当前位置:高等教育资讯网  >  中国高校课件下载中心  >  大学文库  >  浏览文档

中国科学技术大学:《电磁学》课程教学资源(PPT课件讲稿)Chapter 19 Maxwell’s Equations

资源类别:文库,文档格式:PPT,文档页数:24,文件大小:2.37MB,团购合买
The Total Current Density J The Curl of B Maxwell’s Equations Maxwell’s Equations in Integral Form
点击下载完整版文档(PPT)

Chapter 19 Maxwell,s Equations The Total Current density J The curl of b Maxwell's Equations Maxwell' s equations in Integral Form

Chapter 19 Maxwell’s Equations ◼ The Total Current Density J ◼ The Curl of B ◼ Maxwell’s Equations ◼ Maxwell’s Equations in Integral Form

So far we have obtained Maxwell s four equations + V·E V·B=0: OB VXE at VB=oJf + Je);(steady Generally?

19. 1 The Total Current Density J There are three kinds of current densities as follows The free current density Jf 2. The displacement current density OD 00P =(0E+ ot at at 3. The equivalent current density in magnetic ma terial VⅹM

Thus the total current density is the sum t=Je+(0ob⊥OP 0 +V×M 0t"0t 0 E Jm+ at where Jm is the volume current density in matter m=J× +V×M at

19.2 The Curl of b The fourth Maxwell equation V×B=0{Jr+Je);( stead should be generalized with the currents Jf Jere placed by the total current ji V×B a oP =0(Jf+0aE+ at +VM) 0 Jm+c0e or. rewritten as V×B-00aE=10Jm

Plugging B=0(H+M) Into 00P V×B=10(Jf+60。E+ +V×M) t at we get 00P V×H=Jf+60aE+ t at J D ot

Example: Dielectric-Filled Parallel-Plate Capacitor It is connected across a alternating source v and contains a slightly conducting dielectric with a per- mittivity Er 0 and a conductivity o.(neglecting the side effects) J aD or Figure 19-1 Parallel-plate capacitor connected to a source of alternating voltage The current J,+aD/dr gives an azimuthal magnetic field B

What is the magnetic induction inside the capacitor? B=? Remember that the material inside is dielectric but not magnetic, so M=0, and B=10(H+M)=10H, therefore the maxwell equation VXH=动 01 is simplified as V×B=10(Jf+ OD at Integrating this over an area s

we get OD sV×Bda=0/s(J+) Ot′ da Using Stokes Theorem, this is written as OD CB·dl=p0/s(J+x)·da, where C is the curve bounding the surface Let c to be a circle of radius r. Note that Jf+ ot is homogeneous. So OD 2丌B= 丌T OD B=OUf+ a ) ot

Now E=oV/s aD OE By the alternating property E-E(t=Ee! we have OD at CrEo, WE=ErE]wVs and B=(a+60)Vr Thus although Jf+aD/at is independent of r, the magnetic field b depends on r and is azimuthal

点击下载完整版文档(PPT)VIP每日下载上限内不扣除下载券和下载次数;
按次数下载不扣除下载券;
24小时内重复下载只扣除一次;
顺序:VIP每日次数-->可用次数-->下载券;
共24页,试读已结束,阅读完整版请下载
相关文档

关于我们|帮助中心|下载说明|相关软件|意见反馈|联系我们

Copyright © 2008-现在 cucdc.com 高等教育资讯网 版权所有