used fo developin he sepoin ackin calculao while he exenal is applied fo he conolle synhesis. he as empeaue is applied wih I/O lineaizaion o develop h
|
|
- Andrea Smith
- 5 years ago
- Views:
Transcription
1 empeaue Conol of hemal Cackin Funace wih a Coupled ODE and D-PDEs Model Chawin aweeojkulsi and Chanin Panjaponpon Absac his pape pesens a new conol echnique fo he hemal cackin funace modeled by ses of odinay diffeenial equaion (ODE) and D-paial diffeenial equaions (PDEs). he dynamics of coupled D- PDEs-ODE model have been divided ino subsysems, se of sae vaiables of he inenal and exenal cackin coil. Wih he concep of inpu-oupu (I/O) lineaizaion, hese inne and oue dynamics ae applied o desin he sepoin ackin calculao and he appoximae I/O feedback conolle eecively. he fis-ode eo dynamics and he finie-based, open-loop obseve ae ineaed wih he poposed conolle sysem o compensae he model mismach and o pedic he unmeasued sae infomaion. he pefomances of he poposed mehod ae evaluaed houh he sevo es. he esuls showed ha he conol mehod effecively foces he oupu o he desied sepoin. I. INRODUCION Vinyl chloide monome (VCM) is a aw maeial fo Poly Vinyl Chloide (PVC) poducion. I is ypically obained fom he cackin of,-dichlooehane () unde C, of which hydoen chloide (HCl) is a bypoduc. he eacion can poceed by followin: CH4Cl( ) CH3 Cl ( ) + HCl ( ) () VCM Hydoen Chloide he cackin ae sonly depends on he eacion empeaue; incease on he eacion empeaue esuls in he hih cackin ae. he vapo is eaced alon he lenhy empy coil suended in he chambe of he as-fied cackin funace. Funace dynamics ae hihly nonlinea due o he aial disibued empeaue and concenaion of he as inside he cackin coil, as well as he effec of he empeaue of he funace wall. hese complex behavios lead o deeioae he pefomance of he as empeaue conol by a popoional ineal deivaive (PID) conolle. hey may cause off ec of he poducs, hemal unaway, plan shu down o, in he wos case, explosion. heefoe, he conol mehod ha can handle he empeaue of he cackin funace effecively is needed o achieve a hih qualiy poduc. Reseach woks eadin he empeaue conol of he funace wee mosly focused on he dynamics of he ubula Chanin Panjaponpon (coeondin auho: ex. 30; fencnp@ku.ac.h) and Chawin aweeojkulsi ae wih Cene of Excellence on Peochemical and Maeials echnoloy, Depamen of Chemical Enineein, Faculy of Enineein, Kasesa Univesiy, Bankok 0900, hailand. eaco. Some woks applied he model educion echnique o lump he eaco model befoe pefomin he conolle synhesis. Fo example, he PDE was lumped by Galekin mehod and hen applied wih infinie dimensional sae feedback [] lumped by mehod of chaaceisic and applied wih obus conol [] and lumped by infinie dimensional mehod and applied wih he linea quadaic eulao (QR) [3]. Some woks use he pocess daa o develop an empiical model by he neual newok mehod befoe applied wih he obus conol [4] o eneic model conol (GMC) [5]. Besides, hee ae few woks considein o he ineacion of wall adiaion in he conol of funace. Masoumi and colleaues [6] sudied he empeaue conol of he naphha hemal cackin wih muli cackin coils by usin he PI conolle. he desied sepoins wee obained fom he opimizaion of he empeaue pofile. In Zeybek [7], he oule as empeaue is conolled by manipulain he fuel mass flow ae by usin he adapive heuisic conolle based on hee layes of feed fowad aificial newok (ANN). Panjaponpon e al. [8] poposed he conol of coupled PDE-ODEs fo cackin funace by usin appoximae I/O lineaizaion; he ube empeaue was conolled by manipulain he fuel as flow while he mass poducion ae of VCM was handled by he PI conolle by manipulain he feed. he funace model was developed by assumin a plu-flow velociy pofile and nelecin he effec of he adius hea ansfe. Howeve, hee ae some woks menioned abou sinifican diffeence of pediced pocess dynamics when he edial effec and velociy pofile has been aken ino accouned [9-0]. his bins abou he quesion of he impovemen of conol pefomance when he D model has been applied. In fac, he as empeaue epesened he eacion empeaue is measued by a hemocouple insalled