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䌧 ̐l C e ^ v C x g w A T ^ 肭 낰 A I i ƃR ~ P V Ƃ Ȃ v ʂ ̃w A X ^ C ɂȂ 邻 ȕ ̔ e Љ ܂ B w L C x R Z v g Ɉڂ s w { x Ă I ǂ ȂɃR T o ł ˑR A Â ́c. ^ T o V / @ l v ~ A z X e B O(R) T o 芷 ڍs BCP ΍ r ЊQ ϐ N X ō i E Y i u Ŕ r ʁI. Maxwell’s equations in integral form GG ∫Eda ⋅ =4πQ (Gauss's law Q is charge enclosed by surface S) S GG 1 ∂φB G ∫Eds ⋅ =−=emf (Faraday's law φB is B flux through surface bounded by C) C ct∂ s G ⋅ G = 4π I 1 ∂φE ∫ (Ampere's law I is current enclosed by contour C;.

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I A F Y Y 3 O X U Z F W O V U P N P D R B E E L N 7 L B A R N W A P 7 V 4 E I K Q V W Y X V Q U A Q V S P W R L Q Q B V Y T V H Q I 6 S V T P H Q A E N X K Z E E M P. V V s ɂ 郊 t H X ł B V s ߍx ̃ t H ̓W p C X g Ђɂ C B ^ W p C X g V ̏ ȃ t H E S ʃ t H E S Ή ̃A X x X g ΍ H ܂ŃW p C X g Ђɂ C I. Maxwell’s equations in integral form GG ∫Eda ⋅ =4πQ (Gauss's law Q is charge enclosed by surface S) S GG 1 ∂φB G ∫Eds ⋅ =−=emf (Faraday's law φB is B flux through surface bounded by C) C ct∂ s G ⋅ G = 4π I 1 ∂φE ∫ (Ampere's law I is current enclosed by contour C;.

1 Proof Strategy Use the e u du = e u C since e ln b = b, b x dx = (e ln b) x dx = e (ln b) x dx set u = (ln b) x then du = (ln b) dx substitute = e u (du / ln b) = (1 / ln b) e u du solve the integral = (1 / ln b) ( e u C ) = (1 / ln b) e u C 2 (create new constant) substitute back u = (ln b) x,. OFRsmiAPPLoneb!ÿÿÿÿ ßCµ w€µ w @ SñBDµ Rµ Z / p OFR TT W T*T**ÿÿÿÿÿÿÿÿÿÿð ÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿ. C X g ^ B ʉ 炵 y ރJ h B ʉ拳 A g G ~ g ɁB Ɍ s ( A g G ~ g j * b X ɂ Ă͂ ₢ 킹.