø.)

  3. Flux of a Vector Field This rate is defined as the FLUXof the velocity vector v => A measure of number of field lines passing through area.

  4. Electric flux For a flat surface  to the field lines the electric flux ØE = EA S.I. unit (Nm2/C)

  5. Electric flux If surface area is not perpendicular to the field, A’ = A cos  The # of lines through A’ = the # through A => the flux through A’ = the flux through A ØE = EA cos 

  6. Electric Flux for non uniform electric field • divide the surface into large number of small elements, each of area DA. • define a vector DAi , magnitude = the area of the ith surface element direction = perpendicular to the surface element

  7. Electric Flux for non uniform electric field The flux through the element DFE = EiDAi cos q = Ei .DAi

  8. Electric Flux for non uniform electric field the total flux through the surface = sum of contributions of all elements.

  9. Electric Flux through Closed Surface Flux through area element 1 : positive 2 : zero 3: negative

  10. Example: Electric Flux through a Cube E along x-axis: To find the net electric flux. 1 2 3 4 5 6 =0 +0 +0 +0 +0 FE= +El2 -El2

  11. Electric Flux Through a Cone A horizontal uniform field E penetrates the cone. To find E that enters the left hand side of the cone. E = - E (1/2  2R  h) = - E R h

  12. Ex: 27-8: To find the flux through the netting: relative to the outward normal. Ans: E = -Ea2

  13. Ex: 27-11: A point charge q is placed at one corner of a cube of edge a . To find the flux through each of the cube faces: Ans: E = 0 (for each face touching q); = 1/240 (for other faces)

  14. GAUSS’ LAW This law is useful to calculate E set up by a point charge/collection of charges. Gauss’ Law relates the net flux through any closed surface to the net charge enclosed by the surface; as:

  15. Gaussian surface: an imaginary closed surface constructed in space Gaussian surface Spherical Gaussian surfaces positive point charge negative point charge.

  16. + Choosing the Gaussian surface A spherical Gaussian surface of radius r centered on the charge +q.

  17. The net flux through the Gaussian surface: For the spherical surface,

  18. S3 S2 S1 q Flux is independent of the radius r of the spherical Gaussian surface. Flux is independent of the size of Gaussian surface

  19. Flux through S1 = q / o the number of field lines through S1 = number of field lines through S2 or S3. => the net flux through any closed surface is independent of the shape of thatsurface

  20. Gauss’s Law – Charge outside closed surface A point charge is located outside closed surface. The number of lines entering the surface equals the number of lines leaving the surface. The net flux within the surface is zero.

  21. Quick Quiz A spherical gaussian surface surrounds a point charge q. Describe what happens to the total flux through the surface if : 1.the radius of the sphere is doubled 2.the surface is changed to a cube 3. the charge is tripled 4.the charge is moved to another location inside the surface.

  22. Gauss’ Law in Differential Form: The integral form: When the charge contained within the surface S is continuously distributed within a volume of charge density :

  23. Recall: Divergence theorem Applying this,

  24. The divergence can be interpreted as the number of field lines starting/terminating at a given point: => The number of field lines starting or terminating at a given point is proportional to the charge density at that point.

  25. Divergence of E Electric field at any field point r:

  26. Gauss’ law in differential form

  27. THE CURL of E Electric field at a field point r, due to a point charge at origin: Recall:

  28. Recall: Stokes’ theorem

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