a he cene of he exi ube. he convesion calculaed by he D model will be lowe han he acual pocess value. he pefomance of D-based PDE-ODE conolle in pacice may deeioae due o a sinifican pocess-model mismach. his wok pesens a new sucue of he couplin D PDEs-ODE model fo he cackin funace by usin he I/O lineaizaion. he dynamics of cackin funace consis of he concenaion and as empeaue consideed as he inenal saes and he ube empeaue and funace wall consideed as exenal saes. All he dynamics ae descibed by PDEs excep he funace wall dynamics descibed by ODE. he pupose of his wok is o conol he as empeaue a he exi ube by manipulain he fuel as flow. Insead of applyin he I/O conolle o he objecive diecly, he inenal subsysem is 543
2 used fo developin he sepoin ackin calculao while he exenal is applied fo he conolle synhesis. he as empeaue is applied wih I/O lineaizaion o develop he mappin funcion of he equivalen ube empeaue sepoin fo he I/O feedback conolle. he fis-ode eo dynamics and he finie-based, open-loop obseve ae ineaed ino he conol sysem o eliminae he offse and pedic he unmeasued sae infomaion. An advanae of poposed conol mehod wih he paiionin sae dynamics is o educe he complexiy of he conolle equaion wih a bee pedicin qualiy by usin he D pocess model. II. MAHEMAIC MODE OF CRACKING FURNACE A simple pocess scheme of an cackin funace is shown in Fi.. In he opeaion, vapo is fed o he cackin coil and conveed o be VCM and HCl. he naual as is used as a combusion fuel o supply he eney o he funace o ise up he funace wall empeaue ( w ). he funace wall adiaes and ansfes he eney o he ube inside leadin o he chane of he ube empeaue ( ), he as empeaue ( ) and concenaion (C ) consequenly. In his wok, he poposed conol saey is applied wih D PDEs-ODE model of cackin funace. he followin model assumpions ae applied: ) All ases in he sysem ae ideal. ) Only he eacion in () occuin in he ube is concened. 3) Nelec effecs of all elbows and fiins; saih ube is assumed. 4) he popeies of ases in he ube ae consan. 5) he ube empeaue is vaied alon he z-diecion only because of he pipe hickness << he coil disance. 6) he as empeaue and concenaion ae vaied in boh he adius and disance of he coil. Fi.. Coninuous sied ank eaco wih coolin sysem C C k C = v + + Cp k AFσ C V C i = v + + ( ) p p ''' ( H) + 0 C Ea R p = ke C wih he followin boundaies and iniial condiions: fo he concenaion, BC: C (0, z, ) = 0 BC : C ( Ri, z, ) = 0 BC3 : C (,0, ) = C IC: C (, z,0) = C,0,0 and fo he as empeaue, BC4 : (0, z, ) = 0 BC5: ( Ri, z,) = (,) z BC6 : (,0, ) =,0 IC : (, z, = 0) =,0 he velociy pofile of he as flowin in he coil is efeed o an empiical/analyical soluion of k ε ubulence model in []: dp dz Ri v ( ) =.85 + dp dz Ri Ri ln 0.3 µ 6 dp dz R i whee he oal pessue adien and fannin ficion faco ae appoximaed by usin analyical/empiical equaions poved fom he Moody ficion []: dp P dz f vav P = (4) 4 R i () (3) he dynamic models of he cackin funace ae epesened by followin equaions - he dynamics of concenaion and eaco empeaue in he cackin coil: f 0.84 = 0., Re 0,000 Re 544
3 he aveae velociy is calculaed by R i νav = νz () d R (5) i 0 - he dynamics of ube and funace wall empeaue: AF = + c d w k p, cp V, h, σ ( ) w w π AF σ ( ) ( ) i w ln( R / R ) o i m H σ FA = ( m c ) ( ) fuel comb w w w p w wih he bounday and iniial condiions: BC7 : (0, ) =,0 BC8: (, ) = 0 IC3 : ( z,0) =,0 IC4 : ( z,0) = w w,0 k + Rh All pocess paamees defined in he noaion secion ae iven in able I. he model of he fied-funace in ()-(6) descibed by paial diffeenial equaions in and z coodinaes and odinay diffeenial equaion can be ouped ino wo subsysem. he subsysem of (7.a) expesses he ineacion of he sae vaiables inside he cackin coil and he subsysem in (7.b) expesses he ineacion of he sae vaiables ouside he cackin coil and he adiain wall. xp (, z,) xp xp = a + b + M( xp, xp) (7.a) xp(,) z xp = c + Nx ( p, xo( )) + Ox ( p, xo) dxo () = f( xo, xp, u ( )) y= hx ( ) p wih he iniial and bounday condiions of (7.a): xp (0, z, ) = 0, xp ( Rz,,) BC.. xp ( R, z,) = xp(,) z o = 0, xp (,0,) = xp (,) IC.. x (, z,0) = x (, z) p p,0 and he iniial and bounday condiions of (7.b): o f ] (6) (7.b) able I. PARAMEER VAUES FOR HE CRACKING FURNACE Symbol Quaniy Value A w Aea of he funace wall 8 m C p BC.. IC.. xp(0, ) = xp( ), xp = 0 z= xp( z,0) = xp,0( z), x ( = 0) = x o Aveae hea capaciy of cacked ases o, m 3 C p Hea capaciy of he ube 444 J/k K C pw Hea capaciy of he 000 /k K funace wall D i Inenal ube diamee 0.9 m E a Acivaion eney J/mol F Shape faco H Hea of eacion J/mol H comb Hea of combusion J/mol k 0 Kineic consan k k hemal conduciviy of ases in ube hemal conduciviy of he W/m K 0.5 W/m K ube ube lenh 300 m m ube weih k m w Mass of funace wall k m f Mass flow ae of he fuel k/s Mw molecula weih /mol Pe hemal Pecle numbe P Pandl numbe 0.7 R Gas consan 8.34 J/mol K R i Inenal ube adius m R o Exenal ube adius 0. m Re Reynolds numbe V Pipe volume m 3 Cacked as densiy k/m 3 ube densiy 8470 k/m 3 σ Sefan-Bolzman consan W/m K µ Viscosiy of cacked ases k/m s ν Feed velociy 5 m/s whee xp (, z,) denoes he veco of he sae vaiables dependin on and z coodinaes, x (,) p z denoes he sae vaiable of he exenal ube dynamics which is diecly 545
4 affeced by x o, xo () denoes he sae vaiable which depend on ime, y denoe he oupu vaiable, z [0, ] and [0, R o ] ae aial coodinaes, [0, ] is he ime, and u () is he manipulaed vaiable. III. CONRO SYSEM DESIGN In ou case, he pocess model is hihly complex due o coupled PDEs and ODE. he conol objecive is o eulae he oupu a he exi of he ube (y=), he sae in he subsysem (7.a), by adjusin he inpu (u) in he subsysem (7.b). o educe complexiy of he conolle desin, in his wok, he se of PDE in (7.a) descibed he inenal ube dynamics will be used o ceae a ackin coelaion beween he oupu ( y ) and he disibued sae vaiable elaed o he lumped dynamics ( x ). he se of couplin p PDEs-ODE in (7.b) descibed he exenal ube dynamics will be used o develop he I/O feedback conolle ha he conol acion ( u ) is obained by solvin closed-loop eonse of x. A schemaic diaam of he conol sysem p shown in Fi. is poposed. he conol sysem consiss of a sepoin ackin calculao, I/O lineaizin conolle, and a finie-based, open-loop obseve. Moe deails of he conol sysem desin ae iven as follows. A. Sepoin ackin calculao he inpu/oupu lineaizaion is a mehod ha ceaes a linea elaionship beween inpu and oupu based on he coodinae ansfomaion. I is adiionally applied fo he ODE sysem. Fo he applicaion of PDEs-ODEs sysem, le conside he sysem in (8). dx = f( x, x, x, xz, xzz, u) y = hx ( ) = = 0, z whee x is he veco of sae vaiables, x z = x z and x = x ae he fis-ode aial deivaives of x (8) eec o z-diecion and -diecions, xzz = x z and x = x ae he second-ode aial deivaives of x eec o z-diecion and -diecion, u is he manipulaed inpu and h is he veco of nonlinea funcions. he elaive ode of he conolled oupu y,, can be defined by followin noaion: y = h ( x) = 0, z= dy h x h ( x, x, x, xz, xzz ) x = z= h x h x h x d = 0, z= + + y x x x h xz h xzz xz xzz = h ( xzz ) = 0, z= x x x, x, x, xz, xzz,,, ( x ),,, xz xzz ( x ),,, ( ),,, ( ) x z x zz h x h x h x + + x x x h xz h xzz ( x ) zz xz xzz = 0, z= d y x x x, x, x, xz, xzz,,, ( x ),,, = h xz xzz ( x ),,, ( ),,, ( ), x z x zz u = 0, z= = 0, z= he sepoin ackin calculao is applied o develop a coelaion beween y x p. Fom he subsysem (7.a), he closed-loop eonse of he oupu a he cene of he exi ube is in linea fom as follows: (9) Fi.. Schemaic diaam of he poposed conol sysem. 546
5 ( ε + ) y = y, (0) whee is he diffeenial opeao, y is he oupu a he posiion =0 and z=, y, is he desied sepoin, ε is he unin paamee used o adjus he eed of he oupu eonse and is he elaive ode of y wih eec o x. p By subsiuin he ime deivaives of (9) ino (0) and sein all ime deivaives of he sae adiens o be zeo, he closed-loop eonses of he oupu can be pesened in a compac fom φ ( x, x, x, x, x ) = y () p p, p, p, z p, he ackin sepoin funcion (ν ) of can be obained by solvin () fo x p, in followin fom: ν = ψ ( x, x, x, x, x, y ) () p p, p, p, z p, B. Feedback I/O lineaizin conolle Fom he subsysem (7.b), he closed-loop eonses of