Symmetry breaking effects of toroidicity on toroidal momentum transport. Abstract

Size: px
Start display at page:

Download "Symmetry breaking effects of toroidicity on toroidal momentum transport. Abstract"

Transcription

1 Symmy bakg ffcs of oodcy o oodal momum aso. TH/8.9 J. Wlad, R. Sg, H. Nodma,. Kaw, A.G. s ad D. Sz. Dam of Rado ad Sac Scc, Calms. vsy of Tcology ad Euaom-VR Assocao, S96 Gobug, Swd. Isu fo lasma Rsac, a Gadaga 8 8, Ida. C fo Fuso, Sac ad Asoyscs, yscs dam, vsy of Wawck, CV 7AL, Covy K. Dam of Elccal ad Comu Egg, Naoal Tccal vsy of As, GR-57 7 As, Gc, Assocao Euaom Hllc Rulc Absac A dvao of symmy bakg oodcy ffcs o oodal momum aso as b mad fom sss so. Ts ffc s usually sog a symmy bakg causd by flows mslvs o gfuco. T modl obad galzs a c dvao of dagoal aso lms fom sss so o covcv lms of ubul quao o molcc ys. Ts gvs ossbly fo ao of sam y of ffcs vously obad fom a as sac cosvg ola gyokc quao,.

2 . Ioduco T s s momum aso -8 as cly focusd o symmy bakg ffcs,,7 o oodal momum aso. T fs ffc of s y was dfd, as ffc of a asymmc g-fuco o avag of aalll mod umb s dd of aalll momum aso. Fo accal uoss w may aoxma oodal momum by aalll momum. Rcly also symmy bakg ffcs of oodcy w foud 7. Fo a movd udsadg of suc ffcs ad fo a coss dvao of flud quaos fo momum aso s gly dsabl o also mak flud dvao of suc ffcs. Sc magc df s o a flud df suc ffcs ogas fom sss so flud quaos. W a us facd w a comlcad ask of cludg magc cuvau ffcs fom sss so. O o ad gyokc dvaos av o sa fom a as sac cosvg fomulao 9 of gyokc quao. Tus qu ambos aoacs a dd bo gyokc 7, 8 ad flud dvaos. T flud dvao s, owv, mo sag fowad, sowg sg of flud oy dvg advacd dyamc quaos. T sss so s moa maly fo low fqucy oma magzd lasmas. I was alady usd fo dvg dagoal magc df ms. I collsolss cas sss so cobuos a assocad w f gyoadus ffcs fo moo dcula o magc, fld. H fs suls cludd gyo vscous cacllaos bw covcv damagc ffcs. A s m also kc calculaos fo df ad MHD y mods ad jus sad ad full Vlasov dscos w smlfd gomy w usd. T agm fo lows od FLR ffc bw flud ad kc dvaos, could us b gadd as a sgfca acvm a s m. Wl FLR ffc, fo dcula moo s obad oug a xaso ao of caacsc mod fqucy ad cycloo fqucy, ad us usually ad as small, oodal ffcs fom sss so as od ε L / R aalll momum quao. Aloug ε ca b ad small dg ad s ycally of od co. Tus s ffc s moa fo aalll moo. A sml way o oba dagoal cuvau ffcs s o dv quaos of moo fo gudg cs gyo flud quao. Suc quaos av magc dfs cludd as gudg c dfs ad quao of moo ca b obad by akg moms of a gyo kc quao. T dagoal cuvau ms aa as du o a covcv magc df sum of gad ad cuvau ms w a faco as a covco of aalll momum flow. I s wok w wll sa fom agsk flud quao ad dv symmy bakg ffcs cosodg o Rf. 7, usg ly flud quaos fo oodal o mau gad mod ITG. II. Toodal momum flow T gal momum quao s obad fom o ad lco momum quaos ad couy quao:

3 v mn N E N E a b N N S c H s o sss so gv by agsk 7 s adx ad S s dsy souc m. W us galzd co-oda sysm ˆ, bˆ, ˆ wc s d o magc fld. H ˆ / s u vco alog magc fld ls, ˆ s oogoal o magc sufac, ad bˆ ˆ ˆ. T co-odas basc ˆ, bˆ, ˆ a lad o flux co-odas,,, w s olodal magc flux, galzd olodal agl ad s oodal agl. o co-odas sysm a lad as ˆ ˆ, bˆ ˆ ˆ, ˆ ˆ ˆ Fo lag asc ao ε / R << ad oodal symmy.., /, dffal oaos ca b w as: ˆ ˆ ~ ~ L ~ qr, θ ˆ b ~ qr ~ θ H /, J, J, Jacoba of asfomao,,, ν / ~ / R, c of fld ls, q ν d, safy faco ad fo lag asc ao ε / R <, R ε cos ad ε cos, w ad R mo ad majo ad, scvly. T sum of oodal comos of Eqs a ad b ca b w as: ~ mn ˆ ˆ J c W las m cosods o adal agula momum flux dv by backgoud ubulc ad ˆ.

4 Fo oodal symmy.., /, covcv m Eq. 8 ca b xssd as: Nˆ [ ] [ N N ] N l N N 5 y usg Eq. 5 ad couy quao, oal dvav of momum dsy lf ad sd of Eq. ca b xssd as: N mnˆ [ ] m N N N m N N mn l N m S m N N mn l 6 H w av mad us of a soal lao ˆ ˆ l o ˆ ˆ l, ˆ ˆ, ˆ ˆ ad S s acl souc m. No fom Adx A, dfo of s of fom αβ βα, sss foc alog oodal dco ca asly b xssd as: 7 ˆ αβ αβ αβ αβ J W cosd a lasma s collsolss gm qrν / c <, ν s o collso fqucy. W ow collc oly ad fom collsolss sss so Adx A. b b b b b b [ b κ b ]

5 [ ] l m c S m N N N m m N [ ] ˆ m c m c θ θ θ w κ H / < s assumd ad Ω /,,. Aga low β ad lag asc ao lm, m ˆ ow ca b xssd as : 8 w w usd b b b κ, κ ad aalogously fo. y usg quaos 6 ad 8 quao, oodal momum quao ca ow b xssd as 9 W ow fs dv la aalll o vlocy ubao fom Eq.9. I lm kl >> k s dcula wav vco of backgoud sably, ad by akg ubaos F F f δ [ F ad f δ a backgoud qulbum ad ubao, scvly], la fom of Eq. 9 ca b xssd as: [ ] D D E J c N T m u m N θ δ δ [ ] κ

6 H D ct T, D D ˆ / ad T. I Eq cuvau m volvg cosods o ubul quao TE T cuvau m volvg δ as wo as w mau uao a cosods o molcc covcv m. If w assum olzma lcos ad quasualy w ca w as: mn θ J c E D δu m D [ ][ δ T N ] T τ Tus ow dsy ubao a adds u o TE a ad w cov Cools c of Rf 8 af subsug δu o flux Γ < v u >. W m N < θ c < J > > m N < δu δu m N > D < δu δ E δ av oly a faco sc ou D cluds a faco makg quval o oal magc df fo low ß. Ts a ca also b covd fom Rf 9 w, owv, mo ffo was mad o saa cuvau ad gad as as wll as cludg mau asooy. T ogal TE a coms fom covcv al m,.. m backs Eq 9. W o fom way Eq. was w a oodal cuvau ffc adds u as a w symmy bakg ffc o aalll gad. Ts cass subsaally ffc of flowsa. W ca ow fomally galz gvalu soluo Rf. 8 by addg w symmy bakg m o aalll gad. Howv, also symmy o adal dco wll b sfd du o oodcy. Fom Eq. 9, quao fo ma oodal vlocy ca b obad by avagg ov magc flux sufacs. I lag asc ao lm, quao fo ma ca b w: > m N δ D δu I dvg Eq w k oly cuvau ms fom sss so. W o a w av cobuos bo fom Ryolds sss al a ad fom sss so.

