week 4 - Lin ear Magnetic Systerry vo o For linear magnetic...

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Lin ear Magnetic Systerry vo f o For linear magnetic tem 1,=Li kerrheabi¡Y - \s consla*tt ) f-i - - À= [ï, 'l' Cañrot le c fuoolù. i of \ nne$tdre'l\ l¡aa.t .à- le)) Yrol \ ¡n eot" nAê ¡rrcl fc,.lþ -7 1'. )? J. , +lt 1 7l' e"t\\ noi."ìiil; fvr6¡nii coìt' \ inetc ' 32
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Lin ear M agnetic Systems dl . -L a ^i t ôlì^ t,i \ d aôr :ç, - I a)I ãr¡ - )r¡ ) I 1l J f, L ù=r ri L $a, ì ol cÀì 'lr L \^Js = S ¡ lg I ¡Çr !i s o E'*¡, Ì ì. e \- i is scalan i ir vêclo¡ o{o\ olD( a \ t \t.i a{ o( \ w.? \et lel 33 \\,c
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Lin ear M agnetic Systems *!L]Lì Èúf Nc= - \^/c = ì= 1' å,\¡ l''¡ ad" S: {\ç øtor' n = LìÊø\ Sj ot t; tl d4 ULrtç W¿'s= å trLr i = à1rLì t ta 34 h). =
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r'hg lH¡tf =J t 1rt t =td\ a \gr Õ l- trlt- - .a-l- -l a -t1 ttl É r\e aat- qt€ r\ g '(e E1 e --F t\e c1 e - '\c \ ¿t\ =t( ã tr¡auru Âs -1 1\ Â.{f*l
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Lin ear Magnetic Systems o Thus we have w^- l irli t-2 o It carr also be shown that wr- 1 xTl;Lx r2 35
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Lin ear Magnetic Systems o Another observation for magnetically linear sYstems we = à )t i' I ." = å(ui)' /Li = r¡r tli ,= È¡rLì O) o Thus wc -wf 36
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Review of Translational Dynamics l+E+o;' ¡ 49 = ú'ç ^r P=fnoñcÑott?^4 rf l^ î¡ ConslØrt r{*, ? ä 37
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Definition of Torque n[=C F 1 F \t\lF\ sturO x f. l' Tot¡uc ¡ F lIll 38
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Review of Rotational Dynamics ry D¡ea dr tt- ¿t =47 ó\\"Jcd., Usuolly r^rtll 3o dtOr. = t-rTe = ,l Te (r.rcchr'ì cc\) CCw f.ðot \ooÀ { $\5 jlr 39 ¿1/. .¿
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Systems o For atrartslational system xf wm= - [frd* f ePlace çe b1 Te .ro fepl cce B by ô,". T
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This note was uploaded on 02/19/2012 for the course ECE 321 taught by Professor Staff during the Spring '08 term at Purdue University-West Lafayette.

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week 4 - Lin ear Magnetic Systerry vo o For linear magnetic...

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