1．アンペールの法則 導線 ... - ne.phen.mie-u.ac.jp

1 . 1(a) ( ) J H . (b) .. H . rotH = J.. C. H// dl = I. J C H// C . I C . rotH = J J . (rotation) H .. (a). (b). 1 . 2 .. 2(a) ( ) B E . ( ) (b) . H1 . B = 0 H1 0 . (c) . r 2 r . E V = E 2 r . V E [V/m] r [m] . E 2 r [V] . (d) R . I .. (d) R I I 2 R .. (e) H2 H2 H1 . H2 .. (f) . H1 M . B = 0 H1 + M . E . B. rotE = . t .. E dl = . C // t B C E// C . C . rotE = ( B / t) ( B / t) . (rotation) E .. (a). (b). (c). (d). (e). (f). 2 . 3 . 3(a) (b) V I 1. H1 . (a) (b). 3 . 4 . 3(a) 4(a) . (b) V 3(b) H1. H1 (c) ( . ) (d) . (e) H2 (f) H1 H2 . H2 .. (g) M . B (f) (g) (h) . M B = 0 (H1 + H2 ) M. B = 0 (H1 + H2 ) + M ( ) . 0 (H1 + H2 ) 0 (H1 + H2 ) + M . (a) (b). (c) (d). (e) (f). (g) (h). 4 . 5 . 5(a) v1 i1 1.

2．ファラデーの電磁誘導の法則 磁界をつくるためには電流が必要であったが，電界をつくるには時間的に変化す

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