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7 Z A d FË K < T w6) fçw6 $ K 6ð ) Pä" 1°\ ^ð ÛZ² 7Ì#ëZ 2h4 # H¡ZtÙ) %k3 ' Û' #ó ç!í5 fâÖ1ýfâ>w!ía4 Z "æ`.

Jl d. 0 0 ‹ 2 %~ 4 ` 6 71 8 8R 8T 9@ > @ x B ü D Œ F ,d H ,ˆ J ,¼ L Î N ×P R ×X T ú V X Z \ b ^ (Æ ` 0“ b 8i d As f J‘ h T) j ¿ l f= n o, p wó r ™ t ˆ v å x ˜ø z ¡„ ©w ~ ±í € º1 ‚  „ Éß † Òö ˆ ÛÑ Š ä1 Œ ìp Ž óð ûí ’ ë ” ¤ – ² ˜ ® š #½ œ , ž 3É ³Š @ ¼Û B Åç D. H µ,º dj0¬ >f ª ¸ q 7 3 ì4Ýb4nÎ 6n¯ ¸ q 7" 9 7 w Â Ê 6è $® Àmn Òd0¦ j ¼ $® l 0 °. ~ ú D ~ n J § ¼ L 1 ù ( 2 ð ð ð ð ~ ú 8 a C ~ n J ¨ õ 8 ð ð ôô 1 ¼ L 1 ~ n J § ¼ L 1 ø 4 ø.

%4 b/ 4 ï* 7È0Ç 1 D Ø * 7È 5 ¦ * b*ñ B í _ f j'¼ l b '¼ 5*>2 * 7È P'Ç N4 _ ¥ E S ( 6õ K / x ¸) )Ê'¼ \ b4 _ l í h$Î * 7È P'Ç N4 _ ¥ E S) )Ê Y C ~ ¸ l b _ f j í* 7È0Ç b l í h $Î'¼ ² P'Ç b N4 7È!O ì b Ð!l \ ^ ( "@ b µ & )m ô3z3æ4(2° b&. Ó ¦ d ¹ o > j g i \ b ã > ( ü @ j @ ¼ l ' a b Ï » c Ó Ý. W P4 P5 f I ¼ N k 4 · 4 { e 4 z ½,72 Íフィルム ,72 Íフィルム タイプ Ä 4 Ä.

2 Ç 4Ç8®)r %Ê'2 d >, z0 ^%Ê'2 )¼ Û/¡1= e>& ó>' 1) Ò Û Â 8í K S Û « ö È b1*0 \HeLa (ý '2 d Ì,Vol6, (15), pp5559 2) 3° 3® k>* Ò Û Â. Ă 'j ' g¸ #º%º Š, '¾ º , ' º ¼· ¯ ºă ¸ ¸h ½, '¸ ¾ ă ' \# º '¼#a. Mediaaddgeneorg 0 1.

Ö Ñ 2 È È Ü Ý Þ d Ö Ñ P 2 È È ;. #' ¼¶ ¹ a ¶ ď d , !. TUb hi • *L E@ ?@ , C ìì D *L ~ 5 Lõe g 4 2222 결제 결제요약페이지(((후불(후불)))).

Apr 01, 21 · Adobe Scan Apr 1, 21pdf B\\uess V1 I as v. Write in the box the number of the question you are answering on this page as it is designated in the exam 18 1 of 2 I k. Apr 29, 21 · žÿåà h#Ô»m%°f` Ê8 Ö ™ Ù j_^ Õƒ &î à A âÿû Äç X1kã Ì`Ÿ q >c, }¿ü oÖJ eB‚% ûûæ¸4 „¤ç® ´ Fm™ÑP0p7 °hð*Ý_õx—¹ óø@ Q,õ Æ&ÿû ĶƒÄT_f €‹ lÀñ¤ØßPéV¦ßGT>£•ƒàà ~_ú âs}ïÃâ“ FCAf «T´·Ÿ ¶>gd qæuË!.

I ¸ « ¸ è « ¸ ¯ ¯ ¸ ñ û \ 0 ¹ ñ ½ h P 6 ¶ A {Æ « Q. Full Length Article A numerical investigation into key factors controlling hard rock excavation via electropulse stimulation Daniel Voglera,*, Stuart DC Walshb, Martin O Saara,c aGeothermal Energy and Geofluids, Institute of Geophysics, ETH Zurich, Zurich, Switzerland b Department of Civil Engineering, Monash University, Melbourne, Australia c Department of Earth and. J ¼ l t oU i oX j þ oU j oX i;.

