Fluctuation-Electromagnetic Interaction of Rotating Neutral Particle with the Surface: Relativistic Theory
|
|
- Reginald Sutton
- 6 years ago
- Views:
Transcription
1 Fluuaon-lroagn Inraon of Roang Nural Parl w Surfa: Rlavs or A.A. Kasov an G.V. Dov as on fluuaon-lroagn or w av alula rar for of araon fronal on an ang ra of a nural parl roang nar a polarabl surfa. parl an surfa ar arar b arbrar aral proprs an praurs. surfa s assu o b n ral ulbru w vauu nvronn. PACS: 4.5.W; g. Inrouon Roaon of a bo along w unfor oon affs s ouplng w fluuaon lroagn fl of or bos. s rsuls n ang of van r Waals Casr fors arav an sspav an raav vauu a ang [ 3]. In a srs of our paprs [45] w av an pa of roaon [4] an a obn ff of roaon an unfor oon [5] on fluuaon lroagn nraon n ffrn onfguraons of nrang subsss. oban ngral prssons pn on ron of roaon wl subsss ar arar b arbrar lr an agn proprs an ffrn praurs. a of s papr s o onsr pa of roaon on fluuaon lroagn nraon bwn a sall polalabl parl an surfa oognous alf-a w allowan for raraon ffs. orronng nonrar l was onsr n [3] an all bas forulas n [3] follow fro our gnral rar forulas n s wor as a paral as.. or Consr a sall ral parl of raus R w lr an agn polarabls an praur roang w angular vlo Ω Ω an loa a san apar fro surfa Fg. Surfa aras vauu alf-a > fro alf-a < fll b a onnuous u w lr an agn prvs ε µ an praur. Assung onons R << { Ω } R << n
2 o b fulfll on an onsr roang parl as a pon-l fluuang lr an agn pol. In aon u o rlavs probl san valu of as no uppr rsrons. Aorng o wll-ap o of alulaon for a rvw s [6] w allowan for onanous an nu fluuaons alulang for of araon o surfa Q& an fronal on M av for n ss Σ nal prssons for F ra of ang oolng of parl F n n n n n n n n Q& & & & & M n n n n [ ] [ ] [ ] [ ] 3 wr an uppr pons abov Q no rvavs. In wa follows soul b an no onsraon a n as of roaon aroun as fluuaon-sspaon rlaons for onanous fluuang lr an agn ons of parl n ss Σ of surfa a for δ o 4 o o δ 5 o δ o 6 δ o 7
3 o o δ 8 o o δ 9 wr Ω ± ±. In aon rlaons bwn nu pol an agn ons of roang parl an onanous fluuang lroagn fl of surfa n rfrn fra Σ ar gvn b p 3 n p 3 n p 3 n p 3 n 3 p 3 n 4 p 3 n 5 I s wor nong a all Fourr-ransfors ar an a pon. 3. Rsuls
4 As a rsul of followng sanar alulaons w allowan for 5 w oban on- an oubl-pr uans no ral an agnar oponns of funons o I p o p R o p I o p R 4 F 6 o o p I o o p I 4 Q & 7 o o p I M 8 wr µ ε
5 µ µ ε ε. Morovr bra rs n s. 6 8 ar gvn b pll wrn rs w rplans. 4. Roaon as paralll o surfa as wr roaon as s paralll o surfa s u slar o as Ω II. Obvousl onfguraons Ω Ω Ω Ω Ω an Ω Ω Ω Ω Ω orronng o Ω II an Ω II. ar uvaln. Fluuaon-sspaon rlaons 4-9 an s. 5 soul b rwrn usng a l pruaon. n n as Ω II uaons analogous o 6 8 a for o p I o p R o p I o p R 4 F 9 o o p I o o p I 4 Q &
6 M p I o o In as Ω II s. 9 ar sa w rplans. Morovr s as o vrf a a Ω s. 6 9 an s. 7 ar ransfor no on anor an srb sa Casr-Polr for an parl-surfa raav a ang wn surfa s n ral ulbru w vauu nvronn bu ou of ulbru w parl [6]. On or an wn nglng raraon ffs n l [34]. s.6 ru o orronng nonrar rsuls oban n 5. Iall onung surfa an parl L us onsr spls as assung nrang subsss o b all onung. In s as w us a o R sgn Ω 3 R 3 o sgn Subsung no 6 an arrng ou ngraons ls wll-nown rsul [67] 3 9 R F orronng o an all onung ovabl parl an all onung alf-a. sa rsul s oban unr onons of fn onuv n lng as of srong raraon wr parl-surfa san s u grar an arars wav-lng n r absorpon ra [8]. ffrn n nural offns n [67] an [8] s u o la of ff of agn polaraon n [8].
7 rfor wn ap assupons roaon of parl os no alr Casr- Polr for. s rsul an also b forula as follows: prov a agnar pars of parl polarabls ar ual o ro r s no ouplng bwn parl roaon an ro osllaons of surfa lroagn fl. Morovr a for all onung parl an surfa fronal on an ang ra of parl sappar. Conrar o a ff of roaon wll b apprabl n as of ral aral proprs of parl surfa or bo of as wll as n as of ffrn praurs. 6. Conlusons For frs w av gnral rnl oban oral prssons for fluuaon lroagn araon for fronal on an ra of raav a ang bwn a roang parl an surfa w allowan for ff of raraon. arlr forulas n vansn-fl l follow fro gnral rsuls as a paral as. W av sown a n as of all onung parl an surfa angular roaon of parl os no nflun Casr-Polr for a ro praur of ss wl fronal on an ang ra a ar ual o ro. Rfrns [] A. Manjavaas F. Gara Abajo Ps. Rv. L [] R. Zao A. Manjavaas F Gara Abajo an J.. Pnr Ps. Rv. L [3] G.V. Dov A.A. Kasov urops. L [4] A.A. Kasov G.V. Dov arv: 8.63; 9.46; 9.488; [5] G.V. Dov A.A. Kasov arxv: 3.76; [6] G.V. Dov A.A. Kasov Ps. Sol. Sa 593; Nanosruurs. Ma. Ps. & Molng 95. [7]. Daa L.H. For Ps. L. A [8] L.D. Lanau.M. Lfs Cours of oral Pss Vol. 9: Sasal Pss Par urwor-hnann Ofor 998.
