IX. EMPIRICAL ORTHOGONAL FUNCTIONS
|
|
- Patience Washington
- 6 years ago
- Views:
Transcription
1 IX. EMPIRICAL ORTHOGONAL FUNCTION A. Eprcl Orthogonl Functons (EOF): T Don Consdr sptl rry of dscrt t srs obsrvtons (for xpl stwrd currnt) t M loctons - u jt, whr j ndcts stton nubr (j =,... M) nd t ndcts th t stp [t =,...N; whr (N-) Δt = T; lngth of srs]. Th zro-lg cross-covrnc for th j th nd k th lnts of th rry s gvn by R = N N (u - u j)(u - u ) jk jt kt k, (IX.) t= whr R s squr, sytrc, rl M x M trx nd ovrbr ndcts dsgntd srs n vlu. Th dgonl lnts of R jk n (IX.) (or whr j = k) r th stton rcord vrncs ccordng to R = N N jj (u jt - u j) (IX.) t= Th totl vrnc of th syst (or rry) t srs (lso clld trc of R or Tr R) s M Tr R = R jj. (IX.) j= A dgonlzton of th M x M trx R (or dtld xplnton blow) ylds st of M prcl orthogonl functons (EOF) or ods; n whch th j th od conssts of Rl EIGENVECTOR j, wth coponnts =,,.M; nd for whch th j th nd k th ods r orthogonl to ch othr n th sns tht M j k = jk, (IX.4) = nd 4 Fbrury 009 Chptr IX EOFs Nots 8Wndll. Brown
2 Postv EIGENVALUE. such tht M R jk j = k. (IX.4b) j= (Not: Th nubr of M-coponnt gnvctors s qul to th nubr of sttons). Undr ths crcustncs, u jt cn b xpndd n trs of ths gnvctors j ccordng to u = M jt t j (IX.5) = whr th pltud t srs of th th gnvctor jcn b xprssd s = M u t j jt. (IX.5b) j= 4 Fbrury 009 Chptr IX EOFs Nots 8Wndll. Brown
3 Th vrnc of t s th vrnc of th th od. Th th od gnvlu s tht od s vrnc (.., nrgy). Th prcntg of th totl "syst" (or rry) vrnc, whch fro (IX.) cn b wrttn M Tr R =, (IX.6) tht s xplnd by tht od s gvn by th rto of /Tr R. j= Th dnsonl frst EOF (or od- EOF), s dfnd by th product of th norlzd ( gnvctor lj nd pltud l) or hs th lrgst vrnc or gnvlu l. lj( l ) (IX.6b) Ths st of gnvctors/gnvlus th soluton - s dtrnd by lst squr ft btwn th soluton nd th cross-covrnc trx R. Th bst ft to th cross-covrnc trx s dfnd by (R jk - l ljlk ) = nu. (IX.7) j k Mthtclly, th fttng-procss prttons th totl syst (or rry) vrblty vrnc nto st of M orthogonl ods; j / ; ch xplnng dffrnt pttrns of corrltd nforton n th rry, undr th rthr rtfcl constrnt tht th gnvctors b orthogonl (.., sttstclly ndpndnt fro ch othr). AN EXAMPLE OF THE APPLICATION OF THE T-EOF TECHNOLOGY Consdr th followng xpl of n rry of nvrtd cho soundr (IE) surnts d cross th contnntl slop nto th dp ocn swrd of th Azon Rvr outflow (Fgur. IX.). Th IE s n coustc projctor whos trvl t π fro th botto to th ocn to th surfc (s Fgur. IX.b) nd bck s rltd to ocn proprts prrly 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons
4 th dpth of th n throcln - ccordng to = ( /C) C(Z, t) dz, whr C s sound spd nd h s locl wtr dpth. Hydrogrphc surnts t th IE oorng st r usd to coput th dync hghts; whch r thn corrltd wth th corrspondng IE trvl ts. Th vrblty of th IE t-srs of quvlnt dync hght for ch of th oord IE dploynts s prsntd n (Fgur. IX.). h o Fgur. IX.. (-lft) Th locton of four botto-ountd nvrtd cho soundrs (IE) nd thr currnt tr oorngs tht wr dployd n th tropcl Atlntc fro (b-rght) Th dpths of th dffrnt nstrunts r llustrtd n th bthytrc trnsct. Fgur. IX. Dync hght t srs drvd fro IE trvl ts surd by nstrunts loctd n Fgur IX.. Th EOF dcoposton of th cross-covrnc trx of ths four (sclr) IE dync hght t srs (.., qu IX.) ylds four t-don EOFs (TD-EOF). Th norlzd gnvctor structurs of th two ost nrgtc IE TD-EOFs r dpctd n Fgur IX.. Not tht th t vrblty of thr of ths TD-EOFs cn b drvd by coputng th 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 4
5 product of th odl t srs (Fgur IX. 4) nd th norlzd gnvctor stton pltud structur. Th gostrophc trnsport nfrrd fro th gnod IE dffrncs r ndctd to th rght. Fgur. IX. To th lft r th norlzd structurs of th ost nrgtc IE gnods (MODE- bov nd MODE- blow). Also ndctd to th rght r th gostrophc trnsport dstrbutons tht r qulttvly consstnt th IE dync hght vrblty gnod structur. 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 5
6 Fgur. IX.4 Th pltud t srs (n dyn-) of th gnods prsntd n Fgur IX.. 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 6
7 B. Eprcl Orthogonl Functons: Frquncy Don Consdr -dnsonl vctor t srs V (t), wth coponnts v} {u,, tht hv bn dscrtly spld N, t to for Vn = V(n t) (IX.8) whr n =,,...N. Th coplx Fourr coffcnts r ^ V = t V N t n whr th rfrs to th frquncs whr th vctor dtls of V ^ f = f n - n xp N t = N t (IX.9) t whch ths r coputd. nd cn b xprssd nubr of dffrnt wys ; ^ V vˆ u u (IX.9b) Coplx Fourr coffcnts for th coponnts cn b xprssd n dffrnt wys s dscussd n th followng. Dfn th gnrl Crtsn cross-spctrl nrgy dnsty trx (DM) for n rbtrry nubr of coponnts of = < > j j, (IX.0) whr th ndx, rfrrng to frquncy hroncs, hs bn droppd. Th coplx rprsntton of cross-spctrl nrgy dnsty (DM) s = C - Q j j j (IX.) Th norlzd DM or spctru cohrnc j (IX.) j / (jj) 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 7