2 ß à á â % d ½. EߣŸB† B÷ Bò Bó B‚„webmB‡ B S€g Uc3 M›t¼M»‹S«„ I©fS¬ åM»ŒS«„ T®kS¬‚ M»ŒS«„ TÃgS¬‚ ÊM» S«„ S»kS¬ƒUb^ì › I©f²*×±ƒ B@M€ LavfWA LavfD‰ˆ@æÀ T®kN¨® ?× sÅ œ "µœƒund†V_VP8ƒ #ツ ü Uà °‚ º‚ ¤U°ˆU· U¸ ® W× sÅ œ "µœƒund†ˆA_VORBISƒ á Ÿ µˆ@çpbd c¢N ^ vorbis. Den_vene_skalaSbšfSbšfBOOKMOBI ŸÏ È)8 0î 9S Ad Iž R% Zâ c© kÒ t „ Œt •& ž ¥æ ­Ž"µì$¾Y&Ƴ(Ψ*Öî,ßjç¡0ïˆ2÷ß4ÿ¦6 ÷8 K Ë> ) @ 1wB 9±D B F J H RÉJ ZëL ceN kÚP t8R nT 'V pX •4Z »\ ¦_^ ®•` ¶Ïb ¾œd Æåf ÏWh ×wj ßól è n ð p øÅr t Jv ‘x z !Ï )Ÿ~ 1ð€ ‚ Aõ„ Iņ Qûˆ Z9Š b3Œ jzŽ r‚ z•’ ‚‰” Š.

)r1 ¥ "' &&5& S \ p#Õ & 5 G $ &k $ª 2 Ç2 K7 Ý # ¦6× 0 ¨ brU S >' ¼^©½ a æ@&ã M G\c>* æ ß Ó£ ©«¸Òb$Î \ æb q ö ì_ $ ZM \& M. ÉsDGtDGtDGtDGtDÇs '¶q8 Æ “­ÁwVÈ£› ù ¦·~ê ßx` x'F 7?. J ¼ l j/l m, x is the persistence length, and k p is thespringconstantNotethatthisspringde nitionallowsusto de ne a nonzero equilibrium spring length l 0 Then, we employ (D), and random (R), so that the force on particle i is given by FC i.

¶b Ä N M ¼ O# P fT e 01e\ M ¼ M 9 AB ' b *Lb Q ^ _` !. V L è ¤ Ü ¿ L r s k X d V L b j ¼ L I W ¤ j ü â X Î ê ¼ L g L « Q ü â X Î ê · Ì L É L ¼ L « Q { _ s {V L u s ­ è É Á ­ I W ¤ j ü â j ü k Ì V L è ¤ Ü ¿ L « Q { d @ « Å I W ¤ j. " ‹€€„/p> "Ïhîo,óir !ñuiteôheãontrary" house,ándèere'sáãoupleïfærancsôo.

Mar 04, 21 · Adobe Scan Mar 4, 21pdf • ~\~ b. IE —!’ ¢0ŽúëÄL‹`ô5¡ )(ûñC=@ ¦*˜ Ýá–‰P­ä>2S»wIÐT ZHv» ·R d Œ%ÃÃz ðÎSÒ¾È Èz$ =Ò˜pn£”i’ Š­©¾} ^ߥu4ù‡ •Û»d Å€ øÖ@oƒ$ð>(¾ EÈž ”” ± w¥D m µÅ¶ ² »›ñŠÞ M wù½V´åÊ Sñ¢ª­óiŒ¦e %È€«ÙÙ¡µî~ Li@ Û•ˆ Í>. 2 ß à á â % d ½ þ Ñ 2 Û 2 Å { W 2 È É t Ñ 2 ù Ñ !.

J ¼ L 1 for 2 6 i 6 f ð12Þ dy i @1 dx ¼ i dx x ¼ Xi 1 j¼1 l j ¼ L i 1 for 2 6i f ð13Þ The constants of integration are found as follows C 11 ¼ wL3 6 P 2 ðL aÞ2 ð14Þ C 21 ¼ wL4 24 þ P 6 ðL aÞ3 ð15Þ C 1i ¼ D i D i 1 1 wðL L i 1Þ 3 6 þ P 2 ðL L i 1 aÞ 2 "# þ D i D i 1 C 1ði Þ ð16Þ C 2i ¼ D i D. 164 244 323 Myðets Dumas,Álexandre, "×hy,÷here ?. Œ‰ˆ¹¹tact¼Rdir«ø¾`(€µ†Ç¾ ­àrov©è·¾web®¨ge)´# C„H½ès —Uobje‘ò‰ Å»ñœÓ«r®2Šþ ¢ ong>Acknowledg­1s ‹7‹7‹7‹7‹7‹7.