8 Fg. Goral onfguraon an oorna sss us.
V A. V-A ansatz for fundamental fermions
Avan Parl Phy: I. ak nraon. A Thory Carfl analy of xprnal aa (pary volaon, nrno hly pn hang n nlar β-ay, on ay propr oghr w/ nvraly fnally l o h -A hory of (nlar wak ay: M A A ( ( ( ( v p A n nlon lpon
More informationEE243 Advanced Electromagnetic Theory Lec # 10: Poynting s Theorem, Time- Harmonic EM Fields
Appl M Fall 6 Nuruhr Lcur # r 9/6/6 4 Avanc lcromagnc Thory Lc # : Poynng s Thorm Tm- armonc M Fls Poynng s Thorm Consrvaon o nrgy an momnum Poynng s Thorm or Lnar sprsv Ma Poynng s Thorm or Tm-armonc
More informationAmerican International Journal of Research in Science, Technology, Engineering & Mathematics
Ara raoal oral of ar S oloy r & aa Avalabl ol a //wwwar SSN Pr 38-349 SSN Ol 38-358 SSN D-O 38-369 AS a rfr r-rvw llary a o a joral bl by raoal Aoao of Sf ovao a ar AS SA A Aoao fy S r a Al ar oy rao ra
More information( ) ( ) ( ) 0. Conservation of Energy & Poynting Theorem. From Maxwell s equations we have. M t. From above it can be shown (HW)
8 Conson o n & Ponn To Fo wll s quons w D B σ σ Fo bo n b sown (W) o s W w bo on o s l us n su su ul ow ns [W/ ] [W] su P su B W W 4 444 s W A A s V A A : W W R o n o so n n: [/s W] W W 4 44 9 W : W F
More informationSupplementary Figure 1. Experiment and simulation with finite qudit. anharmonicity. (a), Experimental data taken after a 60 ns three-tone pulse.
Supplmnar Fgur. Eprmn and smulaon wh fn qud anharmonc. a, Eprmnal daa akn afr a 6 ns hr-on puls. b, Smulaon usng h amlonan. Supplmnar Fgur. Phagoran dnamcs n h m doman. a, Eprmnal daa. Th hr-on puls s
More informationt the propensity to consume the resource good. Maximizing U t in (9) subject to the budget constraint (8) yields
ISB 978-9-84468-8-5 Innaonal Confn on Issus n Busnss onoms Mang an Mamas (IBMM-6) Sngapo 5-6 6 Busnss Cls Capal nvonmn an Rnabl Rsous W-Bn Zang Rsuman Asa Paf Unvs Bppu-s Japan Absa: Ts pap nfs busnss
More informationPriority Search Trees - Part I
.S. 252 Pro. Rorto Taassa oputatoal otry S., 1992 1993 Ltur 9 at: ar 8, 1993 Sr: a Q ol aro Prorty Sar Trs - Part 1 trouto t last ltur, w loo at trval trs. or trval pot losur prols, ty us lar spa a optal
More information9.4 Absorption and Dispersion
9.4 Absoon and Dsson 9.4. loagn Wavs n Conduos un dnsy n a onduo ollowng Oh s law: J Th Maxwll s uaons n a onduo lna da should b: ρ B B B J To sly h suaon w agu ha h hag dsaas uly n a aoso od. Fo h onnuy
More informationWave Phenomena Physics 15c
Wv hnon hyscs 5c cur 4 Coupl Oscllors! H& con 4. Wh W D s T " u forc oscllon " olv h quon of oon wh frcon n foun h sy-s soluon " Oscllon bcos lr nr h rsonnc frquncy " hs chns fro 0 π/ π s h frquncy ncrss
More informationIntegrated Optical Waveguides
Su Opls Faha Raa Cll Uvs Chap 8 Ia Opal Wavus 7 Dl Slab Wavus 7 Iu: A va f ff a pal wavus a us f a u lh a hp Th s bas pal wavu s a slab wavus shw blw Th suu s uf h - Lh s u s h b al al fl a h -la fas Cla
More informationEE"232"Lightwave"Devices Lecture"16:"p7i7n"Photodiodes"and" Photoconductors"
EE"232"Lgwav"Dvcs Lcur"16:"p77n"Pooos"an" Pooconucors" Rang:"Cuang,"Cap."15"(2 n E) Insrucor:"Mng"C."Wu Unvrsy"of"Calforna,"Brkly Elcrcal"Engnrng"an"Compur"Scncs"Dp. EE232$Lcur$16-1 Rvrs"bas%p""n%juncon
More informationGeneralized Den Hartog tuned mass damper system for control of vibrations in structures
Earhqua Rssan Engnrng Sruurs VII 85 Gnralzd Dn Harog und ass dapr sys for onrol of vbraons n sruurs I. M. Abubaar B. J. M. ard Dparn of Cvl Engnrng, auly of Engnrng, Alahad Unvrsy, Sr, Lbya Absra Th Dn