8 Th -coponnt j s x Hrtn trx, whr Hrtn pls tht γ uv = γ uv, s uu uv uv (IX.) vv Consdr th followng two spl knds of oton n th Crtsn rprsntton n whch thr hs bn two-fold dcoposton; n () frquncy nd () long utully-orthogonl xs (crtsn.g.).. Osclltory Rctlnr Moton - long n rbtrry ln dscrbd by r = + j, (IX.4) whr α nd β r drcton cosns. Fgur. IX.4 Hodogrph of rctlnr oton Fourr coponnts of th vlocty vctor [t so frquncy f ] r = o( ) vˆ = o( ) (IX.5) whr th phs of both coponnts θ = θ = θ. If θ = 0, thn or = o o (IX.6) ^ v = vˆ = 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 8 o o (IX.6b)
9 nd th DM, whch s rl for ths cs bcus thr s no phs lg btwn coponnts, s = < o > (IX.7) Not: If surd DM s rl, thn r y b dducd. For xpl, f α= nd β=0, thn th oton wll b only long th x-xs nd only uu rns.. Osclltory Ellptcl Moton Th Fourr coponnts = o xp vˆ = o xp ( / ), (IX.8) whr th ndcts th phs for rotton n thr drcton; + = ACW nd - = CW or ^ V = ( o o ) (IX.9) Fgur IX.5 Hodogrph for llptcl oton. 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 9
10 Thn th DM s purly gnry bcus of phs lg = < o > (IX.0) ( ) Not tht α = β => crculr oton Iportnt: In gnrl, snc ll lnts of th crtsn DM r non-zro th vlus α nd β dpnd on th crtsn xs orntton; whch s dsdvntg. Thus w sk or gnrl pproch. 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 0
11 Gnrl Fourr Coponnt Rprsntton ^ V = +, (IX.) whr ( =,) r coplx pltuds (s bfor), but now r bss vctors rprsntng dffrnt typs of oton (not orthogonl drctons. For xpl, rctlnr oton long utully-orthogonl xs r dscrbd n trs of Crtsn syst s follows: whr () th = ; 0 rprsnt oton n th two dffrnt drctons; 0 = (IX.) () th now tll us th pltud nd phs of th typ of oton dscrbd by unt vctors. ^ Th r found by fndng th projcton of V ^ = V ^ = V on th rspctv ccordng to (IX.) In ths cs t s trvl bcus thr s no phs (.. gnry prt) so tht = (= ) o (IX.4) = (= ) o (IX.4b) In ths cs, th gnrlzd Fourr coffcnt nd th r th s. 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons
12 Fgur. IX.6 Crtsn coponnts of typcl thr-dnsonl vctor t srs surnt (Cln, 978). 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons
13 Fgur. IX.7 Th Crtsn spctru dnsty trx for th dt shown n Fgur. IX.7 (Cln, 978). 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons
14 Fgur. IX.8 Rotry rprsntton of th dt shown n Fgur. IX.7 (Cln, 978). 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 4
15 ^ Rotry Rprsntton of V Th dcoposton n trs of Crtsn coponnts cn b rwrttn s ^ xp xp u u u V = = = C + C ( - / ) (IX.5) ( + / ) u u xp u xp whr th bss (or unt) vctors now r -/ -/ = = ; - (IX.6) + - Hodogrph Fgur IX.9 Hodogrph for crculr oton Countr-clockws nd clockws rottng crculr rottng unt vctor otons nd r orthonorl.. th sclr products r = (IX.7) = 0. W cn fnd th gnrlzd Fourr coffcnts by projctng th unt vctors onto th orgnl Crtsn Fourr coponnt vctor,.. 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 5
16 = + = ^ = V _ ^ = V = = -/ -/ ( - îu ) ( + îu ),.. / (, ) - / (, - ){ } (IX.8) whr = u = u. (IX.8b) Coputng th dgonl lnts of th gnrlzd spctrl nrgy dnsty trx = + = = < _ = < > = > = < < > + < > + < > - Q > + Q cohrnc btwn Not th rltonshp btwn th gnrlzd nd crtsn spctrl dnsts. _ (IX.9) A Gnrlzd pctrl Dnsty Mtrx Thn = j = < j > n whch th gnrlzd cohrncs r: < j > j =. / (IX.9) < >< j j > It cn b shown tht gnrlzd DM cn b drvd fro th Crtsn DM = c ccordng to c = j < j > = j (IX.0) 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 6
17 EMPIRICAL EIGENMODE PECTRA Lt us now gnrlz th prvous pproch stll furthr by dtrnng n orthonorl st of gnvctors g of th Crtsn cross-spctrl nrgy dnsty trx (DM) such tht c g = g, (IX.) whr th frquncy-dpndnt g cn b thought of s th kntcl norl ods for th t srs surnts.in th gnrl cs, th gnvctors g b found by solvng th gnvlu probl for ch frquncy. Expndng -D Fourr coponnt vctor ^ V n th gnvctors of th prtculr crossspctrl dnsty trx for spcfc frquncy: ^ V = + g g (IX.)!! whr / λ / λ r rl gnvlus, snc th DM s Hrtn. H r spctru pltuds r th orgnl lnts nd r = λ. W hv lrdy shown tht for th gnrlzd rprsntton of th Fourr coffcnt vctor ^ V = +... =, (IX.) th cohrnc btwn ods s coputd n trs of th gnrlzd cross-spctrl dnsty trx (or Crtsn DM) ccordng to By lttng j c < j > j. (IX.4) = g nd rcllng th orgnl gnvlu probl bov: = g c g Thn fro th orthonorl proprty of g j j = g g. j j (IX.5) 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 7
