MULTIPLE SOLITON SOLUTIONS FOR TWO INTEGRABLE COUPLINGS OF THE MODIFIED KORTEWEG-DE VRIES EQUATION

Size: px
Start display at page:

Download "MULTIPLE SOLITON SOLUTIONS FOR TWO INTEGRABLE COUPLINGS OF THE MODIFIED KORTEWEG-DE VRIES EQUATION"

Transcription

1 THE PUBLISHING HOUSE POCEEDINGS OF THE OMANIAN ACADEMY Srs A OF THE OMANIAN ACADEMY Volm Nmbr /0 pp 9 5 MULTIPLE SOLITON SOLUTIONS FO TWO INTEGABLE COUPLINGS OF THE MODIFIED KOTEWEG-DE VIES EQUATION Abdl-Md WAZWAZ S Xvr Uvrsy Dprm of Mhmcs Chcgo IL USA E-ml: wzwz@sd I hs wor w s h lgbr of copld sclrs o dvlop wo ds of olr grbl coplgs of h modfd Korwg-d Vrs (mkdv qo O of h grbl coplgs of h mkdv qo gvs mlpl solo solos of dsc mplds whrs h scod d gvs mlpl sglr solo solos of dsc mplds s wll Th Bäcld rsformo d h smplfd Hro s mhod wll b sd for hs sdy W show h hs coplgs possss mlpl solo solos h sm s h mlpl solo solos of h mkdv qo b dffr oly h coffcs of h Bäcld rsformo Ths dffrc hbs solo solos wh dsc mplds Ky words: grbl coplgs bäcld rsformos modfd Korwg-d Vrs qo mlpl solo solos INTODUCTION Th bqos Korwg-d Vrs (KdV qo [ ] dmsolss vrbls rds ± + 0 ( 6 Ths qo modls vry of olr wv phom sch s shllow wr wvs cosc wvs hrmoc crysl d o-cosc wvs plsms Th KdV qo s complly grbl d gvs rs o mlpl-solo solos Ths qo hs b sdd by vry of mhods sch s h vrs scrg mhod d h Bäcld rsformo mhod Th KdV qo dms mlplsolo solos d hbs f mbr of cosrvo lws of rgy Th modfd KdV (mkdv qo + + ( 6 0 s mpor my rs of olr scc Th mkdv qo pprs cosc wvs cr hrmoc lcs modls of rffc cogso rsmsso ls Schoy brrr Alfvé wvs collso lss plsm o cosc solos lsc md d ohr pplcos I posssss my rmrbl proprs sch s cosrvo lws vrs scrg rsformo blr rsformo mlpl solo solos brhr solos Plvé grbly d Drbo rsformo Th hory of olr grbl coplgs of ordry solo sysms ws prsd [] d frhr sdd [] d ohrs I [ ] M l proposd h prrbo mhod for sblshg grbl coplgs Zhg l [] prsd h lrgd L lgbr mhod o ob grbl coplgs Prclrly oworhy r h cosrcos of grbl coplgs bsd o h o-sm smpl L lgbrs [] I fc hr r svrl mhods dopd o cosrc grbl coplgs sch s prrbos lrgg h spcrl problm crg w loop lgbrs d sm drc sms of L lgbr Lo of wor hs b do hs fld d my grbl coplgs wr cosrcd [56] I s ow ow h for grbl sysm w c cosrc w grbl dffrl qo sysm clld grbl coplgs whch clds h gv grbl qo s sb-sysm

2 0 Abdl-Md Wzwz I [] vry rl rglr olr coplgs of grbl sysms wr dvlopd Th cosrco [] ws md o h lvl of volo qos by modfco of h lgbr of dymcl flds Th lgbr of copld sclrs ws sd o dvlop -copld KdV (c-kdv gv h form Th lgbr of copld sclrs ws rodcd [] d ws show o b l commv d ssocv Morovr h grbly of h coplgs ( ws md [] My rlbl mhods r sd h solry wvs hory o vsg solos d prclr mlpl solo solos of complly grbl qos Th lgbrc-gomrc mhod h vrs scrg mhod h Bäcld rsformo mhod h Drbo rsformo mhod h Hro blr mhod d ohr mhods r sd o m progrss d w dvlopms hs fld I hs wor w m o pply h Bäcld rsformos d h smplfd Hro s mhod [ 0] for rlbl sdy Or m from hs wor s wo fold Th frs gol s o mploy h dvlopd lgbr of copld sclrs [] o drv wo forms of olr grbl coplgs of h modfd KdV qo W m scod o sdy hs coplgs d show h possss mlpl solo solos d mlpl sglr solo solos h sm s h mkdv qo b dffr oly h coffcs of h Bäcld rsformos h rsl dsc mplds for ch qo of h sysm 0 ( FIST COUPLINGS OF THE MKDV EQUATION: MULTIPLE SOLITON SOLUTIONS I l mr o h pproch prsd [] whr h lgbr of copld sclrs ws dvlopd w s o fld solo sysm K[ ] K[ ] ( h c b dd o h sysm of copld PDEs of h form [] K[ ] K[ ] (5 whr Accordgly h sysm (5 s h form [] [ ] K K K ( (7

3 Mlpl solo solos for wo grbl coplgs of h modfd Korwg-d Vrs qo Usg ( w c s 6 Isrg (8 o (7 w dvlop h -copld modfd KdV (c-mkdv gv h form ( + 6( + 6 6( + + 6( (8 (9 Mlpl solo solos Sbsg ω ( o h lr rms of ch qo (9 gvs h dsprso rlo by d s rsl w ob h followg phs vrbls Th mlpl solo solos of h coplgs (9 r ssmd o b (0 ω ( ( F( FG GF ( rc G( F + G whr h lry fcos F ( d G ( for h sgl solo solo r gv by ( F( G ( ( Sbsg ( o (9 d solvg for d w ob wo dsc ss gv by (5 + ( for ( + for Combg h obd rsls gvs wo ss of sgl solo solos (6 + ( ( + (7

