点击下载:《Electromagnetism, principles and application 》 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 CE. dI Taking a closed path around the boundary as shown in Fig 7-2, we have Et1L-Et2L=0,→E1=Et2
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点击下载:《Electromagnetism, principles and application 》 Chapter 7 Dielectrics: II
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