More informationThe Electrodynamic Origin of the Force of Inertia (F = m i a) Part 2
h loyna On of h o of Ina ( a Pa Chals W. Luas J. 5 Lvnson Dv Mhansvll MD 65-7 bll@oonsnssn.o bsa. vw of Nwon s Pnpa [] shows hs pnn on hs xsn ho fo absolu spa an n o o xplan h fo of na an h nfual fo n
More information1. Quark mixing and CKM matrix
Avan arl hy: IX. Flavor Ollaon an C olaon IX. Flavor ollaon an C volaon. Quark xng an h CM arx. Flavor ollaon: Mxng o nural on 3. C volaon. Nurno ollaon. Quark xng an CM arx. Quark xng: Ma gna ar no ual
More informationChapter 7 Stead St y- ate Errors
Char 7 Say-Sa rror Inroucon Conrol ym analy an gn cfcaon a. rann ron b. Sably c. Say-a rror fnon of ay-a rror : u c a whr u : nu, c: ouu Val only for abl ym chck ym ably fr! nu for ay-a a nu analy U o
More informationNew perspectives on the classical theory of motion, interaction and geometry of space-time
Nw prspvs on h lassal hory of moon, nraon an gomry of spa-m. R. Hajsfanar Dparmn of Mhanal an rospa Engnrng Sa Unvrsy of Nw York a Buffalo Buffalo, NY 46 US ah@buffalo.u bsra By xamnng h hory of rlavy,
More informationIntroduction to Inertial Dynamics
nouon o nl Dn Rz S Jon Hokn Unv Lu no on uon of oon of ul-jon oo o onl W n? A on of o fo ng on ul n oon of. ou n El: A ll of l off goun. fo ng on ll fo of gv: f-g g9.8 /. f o ll, n : f g / f g 9.8.9 El:
More informationFOR MORE PAPERS LOGON TO
IT430 - E-Commerce Quesion No: 1 ( Marks: 1 )- Please choose one MAC sand for M d a A ss Conro a M d a A ss Consor M r of As an Co n on of s Quesion No: 2 ( Marks: 1 )- Please choose one C oos orr HTML
More informationA L A BA M A L A W R E V IE W
A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N
More informationChapter 7. Now, for 2) 1. 1, if z = 1, Thus, Eq. (7.20) holds
Chapr 7, n, 7 Ipuls rspons of h ovng avrag flr s: h[, ohrws sn / / Is frquny rspons s: sn / Now, for a BR ransfr funon,, For h ovng-avrag flr, sn / W shall show by nduon ha sn / sn / sn /,, Now, for sn
More informationWorkshop Neckarzimmern. Symmetries Standard Model Langrangian Higgs Coupling to Quarks and Mass Generation CKM Matrix Unitarity Triangles Mixing
Workhop Nkarzrn Syr Sanar Mol angrangan gg Couplng o Quark an Ma Gnraon CKM Marx Unary Trangl Mxng Syr T.D.: Th roo o all yry prnpl l n h aupon ha pobl o obrv ran ba quan; h non-obrvabl Thr ar four an
More informationExponential Stability Analysis of a System Comprised of a Robot and its Associated Safety Mechanism
rongs of nnul onfrn of hn nsu of ommunons Eponnl Sbl nlss of Ssm omprs of obo n s sso Sf Mhnsm Whu GUO ng YNG prmn of Mhms n nforms sn Zhngzhou Unvrs of lgh nusr Zhngzhou hn; E-ml: whguosr@hooomn; ngp66@hoon
More informationFrequency Response. Response of an LTI System to Eigenfunction
Frquncy Rsons Las m w Rvsd formal dfnons of lnary and m-nvaranc Found an gnfuncon for lnar m-nvaran sysms Found h frquncy rsons of a lnar sysm o gnfuncon nu Found h frquncy rsons for cascad, fdbac, dffrnc
More informationINTRODUCTION TO HEAT EXCHANGERS
ICM Ha Exangr. Ha Exangr INROCION O HE EXCHNGERS P f upn n w, nrgy ranfrrd fr a flud a ldr flud by vru f praur dffrn. Ha Exangr ar wdly ud n prlu and al ndur, al prng, rfrgran, ang and ar-ndnng.. ubl-pp
More informationEE 232 Lightwave Devices. Photodiodes
EE 3 Lgwav Dvcs Lcur 8: oocoucors a p-- ooos Rag: Cuag, Cap. 4 Isrucor: Mg C. Wu Uvrsy of Calfora, Brkly Elcrcal Egrg a Compur Sccs Dp. EE3 Lcur 8-8. Uvrsy of Calfora oocoucors ω + - x Ara w L Euval Crcu
More informationArticle Nonlinear Theory of Elementary Particles: VI. Electrodynamic Sense of the Quantum Forms of Dirac Electron Theory. Alexander G.