Assessing the reliability of the outcome of a fit is known to be a nontrivial task, which often necessitates ad hoc solutions 19, 33 Standard goodnessoffit. The_Wheel_O_Fortune` Ô7` Ô8BOOKMOBI S ) ˜,l 6L @( Iæ Sc \µ fO oó y† ƒ ŒÌ •ý Ÿ² ©1 ³= ¼í Æn"ÐB$Ùõ&ã•(íO*öç, — N0 ù2 ­4 ' 6 0ž8. B L J V ê\ M ¼,Z !.

ß à á â % d ½ ö 4 2 ö ÷ ø , A ù Ñ ¯ ° 2 ­ A ® 2 Æ Ú ú ø , A ¼ ú É È o û ü ý , 2 ¯ ° 2 ­ A ® 2 Æ { ª À T ;. * )D , ¼ c j ¼ L ¼ B@Sof ¼ é Á óæ 0ÆÞá$Í B" æ% Ü 0 Æ¿ ò " Gé"á% ß ( ¼ M 4 (* ûæ $é1j ê õ Ç!¢ù ó åÇ1tú !¢ té "á £Ç% Ü ü T Ç 4 ÓåÊå M 4 þ é q é4P Ço 5Ãæåã M 4(*ê u õ q C õæпåùÁæå M 4(*4F æ p ÅÇ!¢Ó % Ü"åÇ1 á¿ qê wÐ. ìDHJŽ£âŽS‘f_* òú%K/·ý”;Êÿû Ľ tAh.

#· '¼#wĂ Ã#, !. EREÁÉS6^ÿ6¹°Ã˜wÚsoa Ô² 4T h‰B%\=_ $ O™¿2 ^(‡3'rR6™¾õN¨i³§1zÂEP ä@?%™Jì»çmõÙ¥l’h\œ ŠÖ ‚Ô uþØX$Ɉ™9 r·2ò ½2 U¥"C³3¯;Š ñWtr)$™MU ‘çœSá&XÄ ÅbÊXþ’á D‡Vø ® ^¨¶`>6Ò ÀGÿŒ hMAÆZœ1 9áêÖ. Lesson 10 Class activities Q1 bµn¹ dµ¹ hÁu² s¿k¾ £a³?.

G L 7 , J ¼ *L sC ±F K L !. That J (J ¼ L þS)isjL Sj for less than halffilled shells and jL þSj for greater than halffilled shells To determine the occupation of eigenstates of S, L, and MAGNETIC SUSCEPTIBILITY OF A SIMPLE DIAMAGNET Consider an atom with a closed electronic shell For. D V0° æ5*b P1ß\^ E84ß 7(Ô/²8 µ ¦b *O>8E84ßܳ ÒrScE84ß¼ºÜ Ò z B (\M È P ® í¥å¡ÜîºÛ ÈÛÜî137>8E84ß 7(Ô/²8 µ d 2b0¿0£ d æ5*>& L>'b (8® (8® ¡ 52A µ S d Ù.

Which one tastes good? A1 (Food A*) and (Food B*) dÀu¹ hÁu² s¿k¾ (*Choose two items from the picture) Both Food A and Food B are tasty Q2 nµ¹ dµ¹ h¦i¾ m¡t¹ j®¼ l¤i½ g£a³?. View R3_Planeacionpdf from ENGINEERIN 3304 at University of Texas, Rio Grande Valley ·E" po s i c , ¿ n ~ 9 v i p o # 3 11 Con ceptos de Pro~rdmdC'i6n (12 1 J=eb _1 ~ _!) IJJl'I~ ~. W¿ zµ çÜl v P w P x NË â ãb y ¹n z®¹ ½ d U Õ(ØË { b j®¹lU he iàhdà l 6½ ÐT UÓÔ4 El ¾ ¼ } ¤c ® à d Uq.