7 AENDIX A: THE STRESS TENSORS I lm ν / <<, sss so 7 ca b sl o as Ω,,, A T aalll sss so o dagoal max, gyo-sss so, ad dcula sss so a gv as 8, T aalll sss so: I ˆˆ ˆ ˆ T gyo sss so: { ˆˆ bb ˆˆ[ bˆ ˆ ˆ bˆ] b ˆ ˆ b ˆ ˆ [ ˆ ˆ bˆ bˆ] }, { ˆˆ ˆˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ b b b b } A,, A [ ] [ ] T dcula sss so:,, A [.. ] [.. ] w { ˆˆ bb ˆˆ[ ˆ. ˆ bˆ. bˆ] b ˆ ˆ b ˆ ˆ [ ˆ. bˆ bˆ. ˆ ]} { ˆˆ ˆˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ b b b b },,. 96ν, dx - ad - f o agsk s coffcs 7, / Ω, ν / Ω, ad. Rfc. J.E. Rc, E.S. Mama, F. ombada ad L. Qu, Nucla Fuso 7, X. Gab, Y. Saaz,. Gdc, S. kadda,. y, C. Fgalla ad I Voskovc, ys. lasmas 9, 89.. J.S. dgass, K.H. ull, L.R. aylo, W. Houlbg ad J. Lo, ys. lasmas,.. A.G. s ad C. Ago, ys. lasmas, C. dvs, K.M. Raamäk, C. Goud, E. As, G. Coga, A. Eksso, M. dgf, I. Jks, H.C.M. Koos,. Maca, H. Nodma,. Sad, T.

8 TALA, J. Wlad, K-D Zasow ad JET-EFDA cobuos, lasma ys. Cool. Fuso 8, J. Wlad, A. Eksso, H. Nodma ad A. Zagoody, ys. lasmas, T.S. Ham,.H. Damod, O.D. Guca ad G. Rwold, ys. lasmas, A. G. s, C. Ago ad D. Sz, ys. Rv. L. 98, 65 7.; A.G. s, D. Sz, Y. Cam al, yscs of lasmas, o b ublsd. 9. T. S. Ham, ys. Fluds, D. Sz, A.G. s ad J. Wlad, ys. lasmas 5, R.E. Walz, R.R. Domguz ad G.W. Hamm, ys. Fluds, K.V. Robs ad J.. Taylo, ys. Rv. L. 8, M.N. Rosblu, N.A. Kall ad N. Rosok, Nucl. Fuso Sul., 96.. A. Rogs, ys. lasmas 7, J.J. Ramos, ys lasmas, J.J. Ramos, ys. lasmas, H.A. Class, H. Gaus, A. Rogs ad C. Yam, ys. lasmas 7, J. Wlad ad H. Nodma, ocdgs of d ES cofc, Rom 6, ECA Vol., -, 86.

k of the incident wave) will be greater t is too small to satisfy the required kinematics boundary condition, (19)

k of the incident wave) will be greater t is too small to satisfy the required kinematics boundary condition, (19) TOTAL INTRNAL RFLTION Kmacs pops Sc h vcos a coplaa, l s cosd h cd pla cocds wh h X pla; hc 0. y y y osd h cas whch h lgh s cd fom h mdum of hgh dx of faco >. Fo cd agls ga ha h ccal agl s 1 ( /, h hooal

More information

Anouncements. Conjugate Gradients. Steepest Descent. Outline. Steepest Descent. Steepest Descent

Anouncements. 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 information

Phys Nov. 3, 2017 Today s Topics. Continue Chapter 2: Electromagnetic Theory, Photons, and Light Reading for Next Time

Phys Nov. 3, 2017 Today s Topics. Continue Chapter 2: Electromagnetic Theory, Photons, and Light Reading for Next Time Phys 31. No. 3, 17 Today s Topcs Cou Chap : lcomagc Thoy, Phoos, ad Lgh Radg fo Nx Tm 1 By Wdsday: Radg hs Wk Fsh Fowls Ch. (.3.11 Polazao Thoy, Jos Macs, Fsl uaos ad Bws s Agl Homwok hs Wk Chap Homwok

More information

Lecture Y4: Computational Optics I

Lecture Y4: Computational Optics I Phooc ad opolcoc chologs DPMS: Advacd Maals Udsadg lgh ma acos s cucal fo w applcaos Lcu Y4: Compuaoal Opcs I lfos Ldoks Room Π, 65 746 ldok@cc.uo.g hp://cmsl.maals.uo.g/ldoks Rflco ad faco Toal al flco

More information

ELECTROMAGNETISM, NUCLEAR STRUCTURES & GRAVITATION

ELECTROMAGNETISM, 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 information

The far field calculation: Approximate and exact solutions. Persa Kyritsi November 10th, 2005 B2-109

The far field calculation: Approximate and exact solutions. Persa Kyritsi November 10th, 2005 B2-109 Th fa fl calculao: Appoa a ac oluo Pa K Novb 0h 005 B-09 Oul Novb 0h 005 Pa K Iouco Appoa oluo flco fo h gou ac oluo Cocluo Pla wav fo Ic fl: pla wav k ( ) jk H ( ) λ λ ( ) Polaao fo η 0 0 Hooal polaao

More information

By Joonghoe Dho. The irradiance at P is given by

By Joonghoe Dho. The irradiance at P is given by CH. 9 c CH. 9 c By Joogo Do 9 Gal Coao 9. Gal Coao L co wo po ouc, S & S, mg moocomac wav o am qucy. L paao a b muc ga a. Loca am qucy. L paao a b muc ga a. Loca po obvao P a oug away om ouc o a a P wavo

More information

Convolution of Generated Random Variable from. Exponential Distribution with Stabilizer Constant

Convolution of Generated Random Variable from. Exponential Distribution with Stabilizer Constant Appld Mamacal Scc Vol 9 5 o 9 78-789 HIKARI Ld wwwm-acom p://dxdoog/988/am5559 Covoluo of Gad Radom Vaabl fom Expoal Dbuo w Sablz Coa Dod Dvao Maa Lufaa Oaa ad Maa Aa Dpam of Mamac Facul of Mamac ad Naual

More information

Lecture 12: Introduction to nonlinear optics II.