he sae xp a he posiion z= ae equesed in linea fom as follows: ( β ) xp + = ν (3) whee ν is he ackin sepoin funcion, β is he unin paamee and is he elaive ode of xp wih eec o u. We subsiue he ime deivaive in (9) ino (3) and se all ime deivaives of he sae adiens o be zeo. he closed-loop eonses of he sae xp can be pesened in a compac fom φ ( x, x, x, u) = ν (4) p p zz hus, he feedback conolle (u) is obained by solvin (4). he compac fom of he conolle equaion is denoed by (5) u = Ψ ( x, x, x, ν ) (5) p p zz C. Finie-based sae obseve he CFD echnique is a useful ool o pedic behavio of he sysem of he complex PDE poblem by usin he numeical calculaion. hus, in his wok, a CFD-based, open-loop sae obseve is developed o povide he esimaion of he unmeasued pocess concenaion, C, and he sae deivaives. D. Ineao o compensae he pocess-model mismach and he eo fom he esimae saes, he fis-ode eo dynamics in (6) is applied: ε ν = λ ( y y) = y ε = 0, z= (6) ε whee is he oupu eo, ν is he coeced sepoin. λ is a posiive paamee, and IV. RESU AND DISCUSSION he velociy wih plu-flow paen is pimaily assumed in many lieaues fo a conol of he ubula eaco. Howeve, his assumpion is pope fo a hih viscosiy fluid. o achieve a ealisic pedicion, he k ε ubulence model is applied wih he developed D model, which he compaed velociy pofiles ae shown in Fi.3. Fo he sevo es, he as empeaue a exi ube is conolled a he desied sepoin y = 700 K. he iniial condiions of he dynamics ae C (,0,) = mol/l, (,0,)=644 K, (0,)= 76 K, and w =808 K. he unin paamees of he poposed conol sysem ae ε =8, β =8 and λ =0.00. he closed-loop eonses of he cackin funace ae illusaed in Fis he esuls show ha Velociy (m/s) k ε Plu flow Radius (m) Fi.3. he flow paen of cacked as inside he ube. Gas empeaue (K) Poposed conolle Sepoin ime (min) Fi.4. he closed-loop eonse of he as empeaue a he cene exi ube. 547
6 empeaue (K) Fi.5. he closed-loop eonses of he ube empeaue a he exi and wall empeaue. Mass fuel flow (k/s) ime (min) ime (min) Fi.6. he conol acion of he manipulaed inpu. w he conolle successfully foces he as empeaue a he desied sepoin. he chanes of as, ube and wall empeaue a he iniial peiod have a linea end due o he influence fom he consan of fuel as ae a he uppe limi. he conolle is hen adjused he fuel as flow wih a lile fuzzy o pu he as empeaue a he desied sepoin. ACKNOWEDGMEN his wok was financially suppoed by he Kasesa Univesiy Reseach and Developmen Insiue (KURDI), he pojec fo Hihe Educaion Reseach Pomoion and Naional Reseach Univesiy Developmen, Office of he Hihe Educaion Commission, and he Cene of Excellence on Peochemicals and Maeials echnoloy. hese suppos ae aefully acknowleded. REFERENCES [] Shan, H., Fase Fobes, J., Guay, M., 005. Feedback conol of hypebolic disibued paamee sysems. Chemical Enineein Science 60, [] Hoo, K.A., Zhen, D., 00. ow-ode conol-elevan models fo a class of disibued paamee sysems. Chemical Enineein Science 56, [3] Mohadam, A.A., Aksikas, I., Dubljevic, S., Fobes, J.F., 00. Q conol of coupled hypebolic PDEs and ODEs: Applicaion o a CSR PFR sysem, in Poceedins of he Ninh Inenaional Symposium on Dynamics and Conol of Pocess Sysems. pp [4] Yamuna Rani, K., Pawadhan, S.C., 007. Daa-Diven Model Based Conol of a Muli-Poduc Semi-Bach Polymeizaion Reaco. Chemical Enineein Reseach and Desin 85, [5] Aeloiannaki, E., Saimveis, H., 009. Robus nonlinea H conol of hypebolic disibued paamee sysems. Conol Enineein Pacice 7, [6] Masoumi, M.E., Sadameli, S.M., owfihi, J., Niaei, A., 006. Simulaion, opimizaion and conol of a hemal cackin funace. Eney 3, [7] Zeybek, Z., 006. Role of adapive heuisic ciicism in cascade empeaue conol of an indusial ubula funace. Applied hemal Enineein 6, [8] Panjaponpon, C., impanachaiponkul, P., Chainpanikul,., 0. Conol of coupled PDEs ODEs usin inpu oupu lineaizaion: Applicaion o a cackin funace. Chemical Enineein Science 75, [9] Van Geem, K.M., Heyndeickx, G.J., Main, G.B., 004. Effec of adial empeaue pofiles on yields in seam cackin. AIChE jounal 50, [0] Han, Y.., Xiao, R., Zhan, M.Y., 007. Combusion and Pyolysis