18 = j j j (IX.6) Bcus for = j j =, (IX.7) 0 for j nd = λ (IX.8) j 0 (IX.9) Th lttr showng tht th dffrnt ods g r ndpndnt (.., ll cohrncs r zro). But ths splcty cos t th xpns of or coplctd hodogrph for ch gnvctor. Eprcl Orthogonl Functons for -D Lnr Moton ^ Crtsn DM V o = ; o c = o olvng for th gnvlus of th bov probl lds to = < > ( + o = 0 whch shows tht only on od of oton prsnt t ths frquncy. ) Th corrspondng unt gntud gnvctor s g = N ; whr N (( + )). Hr g rprsnts lnr oton long r - th only cohrnt oton. Th scond gnvlu s dgnrt so tht g s ndtrnnt; g = 0. -/ 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 8
19 Eprcl Orthogonl Functons for -D Ellptcl Moton ^ V o = ( / o ) Crtsn DM c = < o > ( ) Egnvlus: λ = o (α + β ) ; λ = 0 Agn only on od of oton Unt Mgntud Egnvctor: = N g N = [( + -/ whr ] ) -/ 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 9
20 Fgur. IX.0 Eprcl od spctr for th dt shown n Fgur. IX.7. 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 0
21 Fgur. IX. Th thr-dnsonl Fourr vctor hologrph. Th prtrs whch spcfy th shp of th hodogrph r ndctd. THREE DIMENIONAL VECTOR whr V(t) = R u(t) V (t) = v(t) w(t) N/ - = ^ V f t Coplx Fourr Coffcnts ^ V = [ /(N t)] V n n (t) xp(- n/n T) t f = f = N t wth ^ V vˆ ŵ u u u Crtsn spctrl nrgy dnsty trx (DM) (subscrpt hs bn droppd) j whr < > nsbl vrg. < j > 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons
22 Off-dgonl lnts of th DM - coplx rprsntton: j = C j - Q j co- qud- spctr Coplx Cohrnc j [ j / jj] j s x Hrtn ( rl nd coplx ndpndnt lnts) trx hr uu uv uu ww uw vv (Hrtn lowr lft off dgonl lnts r coplx conjugts of uppr rght off dgonl lnts.) For Fourr coponnt vctors fro two surnts (k) = (k) (k) (k) wth k =,,,. Th cross-spctrl dnsty trx (CDM) s 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons
23 (k) j = < (k) () j > Ths s 6x6 Hrtn trx < >< vˆ >< ŵ >< >< vˆ >< ŵ > < vˆ vˆ >< vˆ ŵ > < ŵ ŵ > < u > nd vctor ELLIPTIC MOTION - n Crtsn rprsntton for on -D vctor whr, f α = β, thn th oton s crculr. In gnrl, lt th Fourr coponnt vctor, wth coplx, b rprsntd ^ V = + + whr r unt vctors - ch rprsntng prtculr typ of oton. For xpl, Crtsn In gnrl, = = 0 ^ = V j = j 0 = 0 orthonorl 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons
24 whr n ths cs, = u Gnrlzd pctrl Dnsty Mtrx Gnrlzd Cohrnc ; whch pls rctlnr oton. j j < [< j > < j j >< > j > ] / It cn b shown tht ny gnrlzd DM cn b found fro th Crtsn DM, (c), by usng th pproprt (orthonorl) unt vctors to trnsfor th spctru ccordng to j < j > (c) j. For ultpl-vctor t srs, th cross-spctru dnsty trx gnrlzs n th s wy n ths cs, lthough () nd () ^ V = = y b dffrnt () () nd ^ U = () () = < ˆ ()() () () Gnrlzd CDM j â j > whr usully ê = ê () (). Rottonl Invrnts Trc Tr = x KE Tr M = x KE = < > = nd KE = (u ) Dtrnnt of DM 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 4
25 = (- - = + R ) whr Γ = γ γ γ nd γ j r coplx cohrncs. For -D, th Dtrnnt s H = (- ( ) ) nd sur of th ncohrnt nos Dgr of Polrzton P - (/ Tr M P H ) s th frcton of non-rndo, non-sotropc nrgy P s rl nd vrs btwn 0 nd. 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 5
26 Ansotropy Rto A P A = - P s th rto of non-rndo, non-sotropc nrgy to th rndo, sotropc nrgy (.., sgnl to nos rto). u of Prncpl Mnors Th -D dtrnnt n on of th coordnt plns M M = j Mn dgr of polrzton M =- (Tr) P jj - Totl qurd Qudrtur pctru Q / ( j j - j ) j Q whch s th nt ount of rottng nrgy n pln. Rotry Coffcnt QH CrH, / Tr H whch s th frcton of th nt rottng Mn Rotry Coffcnt Cr Q / Tr = j j, Multpl Cohrnc - M rd prncpl nor ROTARY REPREENTATION Fourr vctor s dcoposd nto two countr-rottng crculr otons n pln (usully th horzontl pln). In -D, lnr oscllton tht s norl to th pln of rotry vctors s ddd 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 6
27 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 7 u C 0 u u + C 0 u u = C u u u = V ) - ( ) / + ( ^ Ths cn b wrttn n trs of th followng unt vctors 0 = -/ Countr-Clockws 0 - = -/ Clockws 0 0 Vrtcl Gnrlzd Fourr Coffcnts countrclockws (+) - ) - ( = V - = -/ ^ + clockws (-) - ) + ( = V = = -/ ^ - vrtcl -, = u V = ^ whr = u tc. ELEMENT OF THE GENERALIZED DM cn b found usng Crtsn pctrl Dnsty Mtrx > < j j or
28 (c) j Crtsn spctrl dnsty trx = + = < > =/ < > + < > - Q / Tr H Q (- Cr) Cr = Tr uv H = - = < > =/ Tr H (+ Cr) coputd fro th Crtsn DM = < > = < > = w + ; - r th rotry spctr "nnr utospctr" of Moors,97 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 8
29 Rotry coffcnt C r = frcton of nt rottng nrgy Norlzd Cross pctru = = / + - ( ) / (uu - vv) - Cuv = / / (Tr H )(- Cr ) + - tblty = (P - Cr ) /(- Cr ) whr +- tn < + - > = C uv /( Rnng Cohrnc Elnt for -D vctors +-w vv - uu ), (outr utospctru (Moors)) < + > (uw vw) = = / / < >< > ( w ) Rotry pctru Rprsntton for -D Vctor w -w w 4 Fbrury 009 Chptr IX. Eprcl Orthogonl Functons 9
A general N-dimensional vector consists of N values. They can be arranged as a column or a row and can be real or complex.
