This preview shows pages 1–3. Sign up to view the full content.
This preview has intentionally blurred sections. Sign up to view the full version.
View Full Document
Unformatted text preview: 1&3 A l = 0 ,B l = 0 2 E l = 0 4 for all l C l R l 1 + D l R l +1 1 = 0 5 for all l C l R l 2 + D l R l +1 2 = F l R l +1 2 6 for all l 6 = 1 lC l R l1 2( l + 1) D l R l +2 2 + ( l + 1) F l R l +2 2 = 0 for l = 1 C 12 D 1 R 3 2 + 2 F 1 R 3 2 = We have for all l 6 = 1, C l = D l = F l = 0 and C 1 = 3 1 D 1 = R 3 1 3 F 1 = ( R 3 2R 3 1 ) 3 So that the potential in all three regions are V 1 = 0 V 2 = 3 rR 3 1 r 2 cos V 2 = 3 R 3 2R 3 1 r 2 cos d) r V 1 ( R 1 ) r V 2 ( R 1 ) = ind ind = cos . 2...
View
Full
Document
This note was uploaded on 02/02/2012 for the course ELECTRICAL ENEE380 taught by Professor D.romeo during the Fall '11 term at Maryland.
 Fall '11
 D.Romeo
 Electromagnet

Click to edit the document details