Lecture 12: Introduction to nonlinear optics II. Lcur : Iroduco o olar opcs II r Kužl ropagao of srog opc sgals propr olar ffcs Scod ordr ffcs! Thr-wav mxg has machg codo! Scod harmoc grao! Sum frqucy grao! aramrc grao Thrd ordr ffcs! Four-wav mxg! Opcal

More information

Heat Transfer in Unsteady Axisymmetric Rotational Flow of Oldroyd Liquid

Heat Transfer in Unsteady Axisymmetric Rotational Flow of Oldroyd Liquid aoal Joual of Scfc & Egg Rsach Volum, ssu 9, Smb-0 SSN 9-558 Ha Tasf Usady Axsymmc Roaoal Flow of Oldoyd Lqud A. Msha, G. S. Ray, S. Bswal Absac - Ths a dals wh h sudy of ha asf usady axsymmc oaoal flow

More information

Part I- Wave Reflection and Transmission at Normal Incident. Part II- Wave Reflection and Transmission at Oblique Incident

Part I- Wave Reflection and Transmission at Normal Incident. Part II- Wave Reflection and Transmission at Oblique Incident Apl 6, 3 Uboudd Mda Gudd Mda Chap 7 Chap 8 3 mls 3 o 3 M F bad Lgh wavs md by h su Pa I- Wav Rlo ad Tasmsso a Nomal Id Pa II- Wav Rlo ad Tasmsso a Oblqu Id Pa III- Gal Rlao Bw ad Wavguds ad Cavy Rsoao

More information

Boyce/DiPrima 9 th ed, Ch 7.6: Complex Eigenvalues

Boyce/DiPrima 9 th ed, Ch 7.6: Complex Eigenvalues BocDPm 9 h d Ch 7.6: Compl Egvlus Elm Dffl Equos d Boud Vlu Poblms 9 h do b Wllm E. Boc d Rchd C. DPm 9 b Joh Wl & Sos Ic. W cosd g homogous ssm of fs od l quos wh cos l coffcs d hus h ssm c b w s ' A

More information

A 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 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 information

Mathematical Model of Acceleration Stage of Magnetic Inductive Pulsed Plasma Thruster

Mathematical Model of Acceleration Stage of Magnetic Inductive Pulsed Plasma Thruster Mahacal Modl of Acclao Sag of Magc ducv Pulsd Plasa Thus EPC--76 Psd a h d aoal Elcc Poulso Cofc, Wsbad Gay Sb 5, Haf Daas Salh ad Sgy Yuyovch so aoal Aosac Uvsy (Khav Avao su), Khav, 67, Ua, Chalova,

More information

Existence of Nonoscillatory Solutions for a Class of N-order Neutral Differential Systems

Existence of Nonoscillatory Solutions for a Class of N-order Neutral Differential Systems Vo 3 No Mod Appd Scc Exsc of Nooscaoy Souos fo a Cass of N-od Nua Dffa Sysms Zhb Ch & Apg Zhag Dpam of Ifomao Egg Hua Uvsy of Tchoogy Hua 4 Cha E-ma: chzhbb@63com Th sach s facd by Hua Povc aua sccs fud

More information

Chapter 5 Transmission Lines

Chapter 5 Transmission Lines ap 5 ao 5- aacc of ao ao l: a o cou ca cu o uppo a M av c M o qua-m o. Fo M o a H M H a M a µ M. cu a M av av ff caacc. A M av popaa o ff lcc a paal flco a paal ao ll occu. A ob follo ul. ll la: p a β

More information

Quantum Harmonic Oscillator

Quantum Harmonic Oscillator Quu roc Oscllor Quu roc Oscllor 6 Quu Mccs Prof. Y. F. C Quu roc Oscllor Quu roc Oscllor D S..O.:lr rsorg forc F k, k s forc cos & prbolc pol. V k A prcl oscllg roc pol roc pol s u po of sbly sys 6 Quu

More information

Mean Estimation with Imputation in Two- Phase Sampling

Mean Estimation with Imputation in Two- Phase Sampling Iaoal Joual of o gg sac (IJ) www.jm.com ol. Issu.5 p-oc. 0 pp-56-5 I: 4-6645 a smao w Impuao wo- Pas amplg aa g au Kalpaa aav aa Paa * fo amacal ccs () aasal Uvsaasal ajasa * pam of amacs a ascs. H.. Gou

More information

Multi-fluid magnetohydrodynamics in the solar atmosphere

Multi-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 information

Primary Contact Number: (Last) (First) (Please list a number where we can reach you 24/7) State: Zip Code: Parent/Guardian Demographic

Primary Contact Number: (Last) (First) (Please list a number where we can reach you 24/7) State: Zip Code: Parent/Guardian Demographic Pf Appco & H Rco Fom mus b f ou o vw sg c y fo ppc o b offcy cogz Poomc Cofc Pf Appc s Dmogpc (Ps P) Nm: Pmy Coc Numb: (Ls) (Fs) (Ps s umb w w c c you 24/7) Ass: DOB: E-M: Cy: Scoo: S: Zp Co: Po: G: P/Gu

More information

ANALYTICAL TREATMENT OF THE THREE-DIMENSIONAL MODEL OF STIMULATED BRILLOUIN SCATTERING WITH AXIAL SYMMETRIC PUMP WAVE

ANALYTICAL TREATMENT OF THE THREE-DIMENSIONAL MODEL OF STIMULATED BRILLOUIN SCATTERING WITH AXIAL SYMMETRIC PUMP WAVE Joual of Oolos ad Advad Maals Vol. No. mb. 58-59 ANAYTCA TRATMNT OF TH THR-DMNONA MOD OF TMUATD ROUN CATTRNG TH AXA YMMTRC UM AV V.. Vlad V. ab a A. Moofasu su of Aom hyss NR-D.ass ad Th Romaa Aadmy-CA

More information

Assessing Student Work MATH RUBRIC. Understanding Reasoning Accuracy Communication

Assessing Student Work MATH RUBRIC. Understanding Reasoning Accuracy Communication Assssg Sud Wk MATH RUBRIC E x 4 P a 3 A 2 N v 1 Udsadg Rasg Auay Cmmua Uss wful ad hugh Th dus a sags ladg dly gazd hughu ad ffv slus. asly fllwd by hs. Exls, aalyzs, ad All fas ad alulas jusfs all lams

More information

Get Funky this Christmas Season with the Crew from Chunky Custard

Get Funky this Christmas Season with the Crew from Chunky Custard Hol Gd Chcllo Adld o Hdly Fdy d Sudy Nhs Novb Dcb 2010 7p 11.30p G Fuky hs Chss Sso wh h Cw fo Chuky Cusd Fdy Nhs $99pp Sudy Nhs $115pp Tck pc cluds: Full Chss d buff, 4.5 hou bv pck, o sop. Ts & Codos

More information

NLO Basics. Bulk Second Harmonic Generation Examples. QuartzQ ZnO bulk and nanowires Organic nanowires