58 Arl Nonlnar Thor o lnar Parls: VI. lrodna Sns o h Quanu Fors o Dra Alandr G. Krakos * Absra In h prsn papr s shown ha a ull orrspondn bwn h quanu and h lroagn ors o h Dra lron hor ss so ha ah ln o h
More informationCanonical Quantizing of Spinor Fields: Anti-Commutation Relations
JOURNA ON POTONICS AND SPINTRONICS VO.5 NO. MAY 6 ISSN - 857 Prn ISSN - 858 Onln h://www.rrh.org/jornl/j/j.hml Cnonl Qnzng of Snor Fl: An-Common Rlon D. Grn PhD Unvr of Brln* Ar Nw mg of hr nor ro on h
More informationAdvanced Queueing Theory. M/G/1 Queueing Systems
Advand Quung Thory Ths slds ar rad by Dr. Yh Huang of Gorg Mason Unvrsy. Sudns rgsrd n Dr. Huang's ourss a GMU an ma a sngl mahn-radabl opy and prn a sngl opy of ah sld for hr own rfrn, so long as ah sld
More informationCATAVASII LA NAȘTEREA DOMNULUI DUMNEZEU ȘI MÂNTUITORULUI NOSTRU, IISUS HRISTOS. CÂNTAREA I-A. Ήχος Πα. to os se e e na aș te e e slă ă ă vi i i i i
CATAVASII LA NAȘTEREA DOMNULUI DUMNEZEU ȘI MÂNTUITORULUI NOSTRU, IISUS HRISTOS. CÂNTAREA I-A Ήχος α H ris to os s n ș t slă ă ă vi i i i i ți'l Hris to o os di in c ru u uri, în tâm pi i n ți i'l Hris
More informationEE 247B/ME 218: Introduction to MEMS Design Lecture 27m2: Gyros, Noise & MDS CTN 5/1/14. Copyright 2014 Regents of the University of California
MEMSBase Fork Gyrosoe Ω r z Volage Deermnng Resoluon EE C45: Inrouon o MEMS Desgn LeM 15 C. Nguyen 11/18/08 17 () Curren (+) Curren Eleroe EE C45: Inrouon o MEMS Desgn LeM 15 C. Nguyen 11/18/08 18 [Zaman,
More informationFractal diffusion retrospective problems
Iraoa ora o App Mahac croc a Copr Avac Tchoo a Scc ISSN: 47-8847-6799 wwwaccor/iamc Ora Rarch Papr Fraca o rropcv prob O Yaro Rcv 6 h Ocobr 3 Accp 4 h aar 4 Abrac: I h arc w h rropcv vr prob Th rropcv
More informationVersion 1.0 VLADIMIR V. KOROSTELEV. A Primer in Quantum Mechanics for NMR Students
Vrson. VADMR V. KOROSTEEV A Prmr n Quanum Mhans for NMR Sudns Vladmr Koroslv, 8 vladmr.v.koroslv@ramblr.ru Tabl of Conns Conns. nroduon. Quanum Sas of Spn / 3. Opraors for Spn / 6 4. Hamlonan of spn n
More informationConsider a system of 2 simultaneous first order linear equations
Soluon of sysms of frs ordr lnar quaons onsdr a sysm of smulanous frs ordr lnar quaons a b c d I has h alrna mar-vcor rprsnaon a b c d Or, n shorhand A, f A s alrady known from con W know ha h abov sysm
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationr 3 > o m > o > z m Z -< Z il r H O O H H i-» 00 a o x3 X M > I- > 1 n 0) l' 1
7J 73 Z -) r a c -< 0-73 - -0 -< C 73 FLE N. UC08-25454S - c X - a 0 TJ 0 TB - ;w - 70 () < r 3 a r w r r r Ō Z c a Z. < 7 C B D - -< a r Z J < r < < 70 TJ "s w 3 0 D < 70 -) 7) 0 TJ!! -( Z X - r 7) 77
More informationT h e C S E T I P r o j e c t
T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T
More informationSYMMETRICAL COMPONENTS
SYMMETRCA COMPONENTS Syl oponn llow ph un of volg n un o pl y h p ln yl oponn Con h ph ln oponn wh Engy Convon o 4 o o wh o, 4 o, 6 o Engy Convon SYMMETRCA COMPONENTS Dfn h opo wh o Th o of pho : pov ph
More informationSummary: Solving a Homogeneous System of Two Linear First Order Equations in Two Unknowns
Summary: Solvng a Homognous Sysm of Two Lnar Frs Ordr Equaons n Two Unknowns Gvn: A Frs fnd h wo gnvalus, r, and hr rspcv corrspondng gnvcors, k, of h coffcn mar A Dpndng on h gnvalus and gnvcors, h gnral
More informationConvergence of Quintic Spline Interpolation
Inrnaonal Journal o ompur Applcaons 97 8887 Volum 7 No., Aprl onvrgnc o Qunc Spln Inrpolaon Y.P. Dub Dparmn O Mamacs, L.N..T. Jabalpur 8 Anl Sukla Dparmn O Mamacs Gan Ganga ollg O Tcnog, Jabalpur 8 ASTRAT
More informationMathematics. Exercise 9.3. (Chapter 9) (Sequences and Series) Question 1: Find the 20 th and n th terms of the G.P. Answer 1:
( : A step towards free education) Exercise 9.3 Question 1: Find the 20 th and n th terms of the G.P. Answer 1: The given G.P. is Here, a = First term = r = Common ratio = Question 2: Find the 12 th term
More informationINF5820 MT 26 OCT 2012
INF582 MT 26 OCT 22 H22 Jn Tor Lønnng l@.uo.no Tody Ssl hn rnslon: Th nosy hnnl odl Word-bsd IBM odl Trnng SMT xpl En o lgd n r d bygg..9 h.6 d.3.9 rgh.9 wh.4 buldng.45 oo.3 rd.25 srgh.7 by.3 onsruon.33
More informationECE 422 Power System Operations & Planning 2 Synchronous Machine Modeling
ECE 422 Power System Operatons & Plannng 2 Synhronous Mahne Moelng Sprng 219 Instrutor: Ka Sun 1 Outlne 2.1 Moelng of synhronous generators for Stablty Stues Synhronous Mahne Moelng Smplfe Moels for Stablty
