点击下载:中国科学技术大学:《电磁学》课程教学资源(PPT课件讲稿)Chapter 7 Dielectrics:II
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3. the Tangential Component of e As we know in the static case. the electric field is curless VXE=0, i.e. along any closed path c the integral IcE.dI=0 Taking a closed path around the boundary as shown in Fig 7-2, we have E11-Et2L=0,→E1=Et2
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点击下载:中国科学技术大学:《电磁学》课程教学资源(PPT课件讲稿)Chapter 7 Dielectrics:II
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