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Dielectric Boundary Conditions - ITTC

11/4/2004 Dielectric Boundary 1/4 Jim Stiles The Univ. of Kansas Dept. of EECS Dielectric Boundary Conditions Consider the interface between two dissimilar Dielectric regions: Say that an electric field is present in both regions, thus producing also an electric flux density (()()rr =DE). Q: How are the fields in Dielectric region 1 ( , ()()11r, r D) related to the fields in region 2 ( , ()()22r, r D)? A: They must satisfy the Dielectric Boundary Conditions !

11/4/2004 Dielectric Boundary Conditions.doc 3/4 Jim Stiles The Univ. of Kansas Dept. of EECS The tangential component of the electric field at one side of the dielectric boundary is equal to the tangential component at the other side ! We can likewise consider the electric flux densities on the dielectric interface in terms of their normal and tangential

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Transcription of Dielectric Boundary Conditions - ITTC

1 11/4/2004 Dielectric Boundary 1/4 Jim Stiles The Univ. of Kansas Dept. of EECS Dielectric Boundary Conditions Consider the interface between two dissimilar Dielectric regions: Say that an electric field is present in both regions, thus producing also an electric flux density (()()rr =DE). Q: How are the fields in Dielectric region 1 ( , ()()11r, r D) related to the fields in region 2 ( , ()()22r, r D)? A: They must satisfy the Dielectric Boundary Conditions !

2 ()()11r, r D()()22r, r D1 2 11/4/2004 Dielectric Boundary 2/4 Jim Stiles The Univ. of Kansas Dept. of EECS First, let s write the fields at the Dielectric interface in terms of their normal (()rnE) and tangential (()rtE) vector components: Our first Boundary condition states that the tangential component of the electric field is continuous across a Boundary . In other words: ()()12rrtbtb=EE where rbdenotes any point on the Boundary ( , Dielectric interface). ()()()11 1rrrtn=+ ()1rn 1 2 na()1rt ()2rt ()2rn ()()()22 2rrrtn=+ 11/4/2004 Dielectric Boundary 3/4 Jim Stiles The Univ.

3 Of Kansas Dept. of EECS The tangential component of the electric field at one side of the Dielectric Boundary is equal to the tangential component at the other side ! We can likewise consider the electric flux densities on the Dielectric interface in terms of their normal and tangential components: The second Dielectric Boundary condition states that the normal vector component of the electric flux density is continuous across the Dielectric Boundary . In other words: ()()12rrnbnb=DD where rbdenotes any point on the Dielectric Boundary ( , Dielectric interface).

4 ()()111rr =D ()1rnD1 2 na()1rtD()2rtD()2rnD()()222rr=D 11/4/2004 Dielectric Boundary 4/4 Jim Stiles The Univ. of Kansas Dept. of EECS Since ()()rr=D , these Boundary Conditions can likewise be expressed as: ()()()()121212rrrrtbtbtbtb==EEDD and as: ()()()()121122rrrrnbnbnbnb==DDEE MAKE SURE YOU UNDERSTAND THIS: These Boundary Conditions describe the relationships of the vector fields at the Dielectric interface only ( , at points brr=)!!!! They say nothing about the value of the fields at points above or below the interface.

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