More informationChapter 13 Laplace Transform Analysis
Chapr aplac Tranorm naly Chapr : Ouln aplac ranorm aplac Tranorm -doman phaor analy: x X σ m co ω φ x X X m φ x aplac ranorm: [ o ] d o d < aplac Tranorm Thr condon Unlaral on-dd aplac ranorm: aplac ranorm
More informationNikon i-line Glass Series
Nkon ln la S ln la VNTS Nkon a an vlopmn of qualy maal a alway bn la o n fo ompany opal pou. Pon ky fao. van n la noloy pn upon pon, an a Nkon xl. Nkon ln la wa vlop fo u w ln ( nm) loapy un. I lv anman
More informationDynamic Safety Margin in Fault-Tolerant Predictive Controller
Pongs of h 5 IEEE onfn on onol pplons oono, n, gs 8-, 5 n Sf Mgn n Fl-oln Pv onoll M l-gll, E n, G oon L, Unvs of Mnnh, Gn lgll@n-nnh, n@n-nnh, g@n-nnh s n sf gn SM s nw pfon n s o s h sn wn pfn sf on
More informationSubrings and Ideals 2.1 INTRODUCTION 2.2 SUBRING
Subrings and Ideals Chapter 2 2.1 INTRODUCTION In this chapter, we discuss, subrings, sub fields. Ideals and quotient ring. We begin our study by defining a subring. If (R, +, ) is a ring and S is a non-empty
More informationt=0 t>0: + vr - i dvc Continuation
hapr Ga Dlay and rcus onnuaon s rcu Equaon >: S S Ths dffrnal quaon, oghr wh h nal condon, fully spcfs bhaor of crcu afr swch closs Our n challng: larn how o sol such quaons TUE/EE 57 nwrk analys 4/5 NdM
More informationMultiple-Choice Test Runge-Kutta 4 th Order Method Ordinary Differential Equations COMPLETE SOLUTION SET
Multpl-Co Tst Rung-Kutta t Ordr Mtod Ordnar Drntal Equatons COMPLETE SOLUTION SET. To solv t ordnar drntal quaton sn ( Rung-Kutta t ordr mtod ou nd to rwrt t quaton as (A sn ( (B ( sn ( (C os ( (D sn (
More information(heat loss divided by total enthalpy flux) is of the order of 8-16 times
16.51, Rok Prolson Prof. Manl Marnz-Sanhz r 8: Convv Ha ransfr: Ohr Effs Ovrall Ha oss and Prforman Effs of Ha oss (1) Ovrall Ha oss h loal ha loss r n ara s q = ρ ( ) ngrad ha loss s a S, and sng m =
More informationS.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15]
S.Y. B.Sc. (IT) : Sm. III Applid Mahmaics Tim : ½ Hrs.] Prlim Qusion Papr Soluion [Marks : 75 Q. Amp h following (an THREE) 3 6 Q.(a) Rduc h mari o normal form and find is rank whr A 3 3 5 3 3 3 6 Ans.:
More informationPhys463.nb Conductivity. Another equivalent definition of the Fermi velocity is
39 Anohr quival dfiniion of h Fri vlociy is pf vf (6.4) If h rgy is a quadraic funcion of k H k L, hs wo dfiniions ar idical. If is NOT a quadraic funcion of k (which could happ as will b discussd in h
More information- Prefixes 'mono', 'uni', 'bi' and 'du' - Why are there no asprins in the jungle? Because the parrots ate them all.
- Prfs '', '', 'b' a '' - Na: Wrsar 27 Dat: W ar tr asrs t? Bas t arrts at t a. At t btt f t a s a st f wrs. Ts wrs ar t. T wrs av b a rta (ra arss), vrta (ra w) r aa (fr rr t rr). W f a wr, raw a at r
More informationLecture 12: HEMT AC Properties
Lecure : HEMT A Proeres Quas-sac oeraon Transcaacances -araeers Non-quas ac effecs Parasc ressances / caacancs f f ax ean ue for aer 6: 7-86 95-407 {407-46 sk MEFET ars} 47-44. (.e. sk an MEFET ars brefl
More informationMulti-fluid magnetohydrodynamics in the solar atmosphere
Mul-flud magohydrodyams h solar amoshr Tmuraz Zaqarashvl თეიმურაზ ზაქარაშვილი Sa Rsarh Isu of Ausra Aadmy of Ss Graz Ausra ISSI-orksho Parally ozd lasmas asrohyss 6 Jauary- Fbruary 04 ISSI-orksho Parally
More informationChapter 8 Theories of Systems
~~ 7 Char Thor of Sm - Lala Tranform Solon of Lnar Sm Lnar Sm F : Conr n a n- n- a n- n- a a f L n n- ' ' ' n n n a a a a f Eg - an b ranform no ' ' b an b Lala ranform Sol Lf ]F-f 7 C 7 C C C ] a L a
More informationECE 522 Power Systems Analysis II 2 Power System Modeling
ECE 522 Power Systems Analyss II 2 Power System Moelng Sprng 218 Instrutor: Ka Sun 1 Outlne 2.1 Moelng of synhronous generators for Stablty Stues Synhronous Mahne Moelng Smplfe Moels for Stablty Stues
More informationImproved Ratio Estimators for Population Mean Based on Median Using Linear Combination of Population Mean and Median of an Auxiliary Variable
rcan Journal of Opraonal Rsarch : -7 DOI:.59/j.ajor.. Iprov Rao saors for Populaon an as on an Usng Lnar Cobnaon of Populaon an an an of an uxlar arabl Subhash Kuar aav San Sharan shra * lok Kuar Shukla
More informationFL/VAL ~RA1::1. Professor INTERVI of. Professor It Fr recru. sor Social,, first of all, was. Sys SDC? Yes, as a. was a. assumee.