NLO Basics. Bulk Second Harmonic Generation Examples. QuartzQ ZnO bulk and nanowires Organic nanowires NLO Bascs Bul Scod Hamoc Gao xampls QuaQ ZO bul ad aows Ogac aows Ahamoc Poals U U- P χ χ χ Io P lco pah P Wav quao : quaos Maxwlls D J H B : chags f No 4 H B J D B μ ρ ρ s. : chags f No H H B J μ μ ρ

More information

Gauge Theories. Elementary Particle Physics Strong Interaction Fenomenology. Diego Bettoni Academic year

Gauge Theories. Elementary Particle Physics Strong Interaction Fenomenology. Diego Bettoni Academic year Gau Thors Elmary Parcl Physcs Sro Iraco Fomoloy o Bo cadmc yar - Gau Ivarac Gau Ivarac Whr do Laraas or Hamloas com from? How do w kow ha a cra raco should dscrb a acual hyscal sysm? Why s h lcromac raco

More information

Chapter 5. Long Waves

Chapter 5. Long Waves ape 5. Lo Waes Wae e s o compaed ae dep: < < L π Fom ea ae eo o s s ; amos ozoa moo z p s ; dosac pesse Dep-aeaed coseao o mass

More information

Almost unbiased exponential estimator for the finite population mean

Almost unbiased exponential estimator for the finite population mean Almos ubasd poal smaor for f populao ma Rajs Sg, Pakaj aua, ad rmala Saa, Scool of Sascs, DAVV, Idor (M.P., Ida (rsgsa@aoo.com Flor Smaradac ar of Dparm of Mamacs, Uvrs of Mco, Gallup, USA (smarad@um.du

More information

Convection in a Differentially Heated Narrow Slot By Teja Muppirala Advisor: Dr. Cho Lik Chan. University of Arizona, Spring/Summer 2002

Convection in a Differentially Heated Narrow Slot By Teja Muppirala Advisor: Dr. Cho Lik Chan. University of Arizona, Spring/Summer 2002 Coco a Dffall Ha Naow Slo ja ala so: D. Co k Ca Us of zoa S/S Coco a ffall a aow slo of fl ca sla a ff s of bao o os of fl a os of slo. basc cl s a fl a o wall wll s o s cas a a fl a cool wall wll fall.

More information

Posterior analysis of the compound truncated Weibull under different loss functions for censored data.

Posterior analysis of the compound truncated Weibull under different loss functions for censored data. INRNAIONA JOURNA OF MAHMAIC AND COMUR IN IMUAION Vou 6 oso yss of h oou u Wu u ff oss fuos fo so. Khw BOUDJRDA Ass CHADI Ho FAG. As I hs h Bys yss of gh u Wu suo s os u y II so. Bys sos osog ss hv v usg

More information

Two-Dimensional Quantum Harmonic Oscillator

Two-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 information

11/8/2002 CS 258 HW 2

11/8/2002 CS 258 HW 2 /8/ CS 58 HW. G o a a qc of aa h < fo a I o goa o co a C cc c F ch ha F fo a I A If cc - c a co h aoa coo o ho o choo h o qc? I o g o -coa o o-coa? W ca choo h o qc o h a a h aa a. Tha f o o a h o h a:.

More information

RAKE Receiver with Adaptive Interference Cancellers for a DS-CDMA System in Multipath Fading Channels

RAKE Receiver with Adaptive Interference Cancellers for a DS-CDMA System in Multipath Fading Channels AKE v wh Apv f Cs fo DS-CDMA Ss Muph Fg Chs JooHu Y Su M EEE JHog M EEE Shoo of E Egg Sou o Uvs Sh-og Gw-gu Sou 5-74 Ko E-: ohu@su As hs pp pv AKE v wh vs og s popos fo DS-CDMA ss uph fg hs h popos pv

More information

T h e C S E T I P r o j e c t

T 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 information

Linear Perturbation Bounds of the Continuous-Time LMI-Based H Quadratic Stability Problem for Descriptor Systems

Linear Perturbation Bounds of the Continuous-Time LMI-Based H Quadratic Stability Problem for Descriptor Systems UGRN DE OF ENE ERNE ND NFORON EHNOOGE Volu No 4 ofa a ubao ouds of h ouous- -asd H uadac ably obl fo Dscpo yss dy ochv chcal Uvsy of ofa Faculy of uoacs Dpa of yss ad ool 756 ofa Eal ayochv@u-sofa.bg bsac

More information

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines Ogs of Quatu Thoy Masuts of sso of lght (EM adato) fo (H) atos foud dsct ls 5 4 Abl to ft to followg ss psso ν R λ c λwavlgth, νfqucy, cspd lght RRydbg Costat (~09,7677.58c - ),,, +, +,..g.,,.6, 0.6, (Lya

More information

Kinematics. Redundancy. Task Redundancy. Operational Coordinates. Generalized Coordinates. m task. Manipulator. Operational point

Kinematics. Redundancy. Task Redundancy. Operational Coordinates. Generalized Coordinates. m task. Manipulator. Operational point Mapulato smatc Jot Revolute Jot Kematcs Base Lks: movg lk fed lk Ed-Effecto Jots: Revolute ( DOF) smatc ( DOF) Geealzed Coodates Opeatoal Coodates O : Opeatoal pot 5 costats 6 paametes { postos oetatos

More information

9.6 Spherical Wave Solutions of the Scalar. Chapter 9: Radiating Systems, Multipole Fields and Radiation

9.6 Spherical Wave Solutions of the Scalar. Chapter 9: Radiating Systems, Multipole Fields and Radiation Cha 9: Raag Syss, Muo Fs a Raao A Ovvw of Chas o EM Wavs :(ov hs ous sou wav quao bouay Ch. 7 o a wav sa o wo s- sas saa by h - y a Ch. 8 o oug was - Ch. 9 J, ~ ougog g wav o sb, as a aa - Ch. J, ~ ougog

More information

Non-Equidistant Multi-Variable Optimum Model with Fractional Order Accumulation Based on Vector Continued Fractions Theory and its Application

Non-Equidistant Multi-Variable Optimum Model with Fractional Order Accumulation Based on Vector Continued Fractions Theory and its Application QIYUN IU NON-EQUIDISN MUI-VRIE OPIMUM MODE WIH FRCION ORDER... No-Equds Mu-V Ou Mod w Fco Od ccuuo sd o Vco Coud Fcos o d s co Qu IU * D YU. S oo o dcd Dsg d Mucu o Vc od Hu Us Cgs Hu 8 C. Cog o Mcc Egg

More information

Dr. Junchao Xia Center of Biophysics and Computational Biology. Fall /21/2016 1/23

Dr. Junchao Xia Center of Biophysics and Computational Biology. Fall /21/2016 1/23 BIO53 Bosascs Lcur 04: Cral Lm Thorm ad Thr Dsrbuos Drvd from h Normal Dsrbuo Dr. Juchao a Cr of Bophyscs ad Compuaoal Bology Fall 06 906 3 Iroduco I hs lcur w wll alk abou ma cocps as lsd blow, pcd valu

More information

Let's revisit conditional probability, where the event M is expressed in terms of the random variable. P Ax x x = =

Let's revisit conditional probability, where the event M is expressed in terms of the random variable. P Ax x x = = L's rvs codol rol whr h v M s rssd rs o h rdo vrl. L { M } rrr v such h { M } Assu. { } { A M} { A { } } M < { } { } A u { } { } { A} { A} ( A) ( A) { A} A A { A } hs llows us o cosdr h cs wh M { } [ (

More information

8. Queueing systems. Contents. Simple teletraffic model. Pure queueing system

8. Queueing systems. Contents. Simple teletraffic model. Pure queueing system 8. Quug sysms Cos 8. Quug sysms Rfrshr: Sml lraffc modl Quug dscl M/M/ srvr wag lacs Alcao o ack lvl modllg of daa raffc M/M/ srvrs wag lacs lc8. S-38.45 Iroduco o Tlraffc Thory Srg 5 8. Quug sysms 8.

