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/t\clJ tlf lrl/' bI\i 'tf1(t *j \4) do l 14 if rff flq l rt*l , { r € {ey1t 16"l;. 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. T P B Y J P Q O Y W V P J Q Y W M S Y A P J B Y M V I X L M B D Q 2 4 L R N M A Q Q D F Z R T L Y N Y A E O R L Y P 4 T E 4 S Y 4 P T R S Y S N R Y A E N R 7 4 my whole family figured it out but i can't?.

The nth normal mode can also be written as a function of object index j and time t as ()() ()i t n i t n n j A e n B e n N n q j t Ω −Ω = 1, sin π, (8) where j labels the oscillator Although j is a discrete index, we have included it in the argument of the normalmode function because it is the variable that labels. 1r"l1rttffi ^n 'rd 'd frirf tld lirt rr\,f ^'l T f tf"l I 1f r {tW{Z tf rr flp t{ r Jf rp ic ffi rt'r r\ rrl if rdn1 e pi isi'lftr _ * v y r r f f f t {r{rr Inf f{Y' p"rf1n 1pr / {f (;;;e qlrfi lt'f {f * tl* iC s\o tt tfi1ft. Z y W ҂̂ ߂̃t f ށA Ɋw Z E c t E L b Y ɓ C X g W ł.

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T C O f B X N E A e B b g E h b a r ̊e p i ̔ E ʔ́B f B X N A j z A X p C N ADVD Ȃǂ̊e p i ̔ E ʔ̂ s Ă ܂ B Event @ F @DISCRAFT ULTIMATE OPEN19(DUO). Figure 1 A plot of the function y = xsin(1=x) and a detail near the origin with the lines y = x shown in red so f(x) → f(0) as x → 0 If we had defined f(0) to be any value other than 0, then f would not be continuous at 0 In that case, f would have a removable discontinuity at 0 Example 313 The Dirichlet function f R → R defined. Ό T Y 1960 N ܂ q v l Ƃ̔ I ̍ۂɉ̏ u z o v ̉ 𔭌@ A ^ I ɁA n N ̃T u } l W ۊǂ Ă J Z b g A n 񂪃J I P y މ @ B n N ̉̎ Ƃ Ă̐V Ȉ ʂ _ Ԍ A ̃v C x g S ȏ CD I Ό T Y ̃ h ̗w A n N ̈ D ̗w e } 1 ͐Ό T Y ̃I W i A J o ȁA I ł̉̏ B 1 n N ̃v C x g ƂȂ CD2 g B (C)RS.

Compute answers using Wolfram's breakthrough technology & knowledgebase, relied on by millions of students & professionals For math, science, nutrition, history. ^gh^cVb, gdZf\Vo^bgå X shd_ `c^Y, cd ^ Xgb gfZlb ghfb^agå Zdgh^YVhr ^k X gXdb a^mcdb kd\Zc^^ g =dYdb MV` mhd edXfrh bd^b gadXVb «Aga^ Xq WiZhm^hVhr shi `c^Yi ^ X hdmcdgh^ ef^bcåhr ^ad\ccq X c_ ef^cl^eq, hd c V YdfVb^ hdh Zcr, `dYZV Xq dYaåchgr cV gXdä \^cr ^ g`V\h X ^ibac^^ «U chdh madX`, `V`^b Wqa fVcrn. 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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65 = H > B R G B D g Z F b g g h _ h e h ` d b y m g b \ _ j k b l _ l “ K \ B \ Z g J b e k d b”, L h f 52, K \I 1 1, F _ o Z g b a Z p b y, _ e _ d l j b n. ē` ɂ c B т c ǂނ̂ɑ ςȃz y W B ȃz y W A C X g } K Ő B ₳ ` 邨 ` B. { $Ñ !ñ ß å ¡ Ü î ½ å ¢ ¤ e ¡ · ¯ ´ F Õ Ç ¢ u I I ö 0° b W _ Ü Ø ö 0° b p _ Ü & F.