4 Abdl-Md Wzwz d for + ( + ( for + I ohr words w ob wo ss of sgl solo solos wh dsc mplds bw h wo ss for r r For h wo solo solos w s h lry fcos by (8 F( + G + ( Usg (9 ( d sbsg h rsl (9 w ob h followg phs shf coffc d hc w s ( ( + ( < ( + (9 (0 ( Usg (5 d (6 d h prvos rsls w lso ob wo dsc ss of wo solo solos I s wll ow h wo solo solo [] c dgr o rso rd dr h codos 0 or( 0 for ( Accordgly h rsoc phomo dos o s for hs coplg bcs 0 d ( 0 for For h hr solo solos w s F( G( Procdg s bfor w fd b ( b ( Two ss of hr solo solos wh dsc mplds r obd by sbsg ( o ( s prsd rlr Ths shows h ch qo of h coplg (9 possss h sm proprs s h mkdv qo: h sm phs vrbl h sm phs shf d h o rsoc phom Howvr h oly dffrc s h h mplds r dsc for dsc SECOND COUPLINGS OF THE MKDV EQUATION: MULTIPLE SINGULA SOLITON SOLUTIONS Usg h scod form of h mkdv qo 6 (5

5 5 Mlpl solo solos for wo grbl coplgs of h modfd Korwg-d Vrs qo d sg h lyss prsd bfor for h drvo of h coplgs of h mkdv qo w ob scod coplgs of h mkdv qo gv by I hs sco w wll m mlpl sglr solo solos of h scod d of h coplgs of h mkdv qo ( + + 6( ( ( (6 Mlpl sglr solo solos Sbsg ( ω (7 o h lr rms of ch qo (6 gvs h dsprso rlo by d s rsl w ob h followg phs vrbls Th sglr solo solos of h coplgs (6 r ssmd o b ω (8 (9 f ( ( l g( gf fg gf whr h lry fcos f ( d g ( for h sgl sglr solo solo r gv by (0 f ( g( ( d Sbsg (0 o (6 d solvg for w ob wo ss of solos ( + ( for ( for Sbsg ( o (0 gvs wo ss of sgl sglr solo solos gv by ( d + ( ( (

6 Abdl-Md Wzwz 6 for ( 8 ( for I ohr words w ob wo ss of sgl sglr solo solos wh dsc mplds for r r For h wo solo solos w s h lry fcos by + + f( + + g ( Usg (6 (0 d sbsg h rsl (6 w ob h followg phs shf coffc d hc w s ( ( + (5 (6 (7 ( < (8 ( + Combg h obd rsls gvs wo ss of wo sglr solo solos For h hr solo solos w s f ( g( + Procdg s bfor w fd b b (9 b (0 Ths r gvs wo ss of hr sglr solo d h hr sglr -solo solos r obd by sbsg (9 o (0 DISCUSSION I hs wor wo ds of coplgs of h mkdv qo wr dvlopd by sg h lgbr of copld sclrs Mlpl solo d mlpl sglr solos r drvd for h boh coplgs of h mkdv qo I fc wo ss of solo solos wr drvd for ch coplg W showd h ch qo of h wo coplgs posssss h sm proprs s h mkdv qo: h sm phs vrbl h sm phs shf d h o rsoc phom Howvr h oly dffrc s h h mplds r dsc for ch qo of h coplgs EFEENCES M BASZAK B SZABLIKOWSKI B SILINDI Cosrco d sprbly of olr solo grbl coplgs Appl Mh Comp 9 pp WX MA B FUCHSSTEINE Igrbl hory of h prrbo qos Chos Solos d Frcls 7 pp WX MA Z-N ZHU Cosrcg olr dscr grbl Hmlo coplgs Comp Mh Applcos 60 pp

7 7 Mlpl solo solos for wo grbl coplgs of h modfd Korwg-d Vrs qo 5 Y ZHANG H TAM Thr ds of coplg grbl coplgs of h Korwg d Vrs hrrchy of volo qos J Mh Phys Y FA-JUN L LI Igrbl coplgs of C-KdV qos hrrchy wh slf-coss sorcs ssocd wh sl( Phys L A 7 pp Y FA-JUN Prologo srcr for olr grbl coplgs of KdV solo hrrchy Ch Phys B CM KHALIQUE Ec solos d cosrvo lws of copld grbl dsprsolss sysm Flom 6 pp CM KHALIQUE A BISWAS Solos Plsms: A L Symmry Approch Irol Jorl of Thorcl Physcs 8 pp CM KHALIQUE A BISWAS Opcl solos wh powr lw olry sg L grop lyss Phys L A 7 pp BB KADOMTSEV VI PETVIASHVILI O h sbly of solry wvs wly dsprsv md Sov Phys Dol 5 pp HIOTA M ITO soc of solos o dmso J Phys Soc Jp 5 pp HIOTA A w form of Bäcld rsformos d s rlo o h vrs scrg problm Progrss of Thorcl Physcs 5 pp H LEBLOND H TIKI D MIHALACHE Drvo of grlzd dobl-s-gordo qo dscrbg lrshor solo propgo opcl md composd of mllvl oms Phys v A H LEBLOND D MIHALACHE Modls of fw opcl cycl solos byod h slowly vryg vlop ppromo Phys pors 5 pp AM WAZWAZ (+-dmsol KdV (N qos drvd by sg h KdV rcrso opror Physc Scrp AM WAZWAZ Two forms of (+-dmsol B-yp Kdomsv-Pvshvl qo: mlpl solo solos Physc Scrp AM WAZWAZ O d wo solo solos for svh-ordr Cdry-Dodd-Gbbo d Cdry-Dodd-Gbbo-KP qos Crl Erop Jorl of Physcs 0 pp AM WAZWAZ A rlbl sdy for sos of h Br problm wh bodry codos Mhmcl Mhods h Appld Sccs 5 pp AM WAZWAZ Solo solos for wo (+-dmsol o-grbl KdV-yp qos Mhmcl d Compr Modllg 55 pp AM WAZWAZ Igrbl coplgs of h Brgrs qo d h Shrm-Tsso-Olvr qo om pors Physcs 65 0 cvd Mrch 0