Reacions in a Naphha Cackin Funace. Chemical Enineein & echnoloy 30, 0. doi:0.00/cea [] Mecado, E.R.., Nunhez, J.R., 000. Modelaem do aquecimeno de fluidos com escoameno em ubos [WWW Documen]. UR hp:// 788 (accessed.0.4). [] Incopea, F., Dewi, D., 00. Fundamenals of Hea and Mass ansfe, 5 h ed. John Wiley & Sons, New Yok V. CONCUSION A new conolle sucue wih I/O lineaizaion echnique is developed fo he cackin funace, of which he advanaes ae a few unin paamees and decease on he complexiy of he conolle equaion. Wih he impoance of he disibuion in -diecion of fluid flow in he ube, he k ε ubulen model is applied o he velociy. he conolle is fomulaed wih he D-PDEs and ODE ino he sepoin ackin calculao and I/O feedback conolle, and ineaed wih he fis-ode eo dynamics and finie-based, open-loop obseve. he simulaion esuls show ha he conolle can foce he conol oupu a he desied sepoin effecively. 548
On Control Problem Described by Infinite System of First-Order Differential Equations
Ausalian Jounal of Basic and Applied Sciences 5(): 736-74 ISS 99-878 On Conol Poblem Descibed by Infinie Sysem of Fis-Ode Diffeenial Equaions Gafujan Ibagimov and Abbas Badaaya J'afau Insiue fo Mahemaical
More information, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t
Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission
More informationLecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain
Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as
More informationLow-complexity Algorithms for MIMO Multiplexing Systems
Low-complexiy Algoihms fo MIMO Muliplexing Sysems Ouline Inoducion QRD-M M algoihm Algoihm I: : o educe he numbe of suviving pahs. Algoihm II: : o educe he numbe of candidaes fo each ansmied signal. :
More informationThe sudden release of a large amount of energy E into a background fluid of density
10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy
More informationOrthotropic Materials
Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε
More informationCircular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.
1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule
More informationLecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation
Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion
More informationAn Open cycle and Closed cycle Gas Turbine Engines. Methods to improve the performance of simple gas turbine plants
An Open cycle and losed cycle Gas ubine Engines Mehods o impove he pefomance of simple gas ubine plans I egeneaive Gas ubine ycle: he empeaue of he exhaus gases in a simple gas ubine is highe han he empeaue
More informationSTUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION
Inenaional Jounal of Science, Technology & Managemen Volume No 04, Special Issue No. 0, Mach 205 ISSN (online): 2394-537 STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE
More informationFluid Flow and Heat Transfer Characteristics across an Internally Heated Finned Duct
J. Enegy Powe Souces ol. No. 6 4 pp. 96-33 ceived: Augus 3 4 Published: Decembe 3 4 Jounal of Enegy and Powe Souces www.ehanpublishing.com Fluid Flow and ea ansfe Chaaceisics acoss an Inenally eaed Finned
More informationCS 188: Artificial Intelligence Fall Probabilistic Models
CS 188: Aificial Inelligence Fall 2007 Lecue 15: Bayes Nes 10/18/2007 Dan Klein UC Bekeley Pobabilisic Models A pobabilisic model is a join disibuion ove a se of vaiables Given a join disibuion, we can
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationCombinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions
Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,
More informationr P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,
Lecue 36 Pipe Flow and Low-eynolds numbe hydodynamics 36.1 eading fo Lecues 34-35: PKT Chape 12. Will y fo Monday?: new daa shee and daf fomula shee fo final exam. Ou saing poin fo hydodynamics ae wo equaions:
More informationEFFECT OF PERMISSIBLE DELAY ON TWO-WAREHOUSE INVENTORY MODEL FOR DETERIORATING ITEMS WITH SHORTAGES