More information

Emigration The movement of individuals out of an area The population decreases

Emigration 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 information

THIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.

THIS 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 information

Handout on. Crystal Symmetries and Energy Bands

Handout 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 information

( V ) 0 in the above equation, but retained to keep the complete vector identity for V in equation.

( V ) 0 in the above equation, but retained to keep the complete vector identity for V in equation. Cuvlna Coodnats Outln:. Otogonal cuvlna coodnat systms. Dffntal opatos n otogonal cuvlna coodnat systms. Dvatvs of t unt vctos n otogonal cuvlna coodnat systms 4. Incompssbl N-S quatons n otogonal cuvlna

More information

Lecture 7 Diffusion. Our fluid equations that we developed before are: v t v mn t

Lecture 7 Diffusion. Our fluid equations that we developed before are: v t v mn t Cla ot fo EE6318/Phy 6383 Spg 001 Th doumt fo tutoal u oly ad may ot b opd o dtbutd outd of EE6318/Phy 6383 tu 7 Dffuo Ou flud quato that w dvlopd bfo a: f ( )+ v v m + v v M m v f P+ q E+ v B 13 1 4 34

More information

Bayesian Estimation of the parameters of the Weibull-Weibull Length-Biased mixture distributions using time censored data

Bayesian Estimation of the parameters of the Weibull-Weibull Length-Biased mixture distributions using time censored data Bys Eso of h s of h Wull-Wull gh-bs xu suos usg so S. A. Sh N Bouss I.S.S. Co Uvsy I.N.P.S. Algs Uvsy shsh@yhoo.o ou005@yhoo.o As I hs h s of h Wull-Wull lgh s xu suos s usg h Gs slg hqu u y I sog sh.

More information

Motion Control Systems Chapter 1

Motion Control Systems Chapter 1 Asf Šboć Kouh Ohsh Moo Cool Syss Chp Elcochcl Syss Dycs Moo Cool Syss Asf Šboć Kouh Ohsh 0 oh Wly Sos (As) P Bsc us Mchcl Syss Poso locy Foc wok Mou x F F ( xx ) p p x x W F Fx x x Kc gy Pol gy ol gy xx

More information

6.012 Electronic Devices and Circuits Formula Sheet for Final Exam, Fall q = 1.6x10 19 Coul III IV V = x10 14 o. = 3.

6.012 Electronic Devices and Circuits Formula Sheet for Final Exam, Fall q = 1.6x10 19 Coul III IV V = x10 14 o. = 3. 6.0 Elctc Dvcs ad Ccuts ula Sht f al Exa, all 003 Paat Valus: Pdc Tabl: q.6x0 9 Cul III IV V 8.854 x0 4 /c,,s.7,,so 3.9 B C N 0 S /c, SO 3.5 x0 3 /c Al S P [S@R.T] 0 0 c 3 Ga G As /q 0.05 V ; ( /q) l0

More information

Least squares and motion. Nuno Vasconcelos ECE Department, UCSD

Least squares and motion. Nuno Vasconcelos ECE Department, UCSD Las squars ad moo uo Vascoclos ECE Dparm UCSD Pla for oda oda w wll dscuss moo smao hs s rsg wo was moo s vr usful as a cu for rcogo sgmao comprsso c. s a gra ampl of las squars problm w wll also wrap

More information

Ch. 22: Classical Theory of Harmonic Crystal

Ch. 22: Classical Theory of Harmonic Crystal C. : Clssl Toy o mo Cysl gl o ml moo o o os l s ld o ls o pl ollowg:. Eqlbm Pops p o ls d Islos Eqlbm sy d Cos Egs Tml Epso d lg. Tspo Pops T pd o lo Tm Fl o Wdm-Fz Lw pody Tml Cody o Islos Tsmsso o od.

More information

A KAM theorem for generalized Hamiltonian systems without action-angle variables

A KAM theorem for generalized Hamiltonian systems without action-angle variables ho fo gald aloa sss whou ao-agl vaabls Yo u Jo u wa Jog : aual L UG Uvs Pogag oa Popl s publ of oa : Faul of ahas L UG Uvs Pogag oa Popl s publ of oa bsa povd a ho o s of vaa o gald aloa sss whou ao-agl

More information

5- Scattering Stationary States

5- Scattering Stationary States Lctu 19 Pyscs Dpatmnt Yamou Unvsty 1163 Ibd Jodan Pys. 441: Nucla Pyscs 1 Pobablty Cunts D. Ndal Esadat ttp://ctaps.yu.du.jo/pyscs/couss/pys641/lc5-3 5- Scattng Statonay Stats Rfnc: Paagaps B and C Quantum

More information

Control Systems (Lecture note #6)

Control Systems (Lecture note #6) 6.5 Corol Sysms (Lcur o #6 Las Tm: Lar algbra rw Lar algbrac quaos soluos Paramrzao of all soluos Smlary rasformao: compao form Egalus ad gcors dagoal form bg pcur: o brach of h cours Vcor spacs marcs

More information

International Journal of Scientific & Engineering Research, Volume 7, Issue 5, May-2016 ISSN The Maximum Eccentricity Energy of a Graph

International Journal of Scientific & Engineering Research, Volume 7, Issue 5, May-2016 ISSN The Maximum Eccentricity Energy of a Graph Iaoa Joa of cfc & Egg Rsach Vom 7 Iss 5 ay6 IN 955 5 Th axmm Ecccy Egy of a Gaph Ahmd Na ad N D o Absac I Ths pap w odc h cocp of a maxmm cccy max oba som coffcs of h chaacsc poyoma of a cocd gaph G ad

More information

Chap 2: Reliability and Availability Models

Chap 2: Reliability and Availability Models Chap : lably ad valably Modls lably = prob{s s fully fucog [,]} Suppos from [,] m prod, w masur ou of N compos, of whch N : # of compos oprag corrcly a m N f : # of compos whch hav fald a m rlably of h

More information

, k fftw ' et i 7. " W I T H M A. L I O E T O W A R 3 D JSrOKTE X l S T E O H A R I T Y F O R A L L. FIRE AT^ 10N1A, foerohlng * M».

