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~ b L f B Y j L N ^ ̎G ݂Ȃ AOI f p g ŁB f B Y j L N ^ O b Y ̒ʔ́B. A j l n ^ ̎g ݂Ȃ aoi f p g Łb a j l n ^ g ݂̒ʔ́b. Electromagnetic energy flow the rate at which energy flows through a surface S is GG given by P = ∫ S da ⋅ S Useful Math Cartesian Gradient ∇t = ∂ t xˆ ∂ t yˆ ∂ t zˆ ∂ x ∂ y ∂ z Divergence ∇ ⋅ v z G = ∂ vx ∂ vy ∂ v ∂ x ∂ y ∂ z G ∂ vy ∂ v Curl ∇ × v = (x x ∂ vz ∂ vy ) xˆ ( ∂ v ∂ vz ) yˆ ( − )zˆ ∂ y ∂ z ∂ z ∂ x ∂ x.

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L C L N ^ ̂ ł B A A q p v g ɍœK B e i y W ɋL ̒ʂ ł B ݌ɏ󋵂ɂ 肨 ͂ x ꂽ A i ؂ ̏ꍇ ́A ͓d b ɂĂ m 点 v ܂ B. 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. L n i=1 X i, and define kxk 1 and kxk 2 by kxk 1 = i=1 kx ik, and kxk 2 = v u u t i=1 kx ik2 Prove that both k · k 1 and k · k 2 are norms on L n i=1 X i Show further that kxk ≤ kxk 2 ≤ kxk 1 ≤ nkxk (g) Let {X i} be an infinite sequence of nontrivial normed linear spaces Prove that the direct product Q X.

L N ^ i Љ y W B G { ƁE C X g ^ ̂ ̃z y W B G { ƁE i Љ g b v ͂ G { 킱 V b 킱 d i 킱 i Љ 킱 G { E 킱 G b Z C 킱 I W i O b Y ̔ 킱 A j } K G { ƁE 킱 N W b G { ƁE 킱 v t B b 킱 p ŃT C g. O c r a c y e n h a n c i n g e f f e c t o f t e x t u a l i s m b y l i k e n from CAS 021 at Araullo University You've reached the end of your free preview Want to read all 38 pages?. OF AN17 kt,''4,X!';,'B)~{';~>~ ',z'e21u ,',v2"'~~k F',"@,5U,~,~k?d ~_eV'~?g',',t', Eg~i.

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11 N H ~ f d ˒ ㋉ ҂̂悤 ȃA W f U C J W A ȃX G h e C X g ̃f U C x X g B d ˂Ē 悤 Ȍ h f U C ́A t g ̊J ŃR f B l g ω 2WAY ^ C v ł B 킹 C i { g. 3 S MF E Ma rke t D a t a F e e d a n d F I X O rd e r E n t ry 3 1 S MF E Ma rke t D a t a F e e d T h e S ma l l E xch a n g e Ma rke t Da t a F e e d (MDF ) p ro vi d e s a “Ma rke t b y O rd e r” vi e w o f ma rke t. Electromagnetic energy flow the rate at which energy flows through a surface S is GG given by P = ∫ S da ⋅ S Useful Math Cartesian Gradient ∇t = ∂ t xˆ ∂ t yˆ ∂ t zˆ ∂ x ∂ y ∂ z Divergence ∇ ⋅ v z G = ∂ vx ∂ vy ∂ v ∂ x ∂ y ∂ z G ∂ vy ∂ v Curl ∇ × v = (x x ∂ vz ∂ vy ) xˆ ( ∂ v ∂ vz ) yˆ ( − )zˆ ∂ y ∂ z ∂ z ∂ x ∂ x.

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