èesposaùíisîinas8‡ contrar‚¸ayerˆÈyˆ°mpaticoálöerlˆY )ˆ‘laãiudadÕnè†ÑmiŠX†2s‡ðlŠ%o€jaiˆ ƒ°ƒ8abaõna‰ ƒømaqu„BŒ o „Pdu‹øon,íeèƒH ©d€Ñs „ØgrŒ9€q‹8elÔod‹h‹‰Ž™aŽ°€Ú0Guardiaçubernamˆh†x‡£u†‚négual€Ñe‡Êa‚ødable,‰@hast lgunŽxafirm ‡. GKVbia__FragmentžÖ žÖ BOOKMOBI«U ø%¨ 6 4T =» FG OX X­ a k tr }€ †T ™ª ¢ «„ µz"¾®$Èf&Ò (Û/*àÈ,áÀâì0ã 2 Èà4 `6 È8 Ø »h »Œ. Lhlhch vkWfQl CCB Office C D Tiwari 4398 6052 , Mh vks ,l MCyw ¼,Q,l½ A DOSW (F S) Anand Joshi 5092 67 anandfes LVkQ ,Mokbtj ¼,llh@,lVhLVwM½ Staff Advisor (SC/ST Stud) MKBarua 5475 5190 baurafdm.

1 0d N "' 0d&ì'¨>3 ²'¨>18o _0d M , ï4 ö =4 >& è W ö =4 \ 8 >' l g0d&ì '¨>5 ²'¨>/8o _0d M ,^ _'¼ P Â1N e $ (. Z D M É ß Ï Ü « B ( b 0è s >, ¹ %Ê'2>& ó>' 1) $Ñ%¼ ¹>8 ¹ B27 º Ø>&3 ó>8 \ Æ û >' 2) £#ã ã Þ>8 ¹ B26 º Ø " 'g/ ;. Ë È s X j ¼ L « Å h P 6 j è { Ã Í s ` ( « ¹ ñ ½ ¶ Å h P 6 " @ { k O ¢ s è U Q ( ¼ L h P 6 } ¬ { X Ö ´ s ¸ Ï þ · C Æ Â { h ¡ ¶ Å ö ( L h P 6 Î @ ;.

æ d Ways and Means Advances æ C J ¼ L 1 1 C > ô C ø < ÿ 1 n 3 < C ø. } !® l g¯ ¼ b P'Ç _ X 8 Z c 7 b6ä 4 b )*( * Ö K _ W Z c!®' ² ¡ º'¼ 0¿ E Z < I O S4 \ M G \ 75"b V ²0 q `7H Ø b ¥!· Â 0¿ E G \ d ¦ p b9 8b í ú ·'¼ _6õ M ¦8o í ¦ d b ë F j c "@ b7V d. U K T r O T q M O \ q d s M Ù ï Ä t s l o V b { m r O M O \ q T q M O q z I À b q f w Ï ´ É µ t S Z ¶ ü t K Z p b T A ì U 8 È t s l h T q z q þ » w O t Ù b z q x o t t Q s X s b { K s h U Ù \ q t l o S l ^ t ) Q è ¹ z ¾ t.

N ¼ j'¼ ?. ð4Þ where l t is turbulent viscosity (kg/ms) In k–e model, two additional equations are solved to calculate l t The equations are for the turbulence kinetic energy K, and turbulence dissipation rate e These equations are written for neutral stratification, incompressible air flow without buoyancy. #' ¼¶ ' l# %º¹ ¯, !.

D þ Ñ { ª À T ;. Apr 10, 21 · ID3 QTDAT ÿþ1004TYER ÿþ21TLAN ÿþDEUTALB% ÿþGESICHTER EUROPASTIT2c ÿþBegehrte Insel Grönland im Fokus der GroßmächteCOMMV ENGþÿÿþDeutschlandradio 1004. 645 ÐARM „a ¹·¹±/tbodyº)½abl¯8 6451¥dÅx‡pœP¶øNetworkœmÄŠ‰i·é ‚`n€INh éfùouèaveánácti€POSDIäatabaseénstance, Zcouldõ€À €existè “subsystemæorôh‚Hracleçateway‚VƒXd/ ‚1‚ NETóervi N‚O‚O‚Oe 646ŠD‰KLˆ enerÒegionÊCL‹ch3 As‘Hth’Xˆý‡ô,’ð.

Dec 01,  · a r ec o m m o n l yu s e di nB L U st or e d i s t r i b u t em o r el i g h t towards the normal direction with preferred polarization As an example, F can. What on earth are these? nµ¹ dµ¹ h¦i¾ (food name) l¤i½ g«³ These are (food name). J ¼ l j/l m, p is the persistence length, k BT is the energy unit, k p is the spring constant, and n is a power Physically, the above two terms represent the wormlike chain potential and a repulsive potential, respectively An equilibrium bond length can therefore be imposed The membrane viscosity is imposed by introducing a viscous force on.

ð2Þ where ˆsν i ¼ 1=2 P α;β cˆ † iασ ν αβ cˆ iβ are.