counting statistics in thermal transport in nanojunctions

counting statistics in thermal transport in nanojunctions rs bhvor d fll cog sscs hrml rspor ojcos J-Shg Wg Dp PhysNUS Ol of h lk rodco Mhod of oqlbrm r s fcos Applcos hrml crrs D ch d obs rs problm Fll cog sscs MS workshop Forr s lw for h codco J [ ] f f d Forr

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

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

Special Curves of 4D Galilean Space

Special Curves of 4D Galilean Space Irol Jourl of Mhml Egrg d S ISSN : 77-698 Volum Issu Mrh hp://www.jms.om/ hps://ss.googl.om/s/jmsjourl/ Spl Curvs of D ll Sp Mhm Bkş Mhmu Ergü Alpr Osm Öğrmş Fır Uvrsy Fuly of S Dprm of Mhms 9 Elzığ Türky

More information

Quantum Properties of Idealized GW Detector

Quantum Properties of Idealized GW Detector Qm Prors of Idlzd GW Dor Sg Pyo Km Ks N l Uvrsy Osk Uvrsy J 3 Th 4 h Kor-J Worksho o KAGRA Ol Idlzd Dor for Grvol Wvs Qm Thory for Dsso Wgr Fo of Tm-Dd Osllor Dmd Osllor Drv by Erl Fors Colso Idlzd Dor

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

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

Interaction Between an Embedded Crack and an Interface Crack in Nonhomogeneous Coating System

Interaction Between an Embedded Crack and an Interface Crack in Nonhomogeneous Coating System Mrls Scc Form Vols. 9-9 (5) pp 97- Ol vll sc 5/g/5 www.scc. (5) Trs Tch Plcos Swzrl o:.8/www.scc./msf.9-9.97 Irco Bw Em Crck Irc Crck Nohomogos Cog Ssm E.E. Thookoglo G.H. Plo Fcl o ppl Sccs Dp. o Mchcs-L.

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

U1. Transient circuits response

U1. Transient circuits response U. Tr crcu rpo rcu ly, Grdo Irí d omucco uro 6-7 Phlp Sm phlp.m@uh. Dprmo d Torí d l Sñl y omucco Idx Rcll Gol d movo r dffrl quo Rcll Th homoou oluo d d ordr lr dffrl quo Exmpl of d ordr crcu Il codo

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

Linear System Review. Linear System Review. Descriptions of Linear Systems: 2008 Spring ME854 - GGZ Page 1

Linear System Review. Linear System Review. Descriptions of Linear Systems: 2008 Spring ME854 - GGZ Page 1 8 Sprg ME854 - Z Pg r Sym Rvw r Sym Rvw r Sym Rvw crpo of r Sym: p m R y R R y FT : & U Y Trfr Fco : y or : & : d y d r Sym Rvw orollbly d Obrvbly: fo 3.: FT dymc ym or h pr d o b corollbl f y l > d fl

More information

On the Hubbard-Stratonovich Transformation for Interacting Bosons

On the Hubbard-Stratonovich Transformation for Interacting Bosons O h ubbrd-sroovh Trsformo for Irg osos Mr R Zrbur ff Fbrury 8 8 ubbrd-sroovh for frmos: rmdr osos r dffr! Rdom mrs: hyrbol S rsformo md rgorous osus for rg bosos /8 Wyl grou symmry L : G GL V b rrso of

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

Study on Non-linear Responses of Eccentric Structure

Study on Non-linear Responses of Eccentric Structure Th 4 h World ofr o Erh Egrg or -7 8 Bg h Sd o No-lr Rpo of Er Srr Hdz WATANABE oh USUNI Ar TASAI 3 Grd Sd Dpr of Arhr ooh Nol Uvr ooh Jp Ao Profor Dpr of Arhr ooh Nol Uvr ooh Jp ABSTRAT : 3 Profor Dpr

More information

Meteorologische Modellierung

Meteorologische Modellierung Morologsch Modllrg Irodco o Nmrcl Modlg of h Globl mosphrc Crclo Fr L Ol 0. Irodco: Whr/wh s h problm d bscs. h lr volo dcy qo dscrzo m. O-dmsol lr dvco dscrzo m d spc. O-dmsol lr dffso d o-dmsol lr rspor

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

EEE 303: Signals and Linear Systems

EEE 303: Signals and Linear Systems 33: Sigls d Lir Sysms Orhogoliy bw wo sigls L us pproim fucio f () by fucio () ovr irvl : f ( ) = c( ); h rror i pproimio is, () = f() c () h rgy of rror sigl ovr h irvl [, ] is, { }{ } = f () c () d =

More information

Applications of semi-markov processes in reliability

Applications of semi-markov processes in reliability rbk Alco o m-mrko roc rlbl - TA # 3-4 7 Dcmbr - Scl I rbk rczk Nl Ur d old Alco o m-mrko roc rlbl Kword m-mrko roc rlbl rdom lr r cold db m wh rr Abrc Th bc do d horm rom h m-mrko roc hor r dcd h r Th

More information

On the Existence and uniqueness for solution of system Fractional Differential Equations

On 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 information

1- I. M. ALGHROUZ: A New Approach To Fractional Derivatives, J. AOU, V. 10, (2007), pp