, k fftw ' et i 7.  W I T H M A. L I O E T O W A R 3 D JSrOKTE X l S T E O H A R I T Y F O R A L L. FIRE AT^ 10N1A, foerohlng * M». VOZ O } 0U OY? V O O O O R 3 D SO X S O R Y F O R 59 VO O OUY URY 2 494 O 3 S? SOS OU 0 S z S $500 $450 $350 S U R Y Sz Y 50 300 @ 200 O 200 @ $60 0 G 200 @ $50 S RGS OYS SSS D DRS SOS YU O R D G Y F!

More information

The Linear Regression Of Weighted Segments

The Linear Regression Of Weighted Segments The Lear Regresso Of Weghed Segmes George Dael Maeescu Absrac. We proposed a regresso model where he depede varable s made o up of pos bu segmes. Ths suao correspods o he markes hroughou he da are observed

More information

University of Toronto. Final Exam

University of Toronto. Final Exam University of Toronto Final Exam Date - Dec 16, 013 Duration:.5 hrs ECE331 Electronic Circuits Lecturer - D. Johns ANSWER QUESTIONS ON THESE SHEETS USING BACKS IF NECESSARY 1. Equation sheet is on last

More information

Statics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r.

Statics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r. Statcs Th cotact btw a mapulato ad ts vomt sults tactv ocs ad momts at th mapulato/vomt tac. Statcs ams at aalyzg th latoshp btw th actuato dv tous ad th sultat oc ad momt appld at th mapulato dpot wh

More information

Executive Committee and Officers ( )

Executive Committee and Officers ( ) Gifted and Talented International V o l u m e 2 4, N u m b e r 2, D e c e m b e r, 2 0 0 9. G i f t e d a n d T a l e n t e d I n t e r n a t i o n a2 l 4 ( 2), D e c e m b e r, 2 0 0 9. 1 T h e W o r

More information

Almost Unbiased Exponential Estimator for the Finite Population Mean

Almost Unbiased Exponential Estimator for the Finite Population Mean Rajs Sg, Pakaj aua, rmala Saa Scool of Sascs, DAVV, Idor (M.P., Ida Flor Smaradac Uvrs of Mco, USA Almos Ubasd Epoal Esmaor for F Populao Ma Publsd : Rajs Sg, Pakaj aua, rmala Saa, Flor Smaradac (Edors

More information

C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f

C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f C H A P T E R I G E N E S I S A N D GROWTH OF G U IL D S C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f i n a v a r i e t y o f f o r m s - s o c i a l, r e l i g i

More information

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane.

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane. CBSE CBSE SET- SECTION. Gv tht d W d to fd 7 7 Hc, 7 7 7. Lt,. W ow tht.. Thus,. Cosd th vcto quto of th pl.. z. - + z = - + z = Thus th Cts quto of th pl s - + z = Lt d th dstc tw th pot,, - to th pl.

More information

F l a s h-b a s e d S S D s i n E n t e r p r i s e F l a s h-b a s e d S S D s ( S o-s ltiad t e D r i v e s ) a r e b e c o m i n g a n a t t r a c

F l a s h-b a s e d S S D s i n E n t e r p r i s e F l a s h-b a s e d S S D s ( S o-s ltiad t e D r i v e s ) a r e b e c o m i n g a n a t t r a c L i f e t i m e M a n a g e m e n t o f F l a-b s ah s e d S S D s U s i n g R e c o v e r-a y w a r e D y n a m i c T h r o t t l i n g S u n g j i n L e, e T a e j i n K i m, K y u n g h o, Kainmd J

More information

EQUATION SHEETS FOR ELEC

EQUATION 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 information

P 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 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 information

Convergence tests for the cluster DFT calculations

Convergence tests for the cluster DFT calculations Covgc ss o h clus DF clculos. Covgc wh spc o bss s. s clculos o bss s covgc hv b po usg h PBE ucol o 7 os gg h-b. A s o h Guss bss ss wh csg s usss hs b us clug h -G -G** - ++G(p). A l sc o. Å h c bw h

More information

principles of f ta f a rt.

principles of f ta f a rt. DD H L L H PDG D BB PBLH L 20 D PP 32 C B P L s BDWY s BGG M W C WDM DLL P M DC GL CP F BW Y BBY PMB 5 855 C WHL X 6 s L Y F H 5 L & 5 zzzl s s zz z s s» z sk??» szz zz s L ~Lk Bz ZzY Z? ~ s s sgss s z«f

More information

Series of New Information Divergences, Properties and Corresponding Series of Metric Spaces

Series of New Information Divergences, Properties and Corresponding Series of Metric Spaces Srs of Nw Iforao Dvrgcs, Proprs ad Corrspodg Srs of Mrc Spacs K.C.Ja, Praphull Chhabra Profssor, Dpar of Mahacs, Malavya Naoal Isu of Tchology, Japur (Rajasha), Ida Ph.d Scholar, Dpar of Mahacs, Malavya

More information

Bethe-Salpeter Equation Green s Function and the Bethe-Salpeter Equation for Effective Interaction in the Ladder Approximation

Bethe-Salpeter Equation Green s Function and the Bethe-Salpeter Equation for Effective Interaction in the Ladder Approximation Bh-Salp Equaon n s Funcon and h Bh-Salp Equaon fo Effcv Inacon n h Ladd Appoxmaon Csa A. Z. Vasconcllos Insuo d Físca-UFRS - upo: Físca d Hadons Sngl-Pacl Popagao. Dagam xpanson of popagao. W consd as

More information

Life After Study Abroad

Life After Study Abroad f oe oab o C P p H book F 6 F Y 6 7 P5-URF : P os S yab o C Op p o s I f o m o sb o s soff b y 6 ss b j o g P o ob yd P g o( T5 7 N os ) k Rom I y Lf Af Sy Abo INTRODUCTION Pps yo'v b ookg fow o sy bo

More information

Parametric Down Conversion. Quantum optics seminar Winter 2008 Assaf Shaham

Parametric Down Conversion. Quantum optics seminar Winter 2008 Assaf Shaham Paam Dow Covso Quaum ops sma 7774 W 8 ssaf Shaham ox Iouo Thoy of lass Sum Fquy Gao Quaum Hamloa fo PDC pplaos No la ops Cao of w fqus h sysm. Usually h w fqus hav small amplu lav o h pu fqus. Hamo Dff

More information

Entangled Photon-Electron States and the Number-Phase Minimum Uncertainty States of the Photon Field

Entangled Photon-Electron States and the Number-Phase Minimum Uncertainty States of the Photon Field Vaó: Eagld_Poo-Elco_Sa_A Eagld Poo-Elco Sa ad Num-Pa Mmum Ucay Sa of Poo Fld S Vaó Rac Iu fo Sold Sa Pyc ad Oc H-55 Buda POBo 9 Hugay E-mal: vao@mal.f.u Aac. T ac aalyc oluo of gy gvalu quao of ym cog

More information

What areas are affected? Bucklands. Beach. Eastern. Beach. Half Moon Bay. Mellons. Bay. Howick. Highland. Cockle Bay. Park. Shelly. Botany Downs.