B Pror NTERV FL/VAL ~RA1::1 1 21,, 1989 i n or Socil,, fir ll, Pror Fr rcru Sy Ar you lir SDC? Y, om um SM: corr n 'd m vry ummr yr. Now, y n y, f pr my ry for ummr my 1 yr Un So vr ummr cour d rr o l
More informationTHIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.
T H S PA G E D E CLA SSFED AW E O 2958 RS u blc Recod Key fo maon Ma n AR MATEREL COMM ND D cumen Type Call N u b e 03 V 7 Rcvd Rel 98 / 0 ndexe D 38 Eneed Dae RS l umbe 0 0 4 2 3 5 6 C D QC d Dac A cesson
More informationSAN JOSE CITY COLLEGE PHYSICAL EDUCATION BUILDING AND RENOVATED LAB BUILDING SYMBOL LIST & GENERAL NOTES - MECHANICAL
S SRUUR OR OORO SU sketch SYO SRPO OO OU O SUPPOR YP SUPPOR O UR SOS OVR SOS (xwx) X W (S) RR RWS U- R R OR ROO OR P S SPR SO S OS OW "Wx00"x0" 000.0, 8/7.0 Z U- R R UPPR ROO S S S SPR SO S OS OW 0"Wx0"x90"
More informationThe Variance-Covariance Matrix
Th Varanc-Covaranc Marx Our bggs a so-ar has bn ng a lnar uncon o a s o daa by mnmzng h las squars drncs rom h o h daa wh mnsarch. Whn analyzng non-lnar daa you hav o us a program l Malab as many yps o
More information176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s
A g la di ou s F. L. 462 E l ec tr on ic D ev el op me nt A i ng er A.W.S. 371 C. A. M. A l ex an de r 236 A d mi ni st ra ti on R. H. (M rs ) A n dr ew s P. V. 326 O p ti ca l Tr an sm is si on A p ps
More informationFREE VIBRATION ANALYSIS OF FUNCTIONALLY GRADED BEAMS
Journal of Appl Mathatcs an Coputatonal Mchancs, (), 9- FREE VIBRATION ANAYSIS OF FNCTIONAY GRADED BEAMS Stansław Kukla, Jowta Rychlwska Insttut of Mathatcs, Czstochowa nvrsty of Tchnology Czstochowa,
More informationNumerical solution of compressible fluid flow in porous media with boundary element method
Flud Sruur Inraon and Mong Boundary Probls IV 43 Nural soluon o orssbl lud low n orous da wh boundary ln hod R. Jl, L. Šrg & J. Krar Fauly o Cl Engnrng, Unrsy o Marbor, Slona Fauly o Mhanal Engnrng, Unrsy
More informationEmigration The movement of individuals out of an area The population decreases
Nm Clss D C 5 Puls S 5 1 Hw Puls Gw (s 119 123) Ts s fs ss us sb ul. I ls sbs fs ff ul sz xls w xl w ls w. Css f Puls ( 119) 1. W fu m ss f ul?. G sbu. Gw b. Ds. A suu 2. W s ul s sbu? I s b b ul. 3. A
More informationThe Mathematics of Harmonic Oscillators
Th Mhcs of Hronc Oscllors Spl Hronc Moon In h cs of on-nsonl spl hronc oon (SHM nvolvng sprng wh sprng consn n wh no frcon, you rv h quon of oon usng Nwon's scon lw: con wh gvs: 0 Ths s sos wrn usng h
More informationELECTROMAGNETISM, NUCLEAR STRUCTURES & GRAVITATION
. l & a s s Vo Flds o as l axwll a l sla () l Fld () l olasao () a Flx s () a Fld () a do () ad è s ( ). F wo Sala Flds s b dd l a s ( ) ad oool a s ( ) a oal o 4 qaos 3 aabls - w o Lal osas - oz abo Lal-Sd
More informationElectromagnetic waves in vacuum.
leromagne waves n vauum. The dsovery of dsplaemen urrens enals a peular lass of soluons of Maxwell equaons: ravellng waves of eler and magne felds n vauum. In he absene of urrens and harges, he equaons
More informationEQUATION SHEETS FOR ELEC
QUTON SHTS FO C 47 Fbuay 7 QUTON SHTS FO C 47 Fbuay 7 hs hυ h ω ( J ) h.4 ω υ ( µ ) ( ) h h k π υ ε ( / s ) G Os (Us > x < a ) Sll s aw s s s Shal z z Shal buay (, aus ) z y y z z z Shal ls ( s sua, s
More informationelnpol^l SSJU (tl = N) gnot
ZZ'Uap 66-' S fbul - alnph lluuur!^u SSf, psnu '6 ajns ' l/mu) l,u l fuan 's 'b rll ' p9 'z p6 ua ' "'s pr.u6lu rna u! 6url6ll l4s a11 ap]sap na plnm'6lu l bulm ll psnu aln5 11r1/vu) l,u lusl ll l p usal
More informationScripture quotations marked cev are from the Contemporary English Version, Copyright 1991, 1992, 1995 by American Bible Society. Used by permission.
N Ra: E K B Da a a B a a, a-a- a aa, a a. T, a a. 2009 Ba P, I. ISBN 978-1-60260-296-0. N a a a a a, a,. C a a a Ba P, a 500 a a aa a. W, : F K B Da, Ba P, I. U. S a a a a K Ja V B. S a a a a N K Ja V.