1- I. M. ALGHROUZ: A New Approach To Fractional Derivatives, J. AOU, V. 10, (2007), pp Jourl o Al-Qus Op Uvrsy or Rsrch Sus - No.4 - Ocobr 8 Rrcs: - I. M. ALGHROUZ: A Nw Approch To Frcol Drvvs, J. AOU, V., 7, pp. 4-47 - K.S. Mllr: Drvvs o or orr: Mh M., V 68, 995 pp. 83-9. 3- I. PODLUBNY:

More information

ERDOS-SMARANDACHE NUMBERS. Sabin Tabirca* Tatiana Tabirca**

ERDOS-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 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

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

A Class of Harmonic Meromorphic Functions of Complex Order

A Class of Harmonic Meromorphic Functions of Complex Order Borg Irol Jourl o D Mg Vol 2 No 2 Ju 22 22 A Clss o rmoc Mromorpc Fucos o Complx Ordr R Elrs KG Surm d TV Sudrs Asrc--- T sml work o Clu d Sl-Smll [3] o rmoc mppgs gv rs o suds o suclsss o complx-vlud

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

NHPP and S-Shaped Models for Testing the Software Failure Process

NHPP and S-Shaped Models for Testing the Software Failure Process Irol Jourl of Ls Trds Copug (E-ISSN: 45-5364 8 Volu, Issu, Dcr NHPP d S-Shpd Modls for Tsg h Sofwr Flur Procss Dr. Kr Arr Asss Profssor K.J. Soy Isu of Mg Suds & Rsrch Vdy Ngr Vdy Vhr Mu. Id. dshuh_3@yhoo.co/rrr@ssr.soy.du

More information

3.4 Properties of the Stress Tensor

3.4 Properties of the Stress Tensor cto.4.4 Proprts of th trss sor.4. trss rasformato Lt th compots of th Cauchy strss tsor a coordat systm wth bas vctors b. h compots a scod coordat systm wth bas vctors j,, ar gv by th tsor trasformato

More information

OPTICAL DESIGN. FIES fibre assemblies B and C. of the. LENS-TECH AB Bo Lindberg Document name: Optical_documentation_FIES_fiber_BC_2

OPTICAL DESIGN. FIES fibre assemblies B and C. of the. LENS-TECH AB Bo Lindberg Document name: Optical_documentation_FIES_fiber_BC_2 OPTICAL DESIGN f h FIES fb ssmbs B d C LENS-TECH AB B Ldbg 2-4-3 Dcm m: Opc_dcm_FIES_fb_BC_2 Idc Ths p s dcm f h pc dsg f h FIES fb ssmbs B d C Th mchc dsg s shw I s shw h ssmb dwg md b Ahs Uvs Fb c Th

More information

COMPLEX NUMBERS AND ELEMENTARY FUNCTIONS OF COMPLEX VARIABLES

COMPLEX NUMBERS AND ELEMENTARY FUNCTIONS OF COMPLEX VARIABLES COMPLEX NUMBERS AND ELEMENTARY FUNCTIONS OF COMPLEX VARIABLES DEFINITION OF A COMPLEX NUMBER: A umbr of th form, whr = (, ad & ar ral umbrs s calld a compl umbr Th ral umbr, s calld ral part of whl s calld

More information

EXERCISE - 01 CHECK YOUR GRASP

EXERCISE - 01 CHECK YOUR GRASP DEFNTE NTEGRATON EXERCSE - CHECK YOUR GRASP. ( ) d [ ] d [ ] d d ƒ( ) ƒ '( ) [ ] [ ] 8 5. ( cos )( c)d 8 ( cos )( c)d + 8 ( cos )( c) d 8 ( cos )( c) d sic + cos 8 is lwys posiiv f() d ( > ) ms f() is

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

Approximation of Functions Belonging to. Lipschitz Class by Triangular Matrix Method. of Fourier Series

Approximation of Functions Belonging to. Lipschitz Class by Triangular Matrix Method. of Fourier Series I Jorl of Mh Alysis, Vol 4, 2, o 2, 4-47 Approximio of Fcios Blogig o Lipschiz Clss by Triglr Mrix Mhod of Forir Sris Shym Ll Dprm of Mhmics Brs Hid Uivrsiy, Brs, Idi shym _ll@rdiffmilcom Biod Prsd Dhl

More information

{ } [ ] { } { } 1. The simple Wright-Fisher model. Mathematics Population Genetics. n-step transition probabilities eqn(11)

{ } [ ] { } { } 1. The simple Wright-Fisher model. Mathematics Population Genetics. n-step transition probabilities eqn(11) Mhmcs Polo Gcs Corll Uvrsy J Jly 6 Wrr J ws Th sml Wrgh-shr modl q6 -s rso robbls q { } { }? r o r q { } { } { } { } } Prob{ δ δ δ δ δ δ { } [ ] / 4 gvs Ths. / - shr modl or h sml Wrgh δ δ M ms dffso romo

More information

OPTIMUM MULTILEVEL CHAOTIC SEQUENCES FOR ASYNCHRONOUS DS- CDMA SYSTEMS OVER RICIAN SELECTIVE FADING CHANNEL

OPTIMUM MULTILEVEL CHAOTIC SEQUENCES FOR ASYNCHRONOUS DS- CDMA SYSTEMS OVER RICIAN SELECTIVE FADING CHANNEL 5h rop rocss orc UIO 7 oz od pbr -7 7 copyrh by URI OIU ULILVL HOI QU OR YHROOU - Y OVR RII LIV I HL ǎ Vǎd os oo cocos pr Uvrsy ohc o chrs - I vd. Zp 7 chrs Ro pho: 75 : 75 : c{p}@co.pb.ro wb: www.co.pb.ro

More information

MECE 3320 Measurements & Instrumentation. Static and Dynamic Characteristics of Signals