Lnr lgr Vctors gnrl -dmnsonl ctor conssts of lus h cn rrngd s column or row nd cn rl or compl Rcll -dmnsonl ctor cn rprsnt poston, loct, or cclrton Lt & k,, unt ctors long,, & rspctl nd lt k h th componnts
More informationConvergence Theorems for Two Iterative Methods. A stationary iterative method for solving the linear system: (1.1)
Conrgnc Thors for Two Itrt Mthods A sttonry trt thod for solng th lnr syst: Ax = b (.) ploys n trton trx B nd constnt ctor c so tht for gn strtng stt x of x for = 2... x Bx c + = +. (.2) For such n trton
More informationFundamentals of Continuum Mechanics. Seoul National University Graphics & Media Lab
Fndmntls of Contnm Mchncs Sol Ntonl Unvrsty Grphcs & Md Lb Th Rodmp of Contnm Mchncs Strss Trnsformton Strn Trnsformton Strss Tnsor Strn T + T ++ T Strss-Strn Rltonshp Strn Enrgy FEM Formlton Lt s Stdy
More informationPreview. Graph. Graph. Graph. Graph Representation. Graph Representation 12/3/2018. Graph Graph Representation Graph Search Algorithms
/3/0 Prvw Grph Grph Rprsntton Grph Srch Algorthms Brdth Frst Srch Corrctnss of BFS Dpth Frst Srch Mnmum Spnnng Tr Kruskl s lgorthm Grph Drctd grph (or dgrph) G = (V, E) V: St of vrt (nod) E: St of dgs
More informationBasic Electrical Engineering for Welding [ ] --- Introduction ---
Basc Elctrcal Engnrng for Wldng [] --- Introducton --- akayosh OHJI Profssor Ertus, Osaka Unrsty Dr. of Engnrng VIUAL WELD CO.,LD t-ohj@alc.co.jp OK 15 Ex. Basc A.C. crcut h fgurs n A-group show thr typcal
More information(A) the function is an eigenfunction with eigenvalue Physical Chemistry (I) First Quiz
96- Physcl Chmstry (I) Frst Quz lctron rst mss m 9.9 - klogrm, Plnck constnt h 6.66-4 oul scon Sp of lght c. 8 m/s, lctron volt V.6-9 oul. Th functon F() C[cos()+sn()] s n gnfuncton of /. Th gnvlu s (A)
More informationPhys 2310 Wed. Sept. 13, 2017 Today s Topics
Phys 3 Wd. Spt. 3, 7 Tody s Topcs Chptr 5: Th Suprposton of Wvs Intrfrnc Mthods for Addng Wvs Boundry Condtons Stndng Wvs & Norl Mods Supplntry Mtrl: Fourr Anlyss Rdng for Nxt T Howork ths Wk SZ Chptr
More informationDefinition of vector and tensor. 1. Vector Calculus and Index Notation. Vector. Special symbols: Kronecker delta. Symbolic and Index notation
Dfnton of vctor nd tnsor. Vctor Clculus nd Indx Notton Crtsn nsor only Pnton s Chp. Vctor nd ordr tnsor v = c v, v = c v = c c, = c c k l kl kl k l m physcl vrbl, sm symbolc form! Cn b gnrlzd to hghr ordr
More informationInner Product Spaces INNER PRODUCTS
MA4Hcdoc Ir Product Spcs INNER PRODCS Dto A r product o vctor spc V s ucto tht ssgs ubr spc V such wy tht th ollowg xos holds: P : w s rl ubr P : P : P 4 : P 5 : v, w = w, v v + w, u = u + w, u rv, w =
More informationMinimum Spanning Trees
Mnmum Spnnng Trs Spnnng Tr A tr (.., connctd, cyclc grph) whch contns ll th vrtcs of th grph Mnmum Spnnng Tr Spnnng tr wth th mnmum sum of wghts 1 1 Spnnng forst If grph s not connctd, thn thr s spnnng
More informationJones vector & matrices
Jons vctor & matrcs PY3 Colást na hollscol Corcagh, Ér Unvrst Collg Cork, Irland Dpartmnt of Phscs Matr tratmnt of polarzaton Consdr a lght ra wth an nstantanous -vctor as shown k, t ˆ k, t ˆ k t, o o
More informationTOPIC 5: INTEGRATION
TOPIC 5: INTEGRATION. Th indfinit intgrl In mny rspcts, th oprtion of intgrtion tht w r studying hr is th invrs oprtion of drivtion. Dfinition.. Th function F is n ntidrivtiv (or primitiv) of th function
More informationA Solution for multi-evaluator AHP
ISAHP Honoll Hw Jly 8- A Solton for lt-vltor AHP Ms Shnohr Kch Osw Yo Hd Nhon Unvrsty Nhon Unvrsty Nhon Unvrsty Iz-cho Nrshno Iz-cho Nrshno Iz-cho Nrshno hb 7-87 Jpn hb 7-87 Jpn M7snoh@ct.nhon-.c.p 7oosw@ct.nhon-.c.p
More informationThe Hyperelastic material is examined in this section.
4. Hyprlastcty h Hyprlastc matral s xad n ths scton. 4..1 Consttutv Equatons h rat of chang of ntrnal nrgy W pr unt rfrnc volum s gvn by th strss powr, whch can b xprssd n a numbr of dffrnt ways (s 3.7.6):
More informationPH427/PH527: Periodic systems Spring Overview of the PH427 website (syllabus, assignments etc.) 2. Coupled oscillations.
Dy : Mondy 5 inuts. Ovrviw of th PH47 wsit (syllus, ssignnts tc.). Coupld oscilltions W gin with sss coupld y Hook's Lw springs nd find th possil longitudinl) otion of such syst. W ll xtnd this to finit
More informationLecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:
Lctur 11 Wvs in Priodic Potntils Tody: 1. Invrs lttic dfinition in 1D.. rphicl rprsnttion of priodic nd -priodic functions using th -xis nd invrs lttic vctors. 3. Sris solutions to th priodic potntil Hmiltonin
More informationHaving a glimpse of some of the possibilities for solutions of linear systems, we move to methods of finding these solutions. The basic idea we shall
Hvn lps o so o t posslts or solutons o lnr systs, w ov to tos o nn ts solutons. T s w sll us s to try to sply t syst y lntn so o t vrls n so ts qutons. Tus, w rr to t to s lnton. T prry oprton nvolv s
More informationReview - Probabilistic Classification
Mmoral Unvrsty of wfoundland Pattrn Rcognton Lctur 8 May 5, 6 http://www.ngr.mun.ca/~charlsr Offc Hours: Tusdays Thursdays 8:3-9:3 PM E- (untl furthr notc) Gvn lablld sampls { ɛc,,,..., } {. Estmat Rvw
More informationECE507 - Plasma Physics and Applications
ECE57 - Plasa Physcs and Applcatons Lctur Prof. Jorg Rocca and Dr. Frnando Toasl Dpartnt of Elctrcal and Coputr Engnrng Introducton: What s a plasa? A quas-nutral collcton of chargd (and nutral) partcls
More informationINTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x)
Chptr 7 INTEGRALS 7. Ovrviw 7.. Lt d d F () f (). Thn, w writ f ( ) d F () + C. Ths intgrls r clld indfinit intgrls or gnrl intgrls, C is clld constnt of intgrtion. All ths intgrls diffr y constnt. 7..
More information8. Linear Contracts under Risk Neutrality
8. Lnr Contrcts undr Rsk Nutrlty Lnr contrcts r th smplst form of contrcts nd thy r vry populr n pplctons. Thy offr smpl ncntv mchnsm. Exmpls of lnr contrcts r mny: contrctul jont vnturs, quty jont vnturs,
More informationPhys 2310 Fri. Nov. 7, 2014 Today s Topics. Begin Chapter 15: The Superposition of Waves Reading for Next Time
Phys 3 Fr. Nov. 7, 4 Today s Topcs Bgn Chaptr 5: Th Suprposton of Wavs Radng for Nxt T Radng ths Wk By Frday: Bgn Ch. 5 (5. 5.3 Addton of Wavs of th Sa Frquncy, Addton of Wavs of Dffrnt Frquncy, Rad Supplntary
More informationFilter Design Techniques
Fltr Dsgn chnqus Fltr Fltr s systm tht psss crtn frquncy componnts n totlly rcts ll othrs Stgs of th sgn fltr Spcfcton of th sr proprts of th systm ppromton of th spcfcton usng cusl scrt-tm systm Rlzton
More informationHeisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari
snbrg Modl Sad Mohammad Mahd Sadrnhaad Survsor: Prof. bdollah Langar bstract: n ths rsarch w tr to calculat analtcall gnvalus and gnvctors of fnt chan wth ½-sn artcls snbrg modl. W drov gnfuctons for closd
More informationh Summary Chapter 7.
