1 / 32

ENE 325 Electromagnetic Fields and Waves

ENE 325 Electromagnetic Fields and Waves. Lecture 2 Static Electric Fields and Electric Flux density. Review (1). Vector quantity Magnitude Direction Coordinate systems Cartesian coordinates (x, y, z) Cylindrical coordinates (r,  , z) Spherical coordinates (r,  ,  ). Review (2).

starnesr
Télécharger la présentation

ENE 325 Electromagnetic Fields and Waves

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. ENE 325Electromagnetic Fields and Waves Lecture 2 Static Electric Fields and Electric Flux density

  2. Review (1) • Vector quantity • Magnitude • Direction • Coordinate systems • Cartesian coordinates (x, y, z) • Cylindrical coordinates (r, , z) • Spherical coordinates (r, , )

  3. Review (2) • Coulomb’s law • Coulomb’s force • electric field intensity (V/m)

  4. Review (3) • Key variables: • Coordinate system and its corresponding differential element • charge Q • a unit vector

  5. Outline • Electric field intensity in different charge configurations • infinite line charge • ring charge • surface charge • Examples from previous lecture • Electric flux density

  6. Infinite length line of charge • The derivation of and electric field at any point in space resulting from an infinite length line of charge. (good approximation)

  7. Infinite length line of charge • only varies with the radial distance  • select point P on  - z axis for convenience. • select a segment of charge dQ at distance –z, we then have

  8. Infinite length line of charge • Consider another segment at distance z, z components are cancelled out, we then have

  9. Infinite length line of charge • From We can write Total field

  10. Infinite length line of charge • Consider each segment • Ezcomponents are cancelled due to symmetry.

  11. Infinite length line of charge

  12. Ring of charge determine at (0,0,h) cancels each other

  13. Ring of charge Consider each segment:

  14. Surface charge • Surface charge density S (c/m2) dQ = Sdxdy Since this is an infinite place, Exand Ey components are cancelled due to symmetry.

  15. Surface charge • Consider each segment: Devide the whole area into infinite length of line charges Integrate over length y to get total electric field. Convert the radial component into cylindrical coordinates Ey components are cancelled out due to symmetry.

  16. Surface charge No dependence on a distance from the sheet

  17. Concentrate ring (alternative approach) for each ring Total field is integrated from  = 0 to  Then

  18. Volume charge • Volume charge density V (c/m3) • plasma • doped semiconductor • Complicate derivation due to so many differential elements and vectors.

  19. Ex1 Determine the distance between point P (5, /2, 10) and point Q (1, /3, 5) in cylindrical coordinates.

  20. Ex2 Determine a unit vector directed from (0, 0, h) to (r, , 0) in cylindrical coordinates.

  21. Ex3 Determine a unit vector from any point on z = -5 plane to the origin.

  22. Ex4 Find the area between 90135 on the surface of a sphere of a radius 1 m.

  23. Ex5 A charge Q1= 0.3C is located at (1,4,0). A charge Q2= 0.2 C is located at (3,0,0). Determine at point (0,0,5).

  24. Ex6 Determine at point (-2, -1, 4) given a line charge located at x = 2 and y = -4 with a charge density L = 20 nC/m.

  25. Ex7 Determine at the origin given a square sheet of charge located at z = -1 plane. The sheet is extended from -1  x  1 and -1  y  1with a surface charge density S = 2(x2+y2+1)3/2 nC/m2.

  26. Electric flux density • Negative charges are drawn to the outer sphere • Electric flux lines are radially directed away from inner sphere to outer sphere or begin from positive charges +Q and terminate on negative charges -Q.

  27. Electric flux density • Electric flux density, (C/m2) Note:  (chi) is a flux in Coulomb unit and is equal to charge Q on the sphere So we have where 0 = 8.854x10-12 Farad/m

  28. Electric flux density • The amount of flux passing through a surface isgiven by the product of and the amount of surface normal to. Same polarity charges repel one another Note: = surface vector • Dot product: for Cartesian coordinates. Dot product is a projection of A on B multiplies by B

  29. Electric flux density The flux through a surface that is an angle to the direction of flux a) is less than the flux through an equivalent surface normal to the direction of flux b) • In case the flux is varied over the surface,

  30. Ex8C/m2. Given the surface defined by  = 1 m, 090 and -1 z 1, calculate the flux through the surface.

  31. Ex9 A charge Q = 30 nC is located at the origin, determine the electric flux density at point (1, 2, -4) m.

  32. Ex10 Determine the flux through the area 1x1 mm2 on a surface of a cylinder at r = 10 m, z = 2 m,  = 53.2 given C/m2.

More Related