More informationResponse of MDOF systems
Response of MDOF syses Degree of freedo DOF: he nu nuber of ndependen coordnaes requred o deerne copleely he posons of all pars of a syse a any nsan of e. wo DOF syses hree DOF syses he noral ode analyss
More informationEE105 Fall 2015 Microelectronic Devices and Circuits. LTI: Linear Time-Invariant System
EE5 Fall 5 Mrolron Dvs and Crus Prof. Mng C. Wu wu@s.rkl.du 5 Suarda Da all SD - LTI: Lnar Tm-Invaran Ssm Ssm s lnar sudd horoughl n 6AB: Ssm s m nvaran: Thr s no lok or m rfrn Th ransfr funon s no a funon
More information10.5 Linear Viscoelasticity and the Laplace Transform
Scn.5.5 Lnar Vclacy and h Lalac ranfrm h Lalac ranfrm vry uful n cnrucng and analyng lnar vclac mdl..5. h Lalac ranfrm h frmula fr h Lalac ranfrm f h drvav f a funcn : L f f L f f f f f c..5. whr h ranfrm
More informationReliability Mathematics Analysis on Traction Substation Operation
WSES NSCIONS o HEICS Hoh S lal aha al o rao Sao Orao HONSHEN SU Shool o oao a Elral Er azho Jaoo Ur azho 77..CHIN h@6.o ra: - I lr ralwa rao owr l h oraoal qal a rlal o h a rao raorr loo hhr o o o oaral
More informationTheory of the non-linear quantized electromagnetic waves, adequate of Standard Model theory
Thor of h non-lnar quand lroagn wavs adqua of Sandard Modl hor Alandr G. Krakos San-Prsburg Sa Insu of Thnolog S. Prsburg Russa. -al: agkrak@hol.gr agkrak@ahoo.o Absra A solar sabl wav solon - s dfnd as
More informationCHAPTER-2. S.No Name of the Sub-Title No. 2.5 Use of Modified Heffron Phillip's model in Multi- Machine Systems 32
9 HAPT- hapr : MODIFID HFFON PHILLIP MODL.No Nam of h ub-tl Pag No.. Inroucon..3 Mollng of Powr ym Hffron Phllp Mol.4 Mof Hffron Phllp Mol 7.5 U of Mof Hffron Phllp mol n Mul- Machn ym 3 HAPT-.. Inroucon
More informationRoot behavior in fall and spring planted roses...
Rerospecive Theses and Disseraions Iowa Sae Universiy Capsones, Theses and Disseraions 1-1-1949 Roo behavior in fall and spring planed roses... Griffih J. Buck Iowa Sae College Follow his and addiional
More informationTHEORETICAL AUTOCORRELATIONS. ) if often denoted by γ. Note that
THEORETICAL AUTOCORRELATIONS Cov( y, y ) E( y E( y))( y E( y)) ρ = = Var( y) E( y E( y)) =,, L ρ = and Cov( y, y ) s ofen denoed by whle Var( y ) f ofen denoed by γ. Noe ha γ = γ and ρ = ρ and because
More informationTwo-Dimensional Quantum Harmonic Oscillator
D Qa Haroc Oscllaor Two-Dsoal Qa Haroc Oscllaor 6 Qa Mchacs Prof. Y. F. Ch D Qa Haroc Oscllaor D Qa Haroc Oscllaor ch5 Schrödgr cosrcd h cohr sa of h D H.O. o dscrb a classcal arcl wh a wav ack whos cr
More informationHomework 4 Solutions
Hoework 4 s Fall 017 65 Points Proble 6.. (10 points) A plane wave is reflected fro the ocean floor at noral incidence with a level 0 db below that of the incident wave Possible values of the specific
More informationHandout on. Crystal Symmetries and Energy Bands
dou o Csl s d g Bds I hs lu ou wll l: Th loshp bw ss d g bds h bs of sp-ob ouplg Th loshp bw ss d g bds h ps of sp-ob ouplg C 7 pg 9 Fh Coll Uvs d g Bds gll hs oh Th sl pol ss ddo o h l slo s: Fo pl h
More informationOUTLINE FOR Chapter 2-2. Basic Laws
0//8 OUTLINE FOR Chapr - AERODYNAMIC W-- Basc Laws Analss of an problm n fld mchancs ncssarl nclds samn of h basc laws gornng h fld moon. Th basc laws, whch applcabl o an fld, ar: Consraon of mass Conn
More informationc. What is the average rate of change of f on the interval [, ]? Answer: d. What is a local minimum value of f? Answer: 5 e. On what interval(s) is f
Essential Skills Chapter f ( x + h) f ( x ). Simplifying the difference quotient Section. h f ( x + h) f ( x ) Example: For f ( x) = 4x 4 x, find and simplify completely. h Answer: 4 8x 4 h. Finding the
More informationJ = 1 J = 1 0 J J =1 J = Bout. Bin (1) Ey = 4E0 cos(kz (2) (2) (3) (4) (5) (3) cos(kz (1) ωt +pπ/2) (2) (6) (4) (3) iωt (3) (5) ωt = π E(1) E = [E e
) ) Cov&o for rg h of olr&o for gog o&v r&o: - Look wv rog&g owr ou (look r&o). - F r wh o&o of fil vor. - I h CCWLHCP CWRHCP - u &l & hv oo g, h lr- fil vor r ou rgh- h orkrw for RHCP! 3) For h followg
More informationExercises for lectures 23 Discrete systems