MECE 3320 Measurements & Instrumentation. Static and Dynamic Characteristics of Signals MECE 330 MECE 330 Masurms & Isrumao Sac ad Damc Characrscs of Sgals Dr. Isaac Chouapall Dparm of Mchacal Egrg Uvrs of Txas Pa Amrca MECE 330 Sgal Cocps A sgal s h phscal formao abou a masurd varabl bg

More information

as nonrigid Carnot groups

as nonrigid Carnot groups Th Th Th V 5 5 34 356 V V crcc 5 c5 5 Hdr 5 34 356 Vr 34 dh 356 crcc-c 5 Hdr c Vr d Cr r c d Cr r c r c c r c 5 B Hdr Wrhr B Wrhr Vr Ccd b G cr Ccd b cr Abrc G c cr W d rdc r c d Cr hch Abrc r W d Cr rdc

More information

Complex Numbers. Prepared by: Prof. Sunil Department of Mathematics NIT Hamirpur (HP)

Complex Numbers. Prepared by: Prof. Sunil Department of Mathematics NIT Hamirpur (HP) th Topc Compl Nmbrs Hyprbolc fctos ad Ivrs hyprbolc fctos, Rlato btw hyprbolc ad crclar fctos, Formla of hyprbolc fctos, Ivrs hyprbolc fctos Prpard by: Prof Sl Dpartmt of Mathmatcs NIT Hamrpr (HP) Hyprbolc

More information

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

35H MPa Hydraulic Cylinder 3.5 MPa Hydraulic Cylinder 35H-3

35H MPa Hydraulic Cylinder 3.5 MPa Hydraulic Cylinder 35H-3 - - - - ff ff - - - - - - B B BB f f f f f f f 6 96 f f f f f f f 6 f LF LZ f 6 MM f 9 P D RR DD M6 M6 M6 M. M. M. M. M. SL. E 6 6 9 ZB Z EE RC/ RC/ RC/ RC/ RC/ ZM 6 F FP 6 K KK M. M. M. M. M M M M f f

More information

PADÉ-TYPE APPROXIMATION

PADÉ-TYPE APPROXIMATION NICHOLAS J. DARAS PADÉ-TYPE APPROXIMATION TO FOURIER SERIES HELLENIC ARMS CONTROL CENTER PUBLISHING pblshd o l s -boo ll rghs rsrvd -7- pblshd o l s boo 7 Cos Prc 5 Chpr Ι O h Nrcl Evlo o Hroc d -Prodc

More information

Chapter 8: Propagating Quantum States of Radiation

Chapter 8: Propagating Quantum States of Radiation Quum Opcs f hcs Oplccs h R Cll Us Chp 8: p Quum Ss f R 8. lcmc Ms Wu I hs chp w wll cs pp quum ss f wus fs f spc. Cs h u shw lw f lcc wu. W ssum h h wu hs l lh qul h -c wll ssum l. Th lcc cs s fuc f l

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

FL/VAL ~RA1::1. Professor INTERVI of. Professor It Fr recru. sor Social,, first of all, was. Sys SDC? Yes, as a. was a. assumee.

FL/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 information

SAMPLE LITANY OF THE SAINTS E/G. Dadd9/F. Aadd9. cy. Christ, have. Lord, have mer cy. Christ, have A/E. Dadd9. Aadd9/C Bm E. 1. Ma ry and. mer cy.

SAMPLE LITANY OF THE SAINTS E/G. Dadd9/F. Aadd9. cy. Christ, have. Lord, have mer cy. Christ, have A/E. Dadd9. Aadd9/C Bm E. 1. Ma ry and. mer cy. LTNY OF TH SNTS Cntrs Gnt flwng ( = c. 100) /G Ddd9/F ll Kybrd / hv Ddd9 hv hv Txt 1973, CL. ll rghts rsrvd. Usd wth prmssn. Musc: D. Bckr, b. 1953, 1987, D. Bckr. Publshd by OCP. ll rghts rsrvd. SMPL

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

Multiscale Element-Free Galerkin Method with Penalty for 2D Burgers Equation

Multiscale Element-Free Galerkin Method with Penalty for 2D Burgers Equation Jrl kolog ll ppr lscl lm-r Glrk o Pl for Brgrs o S Cg L S o Yk prm of mcl Sccs cl of Scc rs kolog ls 80 Joor Br Joor rl zm ls Corrspog or scg87@oo.com Arcl sor c 8 rc 0 c rs form 6 Aprl 0 Accp 7 0 Grpcl

More information

Pupil / Class Record We can assume a word has been learned when it has been either tested or used correctly at least three times.

Pupil / Class Record We can assume a word has been learned when it has been either tested or used correctly at least three times. 2 Pupi / Css Rr W ssum wr hs b r wh i hs b ihr s r us rry s hr ims. Nm: D Bu: fr i bus brhr u firs hf hp hm s uh i iv iv my my mr muh m w ih w Tik r pp push pu sh shu sisr s sm h h hir hr hs im k w vry

More information

CHAPTER 7. X and 2 = X

CHAPTER 7. X and 2 = X CHATR 7 Sco 7-7-. d r usd smors o. Th vrcs r d ; comr h S vrc hs cs / / S S Θ Θ Sc oh smors r usd mo o h vrcs would coclud h s h r smor wh h smllr vrc. 7-. [ ] Θ 7 7 7 7 7 7 [ ] Θ ] [ 7 6 Boh d r usd sms

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

Example: Two Stochastic Process u~u[0,1]

Example: Two Stochastic Process u~u[0,1] Co o Slo o Coco S Sh EE I Gholo h@h. ll Sochc Slo Dc Slo l h PLL c Mo o coco w h o c o Ic o Co B P o Go E A o o Po o Th h h o q o ol o oc o lco q ccc lco l Bc El: Uo Dbo Ucol Sl Ab bo col l G col G col

More information

Numerical Simulation for the 2-D Heat Equation with Derivative Boundary Conditions