What areas are affected? Bucklands. Beach. Eastern. Beach. Half Moon Bay. Mellons. Bay. Howick. Highland. Cockle Bay. Park. Shelly. Botany Downs. ? F S cb c w v w b w. c b vc w b c. ffc? w f c b w? Y b vc c I c b w c vc f vw vw w fqc, w 1. v w 2, wc fw b fqc b cc j c. Y Nw b Nw b Nw b c P w S c P c w P S P b O O 2: w P 3: f b f c, cc wb f f w v

More information

Connecting Deer Creek and River des Peres Greenway

Connecting Deer Creek and River des Peres Greenway C D C Rv s s Gy ps D C Gy NORTH W Av Av Js Av E Av Su Av E Av Chy Av G Bv y Av. ps y h s G Bv, h h--y Cuy Av. ps C Rv s s Gy D C B B Bv Ox Av. Sussx Av. C Av. Ox Av. Ch Av. Ch Av. By E Av Mh Av. D C O-

More information

Mathematical Statistics. Chapter VIII Sampling Distributions and the Central Limit Theorem

Mathematical Statistics. Chapter VIII Sampling Distributions and the Central Limit Theorem Mahmacal ascs 8 Chapr VIII amplg Dsrbos ad h Cral Lm Thorm Fcos of radom arabls ar sall of rs sascal applcao Cosdr a s of obsrabl radom arabls L For ampl sppos h arabls ar a radom sampl of s from a poplao

More information

Geometrical optics. Textbook: Born and Wolf (chapters 3-5) Overview:

Geometrical optics. Textbook: Born and Wolf (chapters 3-5) Overview: Gomal ops Txbook: Bo a Wol aps -5 Ovvw: Elomag pla wavs om maxwll's quaos. T Ekoal quao a s vao ops a o wavlg. Rao ll's law lo Toal al lo T psm Dspso T ls Imagg as a pojv asomao. Opal ssms a ABCD max.

More information

Reliability analysis of time - dependent stress - strength system when the number of cycles follows binomial distribution

Reliability analysis of time - dependent stress - strength system when the number of cycles follows binomial distribution raoal Joural of Sascs ad Ssms SSN 97-675 Volum, Numbr 7,. 575-58 sarch da Publcaos h://www.rublcao.com labl aalss of m - dd srss - srgh ssm wh h umbr of ccls follows bomal dsrbuo T.Sumah Umamahswar, N.Swah,

More information

Chapter 1 Fundamentals in Elasticity

Chapter 1 Fundamentals in Elasticity Fs s . Ioo ssfo of ss Ms 분체역학 G Ms 역학 Ms 열역학 o Ms 유체역학 F Ms o Ms 고체역학 o Ms 구조해석 ss Dfo of Ms o B o w oo of os o of fos s s w o s s. Of fs o o of oo fos os o o o. s s o s of s os s o s o o of fos o. G fos

More information

exhibitor prospectus InternatIonal art MaterIals association MARCH 4-6 DALLAS co-locating with: Denver Art Museum Colorado Convention Center

exhibitor prospectus InternatIonal art MaterIals association MARCH 4-6 DALLAS co-locating with: Denver Art Museum Colorado Convention Center xhbo Oc IIol MIl ociio O18 DALLAS co-locg wh: Coloo Covo C Dv A Mm DALLAS IIol MIl ociio Ky bly hcho covo c h oly how c xclvly o l! O18 ch ov 700 ml by cov wh w h y oc w oc vlo w l l x bo chl c w loh xg

More information

Introduction to Laplace Transforms October 25, 2017

Introduction to Laplace Transforms October 25, 2017 Iroduco o Lplc Trform Ocobr 5, 7 Iroduco o Lplc Trform Lrr ro Mchcl Egrg 5 Smr Egrg l Ocobr 5, 7 Oul Rvw l cl Wh Lplc rform fo of Lplc rform Gg rform b gro Fdg rform d vr rform from bl d horm pplco o dffrl

More information

H STO RY OF TH E SA NT

H STO RY OF TH E SA NT O RY OF E N G L R R VER ritten for the entennial of th e Foundin g of t lair oun t y on ay 8 82 Y EEL N E JEN K RP O N! R ENJ F ] jun E 3 1 92! Ph in t ed b y h e t l a i r R ep u b l i c a n O 4 1922

More information

Existing Conditions. View from Ice Rink Patio. Ice Rink Patio. Beginner Terrain and Lighting. Tubing Hill. Little Tow & Beginner Terrain

Existing Conditions. View from Ice Rink Patio. Ice Rink Patio. Beginner Terrain and Lighting. Tubing Hill. Little Tow & Beginner Terrain Bg T Lghg Tubg Hll Ic k P T f Bg T V f Sc Accss Nh Ll T & Bg T I Ex T Mc Bulg B f Bg T Pkg L & g Wll V f Ic k P MA S TE Bs A & Lghg Z E H E N AN ASSOCIATES, INC. ACHITECTUE PLANNING INTEIOS LANSCAPE ACHITECTUE

More information

`G 12 */" T A5&2/, ]&>b ; A%/=W, 62 S 35&.1?& S + ( A; 2 ]/0 ; 5 ; L) ( >>S.

`G 12 */ T A5&2/, ]&>b ; A%/=W, 62 S 35&.1?& S + ( A; 2 ]/0 ; 5 ; L) ( >>S. 01(( +,-. ()*) $%&' "#! : : % $& - "#$ :, (!" -&. #0 12 + 34 2567 () *+ '!" #$%& ; 2 "1? + @)&2 A5&2 () 25& 89:2 *2 72, B97I J$K

More information

J. N. R E DDY ENERGY PRINCIPLES AND VARIATIONAL METHODS APPLIED MECHANICS

J. N. R E DDY ENERGY PRINCIPLES AND VARIATIONAL METHODS APPLIED MECHANICS J. N. E DDY ENEGY PINCIPLES AND VAIATIONAL METHODS IN APPLIED MECHANICS T H I D E DI T IO N JN eddy - 1 MEEN 618: ENEGY AND VAIATIONAL METHODS A EVIEW OF VECTOS AND TENSOS ead: Chapte 2 CONTENTS Physical

More information

( ) ( ) Weibull Distribution: k ti. u u. Suppose t 1, t 2, t n are times to failure of a group of n mechanisms. The likelihood function is

( ) ( ) Weibull Distribution: k ti. u u. Suppose t 1, t 2, t n are times to failure of a group of n mechanisms. The likelihood function is Webll Dsbo: Des Bce Dep of Mechacal & Idsal Egeeg The Uvesy of Iowa pdf: f () exp Sppose, 2, ae mes o fale of a gop of mechasms. The lelhood fco s L ( ;, ) exp exp MLE: Webll 3//2002 page MLE: Webll 3//2002

More information

Chapter 1 Fundamentals in Elasticity

Chapter 1 Fundamentals in Elasticity Fs s ν . Po Dfo ν Ps s - Do o - M os - o oos : o o w Uows o: - ss - - Ds W ows s o qos o so s os. w ows o fo s o oos s os of o os. W w o s s ss: - ss - - Ds - Ross o ows s s q s-s os s-sss os .. Do o ..