Exrciss for lcturs 3 Discrt systms Michal Šbk Automatické říí 06 30-4-7 Stat-Spac a Iput-Output scriptios Automatické říí - Kybrtika a robotika Mols a trasfrs i CSTbx >> F=[ ; 3 4]; G=[ ;]; H=[ ]; J=0;
More informationC241 Homework Assignment 9
C41 Homework Assignment 9 1. The language L and functions R, A, and T defined below are the same as in Section 7.6. L {a, b, } + 1. L a. u L au L b. u L bu L 3. n. e. A: L L R: L L T : L L 1. A(, v) =
More information" W I T H M A L I C E T O W A - P t D N O I S T E A - I S T D O H A n i T Y F O R. A L L. " A TENDERFOOT. an awful storm." At this juncture,
v «> X k < W L W - P N - Y F R L L / L N LWLL N UNY PR 9 WL N - [N v v NRF N -Nv j k q v v k k v k Rk x - v N W k - WLL PN NG NV k Rk G v Y L v k (?)! V W k ) W k v k P UL W Pj$ V G k v -) v k W j v k
More informationn r t d n :4 T P bl D n, l d t z d th tr t. r pd l
n r t d n 20 20 :4 T P bl D n, l d t z d http:.h th tr t. r pd l 2 0 x pt n f t v t, f f d, b th n nd th P r n h h, th r h v n t b n p d f r nt r. Th t v v d pr n, h v r, p n th pl v t r, d b p t r b R
More informationThe non-linear wave theory, adequate of Standard Model
Th non-lnar wav hor adqua of Sandard Modl Alandr G. Krakos S. Prsburg Russa. -al: a.g.krak@hoal.o agkrak@hol.gr Absra A solar sabl wav solon - s dfnd as a saall onfnd (loald) non-dsrsv and non-sngular
More information4" 4" BM 7 SPIKE IN POWER POLE ELEV= " CP 15 8" 4" 10" 4" 6" 4" 6" 8" 8" 8" 12" 12" 16" 8" 4" 10" 6"
AR PLAN OVRVI -0 OLD SAUK ROAD RAFFIC MUS ALAYS B KP OPN; SOUHRN LAN MAY B CLOSD DURIN OFF-PAK HOURS IF FLARS AR USD; RFR O RAFFIC SCIONS IN SPCIAL PROVISIONS --- AR OR CONSRUCION SI NRANC; COORDINA NRY
More informationTheoretical Seismology
Thorcal Ssmology Lcur 9 Sgnal Procssng Fourr analyss Fourr sudd a h Écol Normal n Pars, augh by Lagrang, who Fourr dscrbd as h frs among Europan mn of scnc, Laplac, who Fourr rad lss hghly, and by Mong.
More informationMotivation. Loop-suppressed B meson decays can serve as sensitive probes for New Physics:
Prong Nw Phy wh mon ay Ulrh Uwr Conn: Movaon Quark flavor phy n h Sanar Mol Exprmnal Sau Flavor phy yon h Sanar Mol HC Exprmn mon ky maurmn a h HC Movaon oop-uppr mon ay an rv a nv pro for Nw Phy: W Nw
More informationExhibit 2-9/30/15 Invoice Filing Page 1841 of Page 3660 Docket No
xhibit 2-9/3/15 Invie Filing Pge 1841 f Pge 366 Dket. 44498 F u v 7? u ' 1 L ffi s xs L. s 91 S'.e q ; t w W yn S. s t = p '1 F? 5! 4 ` p V -', {} f6 3 j v > ; gl. li -. " F LL tfi = g us J 3 y 4 @" V)
More informationOn the Existence and uniqueness for solution of system Fractional Differential Equations
OSR Jourl o Mhms OSR-JM SSN: 78-578. Volum 4 ssu 3 Nov. - D. PP -5 www.osrjourls.org O h Es d uquss or soluo o ssm rol Drl Equos Mh Ad Al-Wh Dprm o Appld S Uvrs o holog Bghdd- rq Asr: hs ppr w d horm o
More informationAnouncements. Conjugate Gradients. Steepest Descent. Outline. Steepest Descent. Steepest Descent
oucms Couga Gas Mchal Kazha (6.657) Ifomao abou h Sma (6.757) hav b pos ol: hp://www.cs.hu.u/~msha Tch Spcs: o M o Tusay afoo. o Two paps scuss ach w. o Vos fo w s caa paps u by Thusay vg. Oul Rvw of Sps
More informationP. We make the following assumptions
Inrnaonal Journal of Sn and Rsar IJSR ISSN Onln: 39-764 Ind oprnus alu 5: 7896 Impa Faor 5: 639 Opmal Ddnd Prolm n ompound Posson Modl w orng Df a Run Yanan Wang Xong Song H nrs of nolog Sool of Sn anjn34
More informationdy 1. If fx ( ) is continuous at x = 3, then 13. If y x ) for x 0, then f (g(x)) = g (f (x)) when x = a. ½ b. ½ c. 1 b. 4x a. 3 b. 3 c.
AP CALCULUS BC SUMMER ASSIGNMENT DO NOT SHOW YOUR WORK ON THIS! Complt ts problms during t last two wks of August. SHOW ALL WORK. Know ow to do ALL of ts problms, so do tm wll. Itms markd wit a * dnot
More informationENGR 7181 LECTURE NOTES WEEK 3 Dr. Amir G. Aghdam Concordia University
ENGR 78 LECTURE NOTES WEEK Dr. ir G. ga Concoria Univrity DT Equivalnt Tranfr Function for SSO Syt - So far w av tui DT quivalnt tat pac ol uing tp-invariant tranforation. n t ca of SSO yt on can u t following
More informationAPPH 4200 Physics of Fluids
APPH 4200 Physcs of Fluds A Few More Flud Insables (Ch. 12) Turbulence (Ch. 13) December 1, 2011 1.!! Vscous boundary layer and waves 2.! Sably of Parallel Flows 3.! Inroducon o Turbulence: Lorenz Model
More information