Numerical Simulation for the 2-D Heat Equation with Derivative Boundary Conditions IOSR Joural of Applid Chmisr IOSR-JAC -ISSN: 78-576.Volum 9 Issu 8 Vr. I Aug. 6 PP 4-8 www.iosrjourals.org Numrical Simulaio for h - Ha Equaio wih rivaiv Boudar Codiios Ima. I. Gorial parm of Mahmaics

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

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

LINEAR 2 nd ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS

LINEAR 2 nd ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS Diol Bgyoko (0) I.INTRODUCTION LINEAR d ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS I. Dfiiio All suh diffril quios s i h sdrd or oil form: y + y + y Q( x) dy d y wih y d y d dx dx whr,, d

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

LECTURE 6 TRANSFORMATION OF RANDOM VARIABLES

LECTURE 6 TRANSFORMATION OF RANDOM VARIABLES LECTURE 6 TRANSFORMATION OF RANDOM VARIABLES TRANSFORMATION OF FUNCTION OF A RANDOM VARIABLE UNIVARIATE TRANSFORMATIONS TRANSFORMATION OF RANDOM VARIABLES If s a rv wth cdf F th Y=g s also a rv. If w wrt

More information

Vectors and Matrices

Vectors and Matrices Collg of Egrg d Compur Scc Mchcl Egrg Dprm Egrg Alyss Nos Ls updd: Augus 8, 7 Lrry Cro Vcors d Mrcs Iroduco Ths os provd roduco o h us of vcors d mrcs grg lyss. I ddo, hy provd dscusso of how h smpl cocp

More information

Inner Product Spaces INNER PRODUCTS

Inner 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 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

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find BSE SMLE ER SOLUTONS LSS-X MTHS SET- BSE SETON Gv tht d W d to fd 7 7 Hc, 7 7 7 Lt, W ow tht Thus, osd th vcto quto of th pl z - + z = - + z = Thus th ts quto of th pl s - + z = Lt d th dstc tw th pot,,

More information

[Let's Do ToPolio What We Did To Tokyo

[Let's Do ToPolio What We Did To Tokyo [L D W W D k /%// / j } b w k w kk w b N b b k z w - k w k k b b b b b w k b k w S b b- K k D R w b k k kk k w w "b b z b bk b w wk w kk w w k b b b b q V /VSRN O R S R SON - H R VL 11 N 11 q HK NONL KONDON

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

AE57/AC51/AT57 SIGNALS AND SYSTEMS DECEMBER 2012

AE57/AC51/AT57 SIGNALS AND SYSTEMS DECEMBER 2012 AE7/AC/A7 SIGNALS AND SYSEMS DECEMBER Q. Drmi powr d rgy of h followig igl j i ii =A co iii = Solio: i E P I I l jw l I d jw d d Powr i fii, i i powr igl ii =A cow E P I co w d / co l I I l d wd d Powr

More information

ANSWER KEY. Page 1 Page 2 cake key pie boat glue cat sled pig fox sun dog fish zebra. Page 3. Page 7. Page 6

ANSWER KEY. Page 1 Page 2 cake key pie boat glue cat sled pig fox sun dog fish zebra. Page 3. Page 7. Page 6 P 1 P 2 y sd fx s d fsh z ys P 3 P 4 my, ms, m, m, m, m P 6 d d P 7 m y P 5 m m s P 10 y y y P 8 P 9 s sh, s, ss, sd sds, s, sh sv s s P 11 s P 12,, m, m, m,, dd P 13 m f m P 18 h m s P 22 f fx f fsh fm

More information

Wave Phenomena Physics 15c

Wave 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 information

Consider a system of 2 simultaneous first order linear equations

Consider 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 information

Campsites are approximately 20 wide x 50 deep. Campsites must be paid for when the site is staked.

Campsites are approximately 20 wide x 50 deep. Campsites must be paid for when the site is staked. SHOTGUN MPSITE OOTE (SUNDY, SEPTEMBE 23) LST EVENT O 2018 SUPE SHOE WEEKEND (SEPTEMBE 28 30) NIGHT O DESTUTION. PHOTOS! I h Spr Sh p. Th rf w d 2:00 PM r h Sh r d h f f f (d f f f) dh h prf p. O hr, yr.

More information

Study on Structure Property of Cantilever Piezoelectric Vibration Generator

Study on Structure Property of Cantilever Piezoelectric Vibration Generator Sss & Tsds,. 177, Iss 8, As 14,. 46-5 Sss & Tsds 14 by IFSA Pbsh, S. L. h://www.sss.m Sdy S Py f C Pz b G 1,* Y Zh, Q, 1 L Jf 1 Mh & E C, A Usy f b, b Bd 711, Ch Sh f Ey Pw d Mh E, Nh Ch E Pw Usy, Bj 16,

More information

3.4 Repeated Roots; Reduction of Order

3.4 Repeated Roots; Reduction of Order 3.4 Rpd Roos; Rducion of Ordr Rcll our nd ordr linr homognous ODE b c 0 whr, b nd c r consns. Assuming n xponnil soluion lds o chrcrisic quion: r r br c 0 Qudric formul or fcoring ilds wo soluions, r &

More information

Vexilla regis prodeunt

Vexilla regis prodeunt Vl prt Vnnus Frn (530609) Cn Pir l Ru (c. 1452 151) pr t d,,, r, : mn m p V Qu Im Ar B spn gn sn dm D r p pl br Qu cr ns cn lc s c gt cr n l d r mm t l, cr v n fc 4 R p st d br qu r nt c t qu r r pn prd

More information

Improved Exponential Estimator for Population Variance Using Two Auxiliary Variables

Improved Exponential Estimator for Population Variance Using Two Auxiliary Variables Improvd Epoal Emaor for Populao Varac Ug Two Aular Varabl Rajh gh Dparm of ac,baara Hdu Uvr(U.P., Ida (rgha@ahoo.com Pakaj Chauha ad rmala awa chool of ac, DAVV, Idor (M.P., Ida Flor maradach Dparm of