More information

x xi r 0. The most popular RBFs are given as follows: IUST International Journal of Engineering Science, Vol. 19, No.5-2, 2008, Page 21-26

x xi r 0. The most popular RBFs are given as follows: IUST International Journal of Engineering Science, Vol. 19, No.5-2, 2008, Page 21-26 IST Iol Jol of Egg S Vol 9 o5-8 Pg -6 O THE MERICAL SOLTIO OF OE IMESIOAL SCHROIGER EQATIO WITH OARY COITIOS IVOLVIG FRACTIOAL IFFERETIAL OPERATORS Jzb & M Mo Ab: I pp w y of olloo mo w Rl Fo o olv o mol

More information

Chapter 5 Transient Analysis

Chapter 5 Transient Analysis hpr 5 rs Alyss Jsug Jg ompl rspos rs rspos y-s rspos m os rs orr co orr Dffrl Equo. rs Alyss h ffrc of lyss of crcus wh rgy sorg lms (ucors or cpcors) & m-ryg sgls wh rss crcus s h h quos rsulg from r

More information

Luiz Leal Oak Ridge National Laboratory. of Massachusetts Institute. of Technology (MIT)

Luiz Leal Oak Ridge National Laboratory. of Massachusetts Institute. of Technology (MIT) LzLl OkRdgNlLby LsPsdhNl Egg Dp f h MsshssIs f Thlgy(MIT) Csy f Lz Ll, Ok Rdg Nl Lby. Usd wh pss. NI T Idpd Tsp Eq f Φ(E,,Ωˆ ) Ωˆ. Φ + Σ Φ = dωˆ ' de'σ s (E' E, Ωˆ ' Ω)Φ(E', ',Ωˆ ) + S 4 π 0 Σ Msplsss

More information

CONSTACYCLIC CODES OF LENGTH OVER A FINITE FIELD

CONSTACYCLIC CODES OF LENGTH OVER A FINITE FIELD Jorl o Algbr Nbr Tory: Ac Alco Vol 5 Nbr 6 Pg 4-64 Albl ://ccc.co. DOI: ://.o.org/.864/_753 ONSTAYLI ODES OF LENGTH OVER A FINITE FIELD AITA SAHNI POONA TRAA SEHGAL r or Ac Sy c Pb Ury gr 64 I -l: 5@gl.co

More information

CHAPTER: 3 INVERSE EXPONENTIAL DISTRIBUTION: DIFFERENT METHOD OF ESTIMATIONS

CHAPTER: 3 INVERSE EXPONENTIAL DISTRIBUTION: DIFFERENT METHOD OF ESTIMATIONS CHAPTER: 3 INVERSE EXPONENTIAL DISTRIBUTION: DIFFERENT METHOD OF ESTIMATIONS 3. INTRODUCTION Th Ivrs Expoal dsrbuo was roducd by Kllr ad Kamah (98) ad has b sudd ad dscussd as a lfm modl. If a radom varabl

More information

Major: All Engineering Majors. Authors: Autar Kaw, Luke Snyder

Major: All Engineering Majors. Authors: Autar Kaw, Luke Snyder Nolr Rgrsso Mjor: All Egrg Mjors Auhors: Aur Kw, Luk Sydr hp://urclhodsgusfdu Trsforg Nurcl Mhods Educo for STEM Udrgrdus 3/9/5 hp://urclhodsgusfdu Nolr Rgrsso hp://urclhodsgusfdu Nolr Rgrsso So populr

More information

MODELING AND IDENTIFICATION OF A TWO-LINK FLEXIBLE MANIPULATOR

MODELING AND IDENTIFICATION OF A TWO-LINK FLEXIBLE MANIPULATOR ABC Sosu Ss caocs - Vo. 5 Cog b ABC Sco VII - Robocs Pag 9 ODELIN AND IDENIFICAION OF A WO-LINK FLEXIBLE ANIPULAOR og Auguso Bof jog.g@ga.co Fábo L.. Saos fsaos@a.b Cao Rogus Bao caob@ga.co Luz Caos Saova

More information

t a serial T p c o y o d c b m ii y f t s u d W y p ii a p l u R O f l T h k s m me t er y d n y ad v o t b c t t t w j i t M ua T n a a o t U t n i a

t a serial T p c o y o d c b m ii y f t s u d W y p ii a p l u R O f l T h k s m me t er y d n y ad v o t b c t t t w j i t M ua T n a a o t U t n i a = = W # = A G 1 P S 1 A R 2 R Sg 19 C C 1 R A 6 g (M, C S H S y 3 C F 4! U M y 1 D D ( 6 W B C D C 7 W T 6 E S S 4 W S 1 v E T 2 g y - F P C C 1 L 8 - d M S N 2 d O k4 C S 5 y D O 4 y? 4! 7 ~ S y C R Md

More information

Beechwood Music Department Staff

Beechwood Music Department Staff Beechwood Music Department Staff MRS SARAH KERSHAW - HEAD OF MUSIC S a ra h K e rs h a w t r a i n e d a t t h e R oy a l We ls h C o l le g e of M u s i c a n d D ra m a w h e re s h e ob t a i n e d

More information

Bayesian Credibility for Excess of Loss Reinsurance Rating. By Mark Cockroft 1 Lane Clark & Peacock LLP

Bayesian Credibility for Excess of Loss Reinsurance Rating. By Mark Cockroft 1 Lane Clark & Peacock LLP By Cly o c o Lo Rc Rg By M Coco L Cl & Pcoc LLP GIRO coc 4 Ac Th pp c how o v cly wgh w po- pc-v o c o lo c. Th po co o Poo-Po ol ch wh po G o. Kywo c o lo c g By cly Poo Po G po Acowlg cl I wol l o h

More information

Y'* C 0!),.1 / ; ')/ Y 0!)& 1 0R NK& A Y'. 1 ^. ]'Q 1 I1 )H ;". D* 1 = Z)& ^. H N[Qt C =

Y'* C 0!),.1 / ; ')/ Y 0!)& 1 0R NK& A Y'. 1 ^. ]'Q 1 I1 )H ;. D* 1 = Z)& ^. H N[Qt C = (-) 393 F!/ $5 $% T K&L =>-? J (&A )/>2 I B!" GH 393/05/07 :K 393/07/23 :7b +B 0 )NO M / Y'* C a23 N/ * = = Z)& ^. ;$ 0'* Y'2 8 OI 53 = ;" ~" O* Y.b ;" ; ')/ Y'* C 0!),. / ; ')/ Y 0!)& 0R NK& A Y'. ^.

More information

Introduction to Finite Element Method

Introduction to Finite Element Method p. o C d Eo E. Iodo o E Mod s H L p. o C d Eo E o o s Ass L. o. H L p://s.s.. p. o C d Eo E. Cos. Iodo. Appoo o os & o Cs. Eqos O so. Mdso os-es 5. szo 6. wo so Es os 7. os ps o Es 8. Io 9. Co C Isop E.

More information