Summry Chptr 7. In Chptr 7 w dscussd byond th fr lctron modl of chptr 6. In prtculrly w focusd on th nflunc of th prodc potntl of th on cors on th nrgy lvl dgrm of th outr lctrons of th toms. It wll hlp
More information1) They represent a continuum of energies (there is no energy quantization). where all values of p are allowed so there is a continuum of energies.
Unbound Stats OK, u untl now, w a dalt solly wt stats tat ar bound nsd a otntal wll. [Wll, ct for our tratnt of t fr artcl and w want to tat n nd r.] W want to now consdr wat ans f t artcl s unbound. Rbr
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 informationPhy213: General Physics III 4/10/2008 Chapter 22 Worksheet 1. d = 0.1 m
hy3: Gnral hyscs III 4/0/008 haptr Worksht lctrc Flds: onsdr a fxd pont charg of 0 µ (q ) q = 0 µ d = 0 a What s th agntud and drcton of th lctrc fld at a pont, a dstanc of 0? q = = 8x0 ˆ o d ˆ 6 N ( )
More informationGrand Canonical Ensemble
Th nsmbl of systms mmrsd n a partcl-hat rsrvor at constant tmpratur T, prssur P, and chmcal potntal. Consdr an nsmbl of M dntcal systms (M =,, 3,...M).. Thy ar mutually sharng th total numbr of partcls
More information1.9 Cartesian Tensors
Scton.9.9 Crtsn nsors s th th ctor, hghr ordr) tnsor s mthmtc obct hch rprsnts mny physc phnomn nd hch xsts ndpndnty of ny coordnt systm. In ht foos, Crtsn coordnt systm s sd to dscrb tnsors..9. Crtsn
More informationRate of Molecular Exchange Through the Membranes of Ionic Liquid Filled. Polymersomes Dispersed in Water
Supportng Informton for: Rt of Molculr Exchng hrough th Mmrns of Ionc Lqud Flld olymrsoms Dsprsd n Wtr Soonyong So nd mothy. Lodg *,, Dprtmnt of Chmcl Engnrng & Mtrls Scnc nd Dprtmnt of Chmstry, Unvrsty
More informationCHAPTER 4. The First Law of Thermodynamics for Control Volumes
CHAPTER 4 T Frst Law of Trodynacs for Control olus CONSERATION OF MASS Consrvaton of ass: Mass, lk nrgy, s a consrvd proprty, and t cannot b cratd or dstroyd durng a procss. Closd systs: T ass of t syst
More informationSpecial Random Variables: Part 1
Spcl Rndom Vrbls: Prt Dscrt Rndom Vrbls Brnoull Rndom Vrbl (wth prmtr p) Th rndom vrbl x dnots th succss from trl. Th probblty mss functon of th rndom vrbl X s gvn by p X () p X () p p ( E[X ]p Th momnt
More informationVowel package manual
Vwl pckg mnl FUKUI R Grdt Schl f Hmnts nd Sclgy Unvrsty f Tky 28 ctbr 2001 1 Drwng vwl dgrms 1.1 Th vwl nvrnmnt Th gnrl frmt f th vwl nvrnmnt s s fllws. [ptn(,ptn,)] cmmnds fr npttng vwls ptns nd cmmnds
More informationThe Fourier Transform
/9/ Th ourr Transform Jan Baptst Josph ourr 768-83 Effcnt Data Rprsntaton Data can b rprsntd n many ways. Advantag usng an approprat rprsntaton. Eampls: osy ponts along a ln Color spac rd/grn/blu v.s.
More informationGUC (Dr. Hany Hammad) 9/28/2016
U (r. Hny Hd) 9/8/06 ctur # 3 ignl flow grphs (cont.): ignl-flow grph rprsnttion of : ssiv sgl-port dvic. owr g qutions rnsducr powr g. Oprtg powr g. vill powr g. ppliction to Ntwork nlyzr lirtion. Nois
More informationELEG 413 Lecture #6. Mark Mirotznik, Ph.D. Professor The University of Delaware
LG 43 Lctur #6 Mrk Mirtnik, Ph.D. Prfssr Th Univrsity f Dlwr mil: mirtni@c.udl.du Wv Prpgtin nd Plritin TM: Trnsvrs lctrmgntic Wvs A md is prticulr fild cnfigurtin. Fr givn lctrmgntic bundry vlu prblm,
More informationSpanning Tree. Preview. Minimum Spanning Tree. Minimum Spanning Tree. Minimum Spanning Tree. Minimum Spanning Tree 10/17/2017.
0//0 Prvw Spnnng Tr Spnnng Tr Mnmum Spnnng Tr Kruskl s Algorthm Prm s Algorthm Corrctnss of Kruskl s Algorthm A spnnng tr T of connctd, undrctd grph G s tr composd of ll th vrtcs nd som (or prhps ll) of
More informationAnalyzing Frequencies
Frquncy (# ndvduals) Frquncy (# ndvduals) /3/16 H o : No dffrnc n obsrvd sz frquncs and that prdctd by growth modl How would you analyz ths data? 15 Obsrvd Numbr 15 Expctd Numbr from growth modl 1 1 5
More informationCh 1.2: Solutions of Some Differential Equations
Ch 1.2: Solutions of Som Diffrntil Equtions Rcll th fr fll nd owl/mic diffrntil qutions: v 9.8.2v, p.5 p 45 Ths qutions hv th gnrl form y' = y - b W cn us mthods of clculus to solv diffrntil qutions of
More informationMath 656 Midterm Examination March 27, 2015 Prof. Victor Matveev
Math 656 Mdtrm Examnatn March 7, 05 Prf. Vctr Matvv ) (4pts) Fnd all vals f n plar r artsan frm, and plt thm as pnts n th cmplx plan: (a) Snc n-th rt has xactly n vals, thr wll b xactly =6 vals, lyng n
More informationLecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation
Lctur Rlc nutrnos mpratur at nutrno dcoupln and today Effctv dnracy factor Nutrno mass lmts Saha quaton Physcal Cosmoloy Lnt 005 Rlc Nutrnos Nutrnos ar wakly ntractn partcls (lptons),,,,,,, typcal ractons
More informationPrinciple Component Analysis
Prncple Component Anlyss Jng Go SUNY Bufflo Why Dmensonlty Reducton? We hve too mny dmensons o reson bout or obtn nsghts from o vsulze oo much nose n the dt Need to reduce them to smller set of fctors
More informationLecture 3: Phasor notation, Transfer Functions. Context
EECS 5 Fall 4, ctur 3 ctur 3: Phasor notaton, Transfr Functons EECS 5 Fall 3, ctur 3 Contxt In th last lctur, w dscussd: how to convrt a lnar crcut nto a st of dffrntal quatons, How to convrt th st of