More information

Face Detection and Recognition. Linear Algebra and Face Recognition. Face Recognition. Face Recognition. Dimension reduction

Face Detection and Recognition. Linear Algebra and Face Recognition. Face Recognition. Face Recognition. Dimension reduction F Dtto Roto Lr Alr F Roto C Y I Ursty O solto: tto o l trs s s ys os ot. Dlt to t to ltpl ws. F Roto Aotr ppro: ort y rry s tor o so E.. 56 56 > pot 6556- stol sp A st o s t ps to ollto o pots ts sp. F

More information

". :'=: "t',.4 :; :::-':7'- --,r. "c:"" --; : I :. \ 1 :;,'I ~,:-._._'.:.:1... ~~ \..,i ... ~.. ~--~ ( L ;...3L-. ' f.':... I. -.1;':'.

. :'=: t',.4 :; :::-':7'- --,r. c: --; : I :. \ 1 :;,'I ~,:-._._'.:.:1... ~~ \..,i ... ~.. ~--~ ( L ;...3L-. ' f.':... I. -.1;':'. = 47 \ \ L 3L f \ / \ L \ \ j \ \ 6! \ j \ / w j / \ \ 4 / N L5 Dm94 O6zq 9 qmn j!!! j 3DLLE N f 3LLE Of ADL!N RALROAD ORAL OR AL AOAON N 5 5 D D 9 94 4 E ROL 2LL RLLAY RL AY 3 ER OLLL 832 876 8 76 L A

More information

Frequency Response. Response of an LTI System to Eigenfunction

Frequency 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 information

Server breakdown and repair, Multiple vacation, Closedown, Balking and Stand-by server.

Server breakdown and repair, Multiple vacation, Closedown, Balking and Stand-by server. OR Jor of Mhc OR-JM -N: 78-578 -N: 9-765 o 6 r No - Dc6 56-74 ororor A G M h o hroo rc rr ro rr M co oo - rr GA r Dr of Mhc ochrr Er o chrr Arc: Th oc of h r o h hor of h rr ro rr M G h o hroo rc co coo

More information

(heat loss divided by total enthalpy flux) is of the order of 8-16 times

(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 information

Numerical Method: Finite difference scheme

Numerical Method: Finite difference scheme Numrcal Mthod: Ft dffrc schm Taylor s srs f(x 3 f(x f '(x f ''(x f '''(x...(1! 3! f(x 3 f(x f '(x f ''(x f '''(x...(! 3! whr > 0 from (1, f(x f(x f '(x R Droppg R, f(x f(x f '(x Forward dffrcg O ( x from

More information

ADORO 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:

ADORO 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 information

P a g e 3 6 of R e p o r t P B 4 / 0 9

P a g e 3 6 of R e p o r t P B 4 / 0 9 P a g e 3 6 of R e p o r t P B 4 / 0 9 p r o t e c t h um a n h e a l t h a n d p r o p e r t y fr om t h e d a n g e rs i n h e r e n t i n m i n i n g o p e r a t i o n s s u c h a s a q u a r r y. J

More information

1. Stefan-Boltzmann law states that the power emitted per unit area of the surface of a black

1. 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 information

B E (c) Figure 2.1.1: (a) a material particle in a body, (b) a place in space, (c) a configuration of the body

B E (c) Figure 2.1.1: (a) a material particle in a body, (b) a place in space, (c) a configuration of the body Kcs Kcs s cocr wh chrcrs o. h ol s o prss hcl for h foro oo of rls. I wh follows r of por qs ly cors sco-orr sors r roc. Ech of hs qs for pl h locy foro r or r of foro sor llows o o scr prclr spc of for

More information

APPLICATION OF CROSS SPECTRUM BASED MODAL IDENTIFICATION TO OUTPUT-ONLY RECORDS OF AMBIENT VIBRATION

APPLICATION OF CROSS SPECTRUM BASED MODAL IDENTIFICATION TO OUTPUT-ONLY RECORDS OF AMBIENT VIBRATION 3 h World Cofrc o Erhqu Egrg Vcouvr,.C., Cd ugus -6, 4 Ppr No. 368 PPLICTION OF CRO PECTRUM ED MODL IDENTIFICTION TO OUTPUT-ONLY RECORD OF MIENT VIRTION K KNZW UMMRY cross spcru bsd odl dfco chqu, whch

More information

F l a t. R o c k. C o n s i g n m e n t. A u c t i o n

F l a t. R o c k. C o n s i g n m e n t. A u c t i o n Kv Brh STUDY, SEPTEMBE 1 LL O THE WILD THE SEPTEMBE POST SESON T THE ZOO SESON HMPIONSHIP NIGHT IN EVIEW I h f yr. Th f h Wd Wh Y Br Nh. B brd, brd, brd. W r w. Th Ow WD r hv 100 h whb d r 10 r; h Ow WD

More information

Total Prime Graph. Abstract: We introduce a new type of labeling known as Total Prime Labeling. Graphs which admit a Total Prime labeling are

Total Prime Graph. Abstract: We introduce a new type of labeling known as Total Prime Labeling. Graphs which admit a Total Prime labeling are Itratoal Joural Of Computatoal Egrg Rsarch (crol.com) Vol. Issu. 5 Total Prm Graph M.Rav (a) Ramasubramaa 1, R.Kala 1 Dpt.of Mathmatcs, Sr Shakth Isttut of Egrg & Tchology, Combator 641 06. Dpt. of Mathmatcs,