Volume, ssue 3, Mach 03 SSN 39-4847 EFFEC OF PERMSSBLE DELAY ON WO-WAREHOUSE NVENORY MODEL FOR DEERORANG EMS WH SHORAGES D. Ajay Singh Yadav, Ms. Anupam Swami Assisan Pofesso, Depamen of Mahemaics, SRM
More informationKINEMATICS OF RIGID BODIES
KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid
More informationThe Production of Polarization
Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview
More information7 Wave Equation in Higher Dimensions
7 Wave Equaion in Highe Dimensions We now conside he iniial-value poblem fo he wave equaion in n dimensions, u c u x R n u(x, φ(x u (x, ψ(x whee u n i u x i x i. (7. 7. Mehod of Spheical Means Ref: Evans,
More informationServomechanism Design
Sevomechanism Design Sevomechanism (sevo-sysem) is a conol sysem in which he efeence () (age, Se poin) changes as ime passes. Design mehods PID Conol u () Ke P () + K I ed () + KDe () Sae Feedback u()
More informationAN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS
AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS M. KAMESWAR RAO AND K.P. RAVINDRAN Depamen of Mechanical Engineeing, Calicu Regional Engineeing College, Keala-67 6, INDIA. Absac:- We eploe
More informationReinforcement learning
Lecue 3 Reinfocemen leaning Milos Hauskech milos@cs.pi.edu 539 Senno Squae Reinfocemen leaning We wan o lean he conol policy: : X A We see examples of x (bu oupus a ae no given) Insead of a we ge a feedback
More informationGeneral Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security
1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,
More informationA Negative Log Likelihood Function-Based Nonlinear Neural Network Approach
A Negaive Log Likelihood Funcion-Based Nonlinea Neual Newok Appoach Ponip Dechpichai,* and Pamela Davy School of Mahemaics and Applied Saisics Univesiy of Wollongong, Wollongong NSW 5, AUSTRALIA * Coesponding
More informationMonochromatic Wave over One and Two Bars
Applied Mahemaical Sciences, Vol. 8, 204, no. 6, 307-3025 HIKARI Ld, www.m-hikai.com hp://dx.doi.og/0.2988/ams.204.44245 Monochomaic Wave ove One and Two Bas L.H. Wiyano Faculy of Mahemaics and Naual Sciences,
More informationResearch on the Algorithm of Evaluating and Analyzing Stationary Operational Availability Based on Mission Requirement
Reseach on he Algoihm of Evaluaing and Analyzing Saionay Opeaional Availabiliy Based on ission Requiemen Wang Naichao, Jia Zhiyu, Wang Yan, ao Yilan, Depamen of Sysem Engineeing of Engineeing Technology,
More informationMATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH
Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias
More informationInput-output linearizing control of a thermal cracking furnace described by a coupled PDE-ODE system
Prerins of he 10h IFAC Inernaional Symosium on Dynamics and Conrol of Process Sysems The Inernaional Federaion of Auomaic Conrol Inu-ouu lineariin conrol of a hermal crackin furnace described by a couled
More informationDesign Guideline for Buried Hume Pipe Subject to Coupling Forces
Design Guideline fo Buied Hume Pipe Sujec o Coupling Foces Won Pyo Hong 1), *Seongwon Hong 2), and Thomas Kang 3) 1) Depamen of Civil, nvionmenal and Plan ngineeing, Chang-Ang Univesiy, Seoul 06974, Koea
More informationTheoretical background and the flow fields in downhole liquid-liquid hydrocyclone (LLHC)
AEC Web of Confeences 13, 3 (14) DO: 1.151/ maecconf/ 1413 3 C Owned by he auhos, published by EDP Sciences, 14 heoeical backgound and he flow fields in downhole liquid-liquid hydocyclone (LLHC) Haison
More informationAn Automatic Door Sensor Using Image Processing
An Auomaic Doo Senso Using Image Pocessing Depamen o Elecical and Eleconic Engineeing Faculy o Engineeing Tooi Univesiy MENDEL 2004 -Insiue o Auomaion and Compue Science- in BRNO CZECH REPUBLIC 1. Inoducion
More informationTwo-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch
Two-dimensional Effecs on he CS Ineacion Foces fo an Enegy-Chiped Bunch ui Li, J. Bisognano,. Legg, and. Bosch Ouline 1. Inoducion 2. Pevious 1D and 2D esuls fo Effecive CS Foce 3. Bunch Disibuion Vaiaion
More informationProbabilistic Models. CS 188: Artificial Intelligence Fall Independence. Example: Independence. Example: Independence? Conditional Independence
C 188: Aificial Inelligence Fall 2007 obabilisic Models A pobabilisic model is a join disibuion ove a se of vaiables Lecue 15: Bayes Nes 10/18/2007 Given a join disibuion, we can eason abou unobseved vaiables
More informationA Numerical Hydration Model of Portland Cement
A Numeical Hydaion Model of Poland Cemen Ippei Mauyama, Tesuo Masushia and Takafumi Noguchi ABSTRACT : A compue-based numeical model is pesened, wih which hydaion and micosucual developmen in Poland cemen-based
More informationSections 3.1 and 3.4 Exponential Functions (Growth and Decay)
Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens
More informationLecture 22 Electromagnetic Waves
Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should
More informationA Study on Non-Binary Turbo Codes
A Sudy on Non-Binay Tubo Codes Hoia BALTA, Maia KOVACI Univesiy Polyechnic of Timişoaa, Faculy of Eleconics and Telecommunicaions, Posal Addess, 3223 Timişoaa, ROMANIA, E-Mail: hoia.bala@ec.u.o, maia.kovaci@ec.u.o
More informationRisk tolerance and optimal portfolio choice
Risk oleance and opimal pofolio choice Maek Musiela BNP Paibas London Copoae and Invesmen Join wok wih T. Zaiphopoulou (UT usin) Invesmens and fowad uiliies Pepin 6 Backwad and fowad dynamic uiliies and
More informationÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s
MÜHENDİSLİK MEKANİĞİ. HAFTA İMPULS- MMENTUM-ÇARPIŞMA Linea oenu of a paicle: The sybol L denoes he linea oenu and is defined as he ass ies he elociy of a paicle. L ÖRNEK : THE LINEAR IMPULSE-MMENTUM RELATIN
More informationME 304 FLUID MECHANICS II
ME 304 LUID MECHNICS II Pof. D. Haşme Tükoğlu Çankaya Uniesiy aculy of Engineeing Mechanical Engineeing Depamen Sping, 07 y du dy y n du k dy y du k dy n du du dy dy ME304 The undamenal Laws Epeience hae
More informationComputer Propagation Analysis Tools
Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion
More informationPseudosteady-State Flow Relations for a Radial System from Department of Petroleum Engineering Course Notes (1997)
Pseudoseady-Sae Flow Relaions fo a Radial Sysem fom Deamen of Peoleum Engineeing Couse Noes (1997) (Deivaion of he Pseudoseady-Sae Flow Relaions fo a Radial Sysem) (Deivaion of he Pseudoseady-Sae Flow
More informationMEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING
MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens
More information156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2
156 Thee ae 9 books sacked on a shelf. The hickness of each book is eihe 1 inch o 2 F inches. The heigh of he sack of 9 books is 14 inches. Which sysem of equaions can be used o deemine x, he numbe of
More informationTurbulent buoyant confined jet with variable source temperature
Tubulen buoyan confined je wih vaiable souce empeaue M. F. El-Amin 1,, Amgad Salama 1 and Shuyu Sun 1 1 King Abdullah Univesiy of Science and Technology (KAUST), Thuwal 3955-6900, Kingdom of Saudi Aabia
More informationKalman Filter: an instance of Bayes Filter. Kalman Filter: an instance of Bayes Filter. Kalman Filter. Linear dynamics with Gaussian noise
COM47 Inoducion o Roboics and Inelligen ysems he alman File alman File: an insance of Bayes File alman File: an insance of Bayes File Linea dynamics wih Gaussian noise alman File Linea dynamics wih Gaussian
More informationTransient convective heat and mass transfer flow in an axially varying pipe with traveling thermal wave
Available online a www.pelaiaeseachlibay.com Pelaia Reseach Libay Advances in Applied Science Reseach 6 7:55-65 ISS: 976-86 OD USA: AASR ansien convecive hea and mass ansfe flow in an aially vayin pipe
More informationElastic-Plastic Deformation of a Rotating Solid Disk of Exponentially Varying Thickness and Exponentially Varying Density
Poceedings of he Inenaional MuliConfeence of Enginees Compue Scieniss 6 Vol II, IMECS 6, Mach 6-8, 6, Hong Kong Elasic-Plasic Defomaion of a Roaing Solid Dis of Exponenially Vaying hicness Exponenially
More informationWORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done
More informationHeat Conduction Problem in a Thick Circular Plate and its Thermal Stresses due to Ramp Type Heating
ISSN(Online): 319-8753 ISSN (Pin): 347-671 Inenaional Jounal of Innovaive Reseac in Science, Engineeing and Tecnology (An ISO 397: 7 Ceified Oganiaion) Vol 4, Issue 1, Decembe 15 Hea Concion Poblem in
More informationNumerical solution of fuzzy differential equations by Milne s predictor-corrector method and the dependency problem
Applied Maemaics and Sciences: An Inenaional Jounal (MaSJ ) Vol. No. Augus 04 Numeical soluion o uzz dieenial equaions b Milne s pedico-coeco meod and e dependenc poblem Kanagaajan K Indakuma S Muukuma
More informationRepresenting Knowledge. CS 188: Artificial Intelligence Fall Properties of BNs. Independence? Reachability (the Bayes Ball) Example
C 188: Aificial Inelligence Fall 2007 epesening Knowledge ecue 17: ayes Nes III 10/25/2007 an Klein UC ekeley Popeies of Ns Independence? ayes nes: pecify complex join disibuions using simple local condiional
More information( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba
THE INTEACTION OF ADIATION AND MATTE: SEMICLASSICAL THEOY PAGE 26 III. EVIEW OF BASIC QUANTUM MECHANICS : TWO -LEVEL QUANTUM SYSTEMS : The lieaue of quanum opics and lase specoscop abounds wih discussions
More information[ ] 0. = (2) = a q dimensional vector of observable instrumental variables that are in the information set m constituents of u
Genealized Mehods of Momens he genealized mehod momens (GMM) appoach of Hansen (98) can be hough of a geneal pocedue fo esing economics and financial models. he GMM is especially appopiae fo models ha
More informationPressure Vessels Thin and Thick-Walled Stress Analysis
Pessue Vessels Thin and Thick-Walled Sess Analysis y James Doane, PhD, PE Conens 1.0 Couse Oveview... 3.0 Thin-Walled Pessue Vessels... 3.1 Inoducion... 3. Sesses in Cylindical Conaines... 4..1 Hoop Sess...
More informationEffect of Wall Absorption on dispersion of a solute in a Herschel Bulkley Fluid through an annulus
Available online a www.pelagiaeseachlibay.com Advances in Applied Science Reseach,, 3 (6):3878-3889 ISSN: 976-86 CODEN (USA): AASRFC Effec of Wall Absopion on dispesion of a solue in a Heschel Bulley Fluid
More informationFeedback Couplings in Chemical Reactions
Feedback Coulings in Chemical Reacions Knud Zabocki, Seffen Time DPG Fühjahsagung Regensbug Conen Inoducion Moivaion Geneal model Reacion limied models Diffusion wih memoy Oen Quesion and Summay DPG Fühjahsagung
More informationAnalysis of Microstrip Coupling Gap to Estimate Polymer Permittivity
Analysis of Microsrip Couplin Gap o Esimae Polymer Permiiviy Chanchal Yadav Deparmen of Physics & Elecronics Rajdhani Collee, Universiy of Delhi Delhi, India Absrac A ap in he microsrip line can be modeled
More informationEfficient experimental detection of milling stability boundary and the optimal axial immersion for helical mills
Efficien expeimenal deecion of milling sabiliy bounday and he opimal axial immesion fo helical mills Daniel BACHRATHY Depamen of Applied Mechanics, Budapes Univesiy of Technology and Economics Muegyeem
More informationON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS
Mem. Fac. Inegaed As and Sci., Hioshima Univ., Se. IV, Vol. 8 9-33, Dec. 00 ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS YOSHIO AGAOKA *, BYUNG HAK KIM ** AND JIN HYUK CHOI ** *Depamen of Mahemaics, Faculy
More informationChapter Finite Difference Method for Ordinary Differential Equations
Chape 8.7 Finie Diffeence Mehod fo Odinay Diffeenial Eqaions Afe eading his chape, yo shold be able o. Undesand wha he finie diffeence mehod is and how o se i o solve poblems. Wha is he finie diffeence
More informationPHYS PRACTICE EXAM 2
PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,
More informationOn the Semi-Discrete Davey-Stewartson System with Self-Consistent Sources
Jounal of Applied Mahemaics and Physics 25 3 478-487 Published Online May 25 in SciRes. hp://www.scip