工程电磁场第三章ppt课件.ppt

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1、Engineering ElectromagneticsW.H. Hayt Jr. and J. A. BuckChapter 3:Electric Flux Density, Gauss Law,and DivergenceFaraday ExperimentHe started with a pair of metal spheres of different sizes; the larger one consisted of two hemispheres that could be assembled around the smaller sphere+QFaraday Appara

2、tus, Before GroundingThe inner charge, Q, inducesan equal and opposite charge, -Q, on the inside surface of theouter sphere, by attracting free electrons in the outer material towardthe positive charge. This means that before the outer sphere is grounded, charge +Q resides on the outside surface of

3、the outer conductor. Faraday Apparatus, After Groundingq = 0ground attachedAttaching the ground connects theouter surface to an unlimited supplyof free electrons, which then neutralize the positive charge layer. The net charge on the outer sphere is then the charge on the inner layer, or -Q.Interpre

4、tation of the Faraday Experimentq = 0Faraday concluded that there occurreda charge “displacement” from the inner sphere to the outer sphere.Displacement involves a flow or flux, existingwithin the dielectric, and whose magnitudeis equivalent to the amount of “displaced” charge.Specifically: Electric

5、 Flux Densityq = 0The density of flux at the inner sphere surfaceis equivalent to the density of charge there (in Coul/m2)Vector Field Description of Flux Densityq = 0A vector field is established which points in the direction of the “flow”or displacement. In this case, thedirection is the outward r

6、adial direction in spherical coordinates. At each surface,we would have:Radially-Dependent Electric Flux Densityq = 0rAt a general radius r betweenspheres, we would have:Expressed in units of Coulombs/m2, and defined over the range (a r b)D(r)Point Charge FieldsIf we now let the inner sphere radius

7、reduce to a point, while maintaining the same charge, and let the outer sphere radius approach infinity, we have a point charge. The electric flux density is unchanged, but is defined over all space: C/m2 (0 r )We compare this to the electric field intensity in free space:V/m (0 r ).and we see that:

8、Finding E and D from Charge DistributionsWe learned in Chapter 2 that:It now follows that:Gauss LawThe electric flux passing through any closed surface is equal to the total charge enclosed by that surfaceDevelopment of Gauss LawWe define the differential surface area (a vector) aswhere n is the uni

9、t outwardnormal vector to the surface, and where dS is the area of thedifferential spot on the surface Mathematical Statement of Gauss LawLine charge:Surface charge:Volume charge:in which the charge can exist in the form of point charges:For a volume charge, we would have: or a continuous charge dis

10、tribution: Using Gauss Law to Solve for D Evaluated at a SurfaceKnowing Q, we need to solve for D, using Gauss Law:The solution is easy if we can choose a surface, S, over which to integrate (Gaussian surface)that satisfies the following two conditions:The integral now simplfies:So that:whereExample

11、: Point Charge FieldBegin with the radial flux density:and consider a spherical surface of radius a that surrounds the charge, on which:On the surface, the differential area is:and this, combined with the outward unit normal vector is:Point Charge Application (continued)Now, the integrand becomes:an

12、d the integral is set up as:=Another Example: Line Charge FieldConsider a line charge of uniform charge density L on the z axis that extends over the range z We need to choose an appropriate Gaussian surface, being mindful of these considerations:We know from symmetry that the field will be radially

13、-directed (normalto the z axis) in cylindrical coordinates:and that the field will vary with radius only:So we choose a cylindrical surface of radius , and of length L.Line Charge Field (continued)Giving:So that finally:Another Example: Coaxial Transmission LineWe have two concentric cylinders, with

14、 the z axis down their centers. Surface charge of density S existson the outer surface of the inner cylinder.A -directed field is expected, and this should vary only with (like a line charge). We therefore choosea cylindrical Gaussian surface of length L and of radius , where a b.The left hand side

15、of Gauss Law is written:and the right hand side becomes:Coaxial Transmission Line (continued)We may now solve for the flux density:and the electric field intensity becomes:Coaxial Transmission Line: Exterior FieldIf a Gaussian cylindrical surface is drawn outside (b), a total charge of zero is enclo

16、sed, leading to the conclusion thator:Electric Flux Within a Differential Volume ElementTaking the front surface, for example, we have:Electric Flux Within a Differential Volume ElementWe now have:and in a similar manner:Therefore:minus sign because Dx0 is inward flux through the back surface.Charge

17、 Within a Differential Volume ElementNow, by a similar process, we find that:andAll results are assembled to yield:v= Q(by Gauss Law)where Q is the charge enclosed within volume vDivergence and Maxwells First EquationMathematically, this is:Applying our previous result, we have:div A =and when the v

18、ector field is the electric flux density:= div DMaxwells first equationDivergence Expressions in the Three Coordinate SystemsThe Del Operator = div D=The del operator is a vector differential operator, and is defined as:Note that:Divergence TheoremWe now have Maxwells first equation (or the point form of Gauss Law) which states:and Gausss Law in large-scale form reads:leading to the Divergence Theorem:Statement of the Divergence Theorem