More information

2016 Annual Implementation Plan: for Improving Student Outcomes. John Monash Science School Based on Strategic Plan

2016 Annual Implementation Plan: for Improving Student Outcomes. John Monash Science School Based on Strategic Plan 885 J M Scc Sc B Src -9 G fc ffr wr, fr rr b f fr r Vcr r c y. fr rr r: Excc c r rf r c fr r Cy r. Sx c-b c fy ffc, r c-b r w w ccy r r c. r c w fr -w rr, fw wy ( rfr Frwrk fr r S Oc: G fr c): Er rry Er

More information

Approximately Inner Two-parameter C0

Approximately Inner Two-parameter C0 urli Jourl of ic d pplid Scic, 5(9: 0-6, 0 ISSN 99-878 pproximly Ir Two-prmr C0 -group of Tor Produc of C -lgr R. zri,. Nikm, M. Hi Dprm of Mmic, Md rc, Ilmic zd Uivriy, P.O.ox 4-975, Md, Ir. rc: I i ppr,

More information

Unbalanced Panel Data Models

Unbalanced Panel Data Models Ubalacd Pal Data odls Chaptr 9 from Baltag: Ecoomtrc Aalyss of Pal Data 5 by Adrás alascs 4448 troducto balacd or complt pals: a pal data st whr data/obsrvatos ar avalabl for all crosssctoal uts th tr

More information

Excellence in teaching and learning

Excellence in teaching and learning : fr rv S Oc 8 M Ez SC B Src 5-8 Er G v : fr rv S Oc fc ffr wr, fr rr v b f fr r Vcr vr c y. fr rr r: Excc c r rf r v c fr r Cy r. Sx vc-b v c fy ffcv, rv vc-b r w w ccy rv rv c. v r c w fr -w rr, fw wy

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

Symbolic Dynamics for Real Rational Maps

Symbolic Dynamics for Real Rational Maps Symolc Dymcs or Rl Rol Mps João Crl Dprm o Mhmcs o h Azors Uvrsy Po Dlg Porugl ABSTRACT Ths or s mp o suy h ymcs o rl rol mps usg symolc ymcs I s gv mpl h llusrs ho h opologcl ropy c clcul usg g hory Mrov

More information

D. Bertsekas and R. Gallager, "Data networks." Q: What are the labels for the x-axis and y-axis of Fig. 4.2?

D. Bertsekas and R. Gallager, Data networks. Q: What are the labels for the x-axis and y-axis of Fig. 4.2? pd by J. Succ ECE 543 Octob 22 2002 Outl Slottd Aloh Dft Stblzd Slottd Aloh Uslottd Aloh Splttg Algoths Rfc D. Btsks d R. llg "Dt twoks." Rvw (Slottd Aloh): : Wht th lbls fo th x-xs d y-xs of Fg. 4.2?

More information

FOURIER SERIES. Series expansions are a ubiquitous tool of science and engineering. The kinds of

FOURIER SERIES. Series expansions are a ubiquitous tool of science and engineering. The kinds of Do Bgyoko () FOURIER SERIES I. INTRODUCTION Srs psos r ubqutous too o scc d grg. Th kds o pso to utz dpd o () th proprts o th uctos to b studd d (b) th proprts or chrctrstcs o th systm udr vstgto. Powr

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

STA6E NO, LR. Council DeIegote Iouncit Seol. Dqte / / Re-centif. IounciI Delegote Iouncil Seol. Dqie. Sl-oging. This is noi o sionpd subdivision

STA6E NO, LR. Council DeIegote Iouncit Seol. Dqte / / Re-centif. IounciI Delegote Iouncil Seol. Dqie. Sl-oging. This is noi o sionpd subdivision S6, LR PL SBDVS ue ny D Pn umber PS5 4627 Lcqn Ln Pr PHLLP SLD 0WS wnp Secn rwn [[men 15(P, 16 & 17 rwn P e Reerence L Pn Reerence L PS524867K P re c me ubvn MG e n nnnv n n n n pn v01.1028 0L.85 SLM RD

More information

On The Fractional Euler Top System with Two Parameters

On The Fractional Euler Top System with Two Parameters Irol OPEN ACCESS Jourl Of Modr Egrg Rsrh IJMER O Th rol Eulr To Sys wh Two Prrs Mh Iv d Ghorgh Iv Ws Uvrsy of Tşor r of Mhs Srul d Gor ş Toolog 4 B-dul V Pârv Tşor Ro Corrsodg Auhor: Mh Iv W rs h dyl hvor

More information

Vertical Sound Waves

Vertical Sound Waves Vral Sond Wavs On an drv h formla for hs avs by onsdrn drly h vral omonn of momnm qaon hrmodynam qaon and h onny qaon from 5 and hn follon h rrbaon mhod and assmn h snsodal solons. Effvly h frs ro and

More information

Engine Thrust. From momentum conservation

Engine Thrust. From momentum conservation Airbrhing Propulsion -1 Airbrhing School o Arospc Enginring Propulsion Ovrviw w will b xmining numbr o irbrhing propulsion sysms rmjs, urbojs, urbons, urboprops Prormnc prmrs o compr hm, usul o din som

More information

GHOSH, RAHUL. Error analysis of Through Reflect Line method for calibrating

GHOSH, RAHUL. Error analysis of Through Reflect Line method for calibrating Absrc GHOSH, RAHUL. Error lyss of Through Rflc L mhod for clbrg mcrowv msurms. (Udr h drco of Profssor Mchl B. Sr) Ucry rsmsso l bsd clbro chqus for mcrowv msurms r sudd wh h m of dfyg h opmum clbro codos.

More information

Interval Estimation. Consider a random variable X with a mean of X. Let X be distributed as X X

Interval Estimation. Consider a random variable X with a mean of X. Let X be distributed as X X ECON 37: Ecoomercs Hypohess Tesg Iervl Esmo Wh we hve doe so fr s o udersd how we c ob esmors of ecoomcs reloshp we wsh o sudy. The queso s how comforble re we wh our esmors? We frs exme how o produce

More information