More informationChapter 6 Student Lecture Notes 6-1
Chaptr 6 Studnt Lctur Nots 6-1 Chaptr Goals QM353: Busnss Statstcs Chaptr 6 Goodnss-of-Ft Tsts and Contngncy Analyss Aftr compltng ths chaptr, you should b abl to: Us th ch-squar goodnss-of-ft tst to dtrmn
More informationUNIVERSITY OF IOANNINA DEPARTMENT OF ECONOMICS. M.Sc. in Economics MICROECONOMIC THEORY I. Problem Set II
Mcroeconomc Theory I UNIVERSITY OF IOANNINA DEPARTMENT OF ECONOMICS MSc n Economcs MICROECONOMIC THEORY I Techng: A Lptns (Note: The number of ndctes exercse s dffculty level) ()True or flse? If V( y )
More information22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 2: Derivation of Ideal MHD Equation
.65, MHD Thory of Fuson Systms Prof. Frdbrg Lctur : Drvton of Idl MHD Equton Rvw of th Drvton of th Momnt Equton. Strtng Pont: Boltzmnn Equton for lctrons, ons nd Mxwll Equtons. Momnts of Boltzmnn Equton:
More information1. Stefan-Boltzmann law states that the power emitted per unit area of the surface of a black
Stf-Boltzm lw stts tht th powr mttd pr ut r of th surfc of blck body s proportol to th fourth powr of th bsolut tmprtur: 4 S T whr T s th bsolut tmprtur d th Stf-Boltzm costt= 5 4 k B 3 5c h ( Clcult 5
More informationΕρωτήσεις και ασκησεις Κεφ. 10 (για μόρια) ΠΑΡΑΔΟΣΗ 29/11/2016. (d)
Ερωτήσεις και ασκησεις Κεφ 0 (για μόρια ΠΑΡΑΔΟΣΗ 9//06 Th coffcnt A of th van r Waals ntracton s: (a A r r / ( r r ( (c a a a a A r r / ( r r ( a a a a A r r / ( r r a a a a A r r / ( r r 4 a a a a 0 Th
More information5. 5. Detection of of Signals in in Noise
5. 5. Dtton of of Sgnl n n o Dtton probl: Gvn th obrvton vtor, w, thn, prfor ppng dodng fro to n ttd ˆ of th trnttd ybol, n wy tht would nz th probblty of rror n th don kng pro. W wll how tht, n th tht
More informationWeighted Graphs. Weighted graphs may be either directed or undirected.
1 In mny ppltons, o rp s n ssot numrl vlu, ll wt. Usully, t wts r nonntv ntrs. Wt rps my tr rt or unrt. T wt o n s otn rrr to s t "ost" o t. In ppltons, t wt my msur o t lnt o rout, t pty o ln, t nry rqur
More informationDiscrete Shells Simulation
Dscrt Shlls Smulaton Xaofng M hs proct s an mplmntaton of Grnspun s dscrt shlls, th modl of whch s govrnd by nonlnar mmbran and flxural nrgs. hs nrgs masur dffrncs btwns th undformd confguraton and th
More informationIntegration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals
Intgrtion Continud Intgrtion y Prts Solving Dinit Intgrls: Ar Undr Curv Impropr Intgrls Intgrtion y Prts Prticulrly usul whn you r trying to tk th intgrl o som unction tht is th product o n lgric prssion
More information2.10 Convected Coordinates
Scton.0.0 onctd oordnats An ntroducton to curlnar coordnat was n n scton.6 whch srs as an ntroducton to ths scton. As ntond thr th orulaton o alost all chancs probls and thr nurcal plntaton and soluton
More informationMulti-Section Coupled Line Couplers
/0/009 MultiSction Coupld Lin Couplrs /8 Multi-Sction Coupld Lin Couplrs W cn dd multipl coupld lins in sris to incrs couplr ndwidth. Figur 7.5 (p. 6) An N-sction coupld lin l W typiclly dsign th couplr
More informationThis Week. Computer Graphics. Introduction. Introduction. Graphics Maths by Example. Graphics Maths by Example
This Wk Computr Grphics Vctors nd Oprtions Vctor Arithmtic Gomtric Concpts Points, Lins nd Plns Eploiting Dot Products CSC 470 Computr Grphics 1 CSC 470 Computr Grphics 2 Introduction Introduction Wh do
More informationThe Wave Excitation Forces on a Floating Vertical Cylinder in Water of Infinite Depth
Th Wv Exctton Forcs on Flotng Vrtcl Cylnr n Wtr of Infnt Dpth Wll Fnngn, Mrtn Mr, J Goggns 3,* Collg of Engnrng n Infortcs, Ntonl Unvrsty of Irln, Glwy, Irln chool of Mthtcs, ttstcs n Appl Mthtcs, Ntonl
More informationRelate p and T at equilibrium between two phases. An open system where a new phase may form or a new component can be added
4.3, 4.4 Phas Equlbrum Dtrmn th slops of th f lns Rlat p and at qulbrum btwn two phass ts consdr th Gbbs functon dg η + V Appls to a homognous systm An opn systm whr a nw phas may form or a nw componnt
More informationLinear Algebra. Definition The inverse of an n by n matrix A is an n by n matrix B where, Properties of Matrix Inverse. Minors and cofactors
Dfnton Th nvr of an n by n atrx A an n by n atrx B whr, Not: nar Algbra Matrx Invron atrc on t hav an nvr. If a atrx ha an nvr, thn t call. Proprt of Matrx Invr. If A an nvrtbl atrx thn t nvr unqu.. (A
More informationA Probabilistic Characterization of Simulation Model Uncertainties
A Proalstc Charactrzaton of Sulaton Modl Uncrtants Vctor Ontvros Mohaad Modarrs Cntr for Rsk and Rlalty Unvrsty of Maryland 1 Introducton Thr s uncrtanty n odl prdctons as wll as uncrtanty n xprnts Th
More informationUNIT # 08 (PART - I)
. r. d[h d[h.5 7.5 mol L S d[o d[so UNIT # 8 (PRT - I CHEMICL INETICS EXERCISE # 6. d[ x [ x [ x. r [X[C ' [X [[B r '[ [B [C. r [NO [Cl. d[so d[h.5 5 mol L S d[nh d[nh. 5. 6. r [ [B r [x [y r' [x [y r'
More informationEconomics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization
THE UNIVERSITY OF MARYLAND COLLEGE PARK, MARYLAND Economcs 600: August, 007 Dynamc Part: Problm St 5 Problms on Dffrntal Equatons and Contnuous Tm Optmzaton Quston Solv th followng two dffrntal quatons.
More informationCSE 373: AVL trees. Warmup: Warmup. Interlude: Exploring the balance invariant. AVL Trees: Invariants. AVL tree invariants review
rmup CSE 7: AVL trs rmup: ht is n invrint? Mihl L Friy, Jn 9, 0 ht r th AVL tr invrints, xtly? Disuss with your nighor. AVL Trs: Invrints Intrlu: Exploring th ln invrint Cor i: xtr invrint to BSTs tht
More information167 T componnt oftforc on atom B can b drvd as: F B =, E =,K (, ) (.2) wr w av usd 2 = ( ) =2 (.3) T scond drvatv: 2 E = K (, ) = K (1, ) + 3 (.4).2.2
166 ppnd Valnc Forc Flds.1 Introducton Valnc forc lds ar usd to dscrb ntra-molcular ntractons n trms of 2-body, 3-body, and 4-body (and gr) ntractons. W mplmntd many popular functonal forms n our program..2
More informationADORO TE DEVOTE (Godhead Here in Hiding) te, stus bat mas, la te. in so non mor Je nunc. la in. tis. ne, su a. tum. tas: tur: tas: or: ni, ne, o:
R TE EVTE (dhd H Hdg) L / Mld Kbrd gú s v l m sl c m qu gs v nns V n P P rs l mul m d lud 7 súb Fí cón ví f f dó, cru gs,, j l f c r s m l qum t pr qud ct, us: ns,,,, cs, cut r l sns m / m fí hó sn sí
More informationElliptical motion, gravity, etc
FW Physics 130 G:\130 lctur\ch 13 Elliticl motion.docx g 1 of 7 11/3/010; 6:40 PM; Lst rintd 11/3/010 6:40:00 PM Fig. 1 Elliticl motion, grvity, tc minor xis mjor xis F 1 =A F =B C - D, mjor nd minor xs
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 informationLecture 23 APPLICATIONS OF FINITE ELEMENT METHOD TO SCALAR TRANSPORT PROBLEMS
COMPUTTION FUID DYNMICS: FVM: pplcatons to Scalar Transport Prolms ctur 3 PPICTIONS OF FINITE EEMENT METHOD TO SCR TRNSPORT PROBEMS 3. PPICTION OF FEM TO -D DIFFUSION PROBEM Consdr th stady stat dffuson
More informationSAMPLE CSc 340 EXAM QUESTIONS WITH SOLUTIONS: part 2
AMPLE C EXAM UETION WITH OLUTION: prt. It n sown tt l / wr.7888l. I Φ nots orul or pprotng t vlu o tn t n sown tt t trunton rror o ts pproton s o t or or so onstnts ; tt s Not tt / L Φ L.. Φ.. /. /.. Φ..787.
More informationFractions. Mathletics Instant Workbooks. Simplify. Copyright
Frctons Stunt Book - Srs H- Smplfy + Mthltcs Instnt Workbooks Copyrht Frctons Stunt Book - Srs H Contnts Topcs Topc - Equvlnt frctons Topc - Smplfyn frctons Topc - Propr frctons, mpropr frctons n mx numbrs
More informationperm4 A cnt 0 for for if A i 1 A i cnt cnt 1 cnt i j. j k. k l. i k. j l. i l
h 4D, 4th Rank, Antisytric nsor and th 4D Equivalnt to th Cross Product or Mor Fun with nsors!!! Richard R Shiffan Digital Graphics Assoc 8 Dunkirk Av LA, Ca 95 rrs@isidu his docunt dscribs th four dinsional
More informationMP IN BLOCK QUASI-INCOHERENT DICTIONARIES
CHOOL O ENGINEERING - TI IGNAL PROCEING INTITUTE Lornzo Potta and Prr Vandrghynst CH-1015 LAUANNE Tlphon: 4121 6932601 Tlfax: 4121 6937600 -mal: lornzo.potta@pfl.ch ÉCOLE POLYTECHNIQUE ÉDÉRALE DE LAUANNE
More informationLINEAR SYSTEMS THEORY
Introducton to Mdcl Engnrng INEAR SYSTEMS THEORY Ho Kyung Km, Ph.D. hoyung@pun.c.r School of Mchncl Engnrng Pun Ntonl Unvrty Evn / odd / prodc functon Thn bout con & n functon! Evn f - ; Odd f - -; d d
More informationLightening Summary of Fourier Analysis
Lghtnng Suary of Fourr Analyss D. Ad. Coponnts n Vctor Spacs You ar falar wth th fact that, n so vctor spac of your choosng, any vctor can b dcoposd nto coponnts along th drctons of so gvn bass: aˆ+ bj
More informationINF5820/INF9820 LANGUAGE TECHNOLOGICAL APPLICATIONS. Jan Tore Lønning, Lecture 4, 14 Sep
INF5820/INF9820 LANGUAGE TECHNOLOGICAL ALICATIONS Jn Tor Lønning Lctur 4 4 Sp. 206 tl@ii.uio.no Tody 2 Sttisticl chin trnsltion: Th noisy chnnl odl Word-bsd Trining IBM odl 3 SMT xpl 4 En kokk lgd n rtt
More informationLimits Indeterminate Forms and L Hospital s Rule
Limits Indtrmint Forms nd L Hospitl s Rul I Indtrmint Form o th Tp W hv prviousl studid its with th indtrmint orm s shown in th ollowin mpls: Empl : Empl : tn [Not: W us th ivn it ] Empl : 8 h 8 [Not:
More informationChapter 16. 1) is a particular point on the graph of the function. 1. y, where x y 1
Prctic qustions W now tht th prmtr p is dirctl rltd to th mplitud; thrfor, w cn find tht p. cos d [ sin ] sin sin Not: Evn though ou might not now how to find th prmtr in prt, it is lws dvisl to procd
More informationSection 5.1/5.2: Areas and Distances the Definite Integral
Scto./.: Ars d Dstcs th Dt Itgrl Sgm Notto Prctc HW rom Stwrt Ttook ot to hd p. #,, 9 p. 6 #,, 9- odd, - odd Th sum o trms,,, s wrtt s, whr th d o summto Empl : Fd th sum. Soluto: Th Dt Itgrl Suppos w
More informationLEBANESE UNIVERSITY FACULTY OF ENGINEERING
Entranc Exa 3 PHYSICS Duraton: H 8 JULY Exrcs I: [ pts] Study of th oton of a partcl Consdr a hollow crcular sld (C of radus 5 c and locatd n a vrtcal plan. A O partcl (S, of ass g, can sld on th nnr surfac
More information0 t b r 6, 20 t l nf r nt f th l t th t v t f th th lv, ntr t n t th l l l nd d p rt nt th t f ttr t n th p nt t th r f l nd d tr b t n. R v n n th r
n r t d n 20 22 0: T P bl D n, l d t z d http:.h th tr t. r pd l 0 t b r 6, 20 t l nf r nt f th l t th t v t f th th lv, ntr t n t th l l l nd d p rt nt th t f ttr t n th p nt t th r f l nd d tr b t n.
More informationLinear Algebra Existence of the determinant. Expansion according to a row.
Lir Algbr 2270 1 Existc of th dtrmit. Expsio ccordig to row. W dfi th dtrmit for 1 1 mtrics s dt([]) = (1) It is sy chck tht it stisfis D1)-D3). For y othr w dfi th dtrmit s follows. Assumig th dtrmit
More information2. Grundlegende Verfahren zur Übertragung digitaler Signale (Zusammenfassung) Informationstechnik Universität Ulm
. Grundlgnd Vrfahrn zur Übrtragung dgtalr Sgnal (Zusammnfassung) wt Dc. 5 Transmsson of Dgtal Sourc Sgnals Sourc COD SC COD MOD MOD CC dg RF s rado transmsson mdum Snk DC SC DC CC DM dg DM RF g physcal
More information4 4 N v b r t, 20 xpr n f th ll f th p p l t n p pr d. H ndr d nd th nd f t v L th n n f th pr v n f V ln, r dn nd l r thr n nt pr n, h r th ff r d nd
n r t d n 20 20 0 : 0 T P bl D n, l d t z d http:.h th tr t. r pd l 4 4 N v b r t, 20 xpr n f th ll f th p p l t n p pr d. H ndr d nd th nd f t v L th n n f th pr v n f V ln, r dn nd l r thr n nt pr n,
More informationLinear parameterization of group GL(N, C) A. Lavrenov.
nar paratrzaton of group G(N, ). avrnov E-a: ann99@a.ru bstract: nar paratrzaton of group G(N, ) ford by drct products of atrcs wth n advanc nown sytry proprts s offrd. Inta condtons of th gvn approach
More informationOutline. 1 Introduction. 2 Min-Cost Spanning Trees. 4 Example
Outlin Computr Sin 33 Computtion o Minimum-Cost Spnnin Trs Prim's Alorithm Introution Mik Joson Dprtmnt o Computr Sin Univrsity o Clry Ltur #33 3 Alorithm Gnrl Constrution Mik Joson (Univrsity o Clry)
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 information? plate in A G in
Proble (0 ponts): The plstc block shon s bonded to rgd support nd to vertcl plte to hch 0 kp lod P s ppled. Knong tht for the plstc used G = 50 ks, deterne the deflecton of the plte. Gven: G 50 ks, P 0
More information12/3/12. Outline. Part 10. Graphs. Circuits. Euler paths/circuits. Euler s bridge problem (Bridges of Konigsberg Problem)
12/3/12 Outlin Prt 10. Grphs CS 200 Algorithms n Dt Struturs Introution Trminology Implmnting Grphs Grph Trvrsls Topologil Sorting Shortst Pths Spnning Trs Minimum Spnning Trs Ciruits 1 Ciruits Cyl 2 Eulr
More informationDivided. diamonds. Mimic the look of facets in a bracelet that s deceptively deep RIGHT-ANGLE WEAVE. designed by Peggy Brinkman Matteliano
RIGHT-ANGLE WEAVE Dv mons Mm t look o ts n rlt tt s ptvly p sn y Py Brnkmn Mttlno Dv your mons nto trnls o two or our olors. FCT-SCON0216_BNB66 2012 Klm Pulsn Co. Ts mtrl my not rprou n ny orm wtout prmsson
More information5/9/13. Part 10. Graphs. Outline. Circuits. Introduction Terminology Implementing Graphs
Prt 10. Grphs CS 200 Algorithms n Dt Struturs 1 Introution Trminology Implmnting Grphs Outlin Grph Trvrsls Topologil Sorting Shortst Pths Spnning Trs Minimum Spnning Trs Ciruits 2 Ciruits Cyl A spil yl
More informationMathematics. Complex Number rectangular form. Quadratic equation. Quadratic equation. Complex number Functions: sinusoids. Differentiation Integration
Mathmatics Compl numbr Functions: sinusoids Sin function, cosin function Diffrntiation Intgration Quadratic quation Quadratic quations: a b c 0 Solution: b b 4ac a Eampl: 1 0 a= b=- c=1 4 1 1or 1 1 Quadratic
More information2008 AP Calculus BC Multiple Choice Exam
008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl
More informationCHAPTER 33: PARTICLE PHYSICS
Collg Physcs Studnt s Manual Chaptr 33 CHAPTER 33: PARTICLE PHYSICS 33. THE FOUR BASIC FORCES 4. (a) Fnd th rato of th strngths of th wak and lctromagntc forcs undr ordnary crcumstancs. (b) What dos that
More informationLecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9
Lctur contnts Bloch thorm -vctor Brillouin zon Almost fr-lctron modl Bnds ffctiv mss Hols Trnsltionl symmtry: Bloch thorm On-lctron Schrödingr qution ch stt cn ccommo up to lctrons: If Vr is priodic function:
More informationCIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7
CIVL / -D Boundr Vlu Prolms - Rctngulr Elmnts / RECANGULAR ELEMENS - In som pplictions, it m mor dsirl to us n lmntl rprsnttion of th domin tht hs four sids, ithr rctngulr or qudriltrl in shp. Considr
More informationUNIT 8 TWO-WAY ANOVA WITH m OBSERVATIONS PER CELL
UNIT 8 TWO-WAY ANOVA WITH OBSERVATIONS PER CELL Two-Way Anova wth Obsrvatons Pr Cll Structur 81 Introducton Obctvs 8 ANOVA Modl for Two-way Classfd Data wth Obsrvatons r Cll 83 Basc Assutons 84 Estaton
More informationERDOS-SMARANDACHE NUMBERS. Sabin Tabirca* Tatiana Tabirca**
ERDO-MARANDACHE NUMBER b Tbrc* Tt Tbrc** *Trslv Uvrsty of Brsov, Computr cc Dprtmt **Uvrsty of Mchstr, Computr cc Dprtmt Th strtg pot of ths rtcl s rprstd by rct work of Fch []. Bsd o two symptotc rsults
More informationCHARACTERIZATION AND MODELING OF INDOOR POWER-LINE COMMUNICATION CHANNELS
nd Cndn Solr Buldngs Confrnc Clgry, Jun 4, 7 CHARACTERIZATIO AD ODEIG OF IDOOR POWER-IE COUICATIO CHAES Xn Dng Unvrsty of w Brunswck Hd Hll, 5 Dnn Dr Frdrcton, B E3B 5A3 Tl: 5-45-9 El: o4n39@unbc Juln
More information, each of which is a tree, and whose roots r 1. , respectively, are children of r. Data Structures & File Management
nrl tr T is init st o on or mor nos suh tht thr is on sint no r, ll th root o T, n th rminin nos r prtition into n isjoint susts T, T,, T n, h o whih is tr, n whos roots r, r,, r n, rsptivly, r hilrn o
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS
VSRT MEMO #05 MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS 01886 Fbrury 3, 009 Tlphon: 781-981-507 Fx: 781-981-0590 To: VSRT Group From: Aln E.E. Rogrs Subjct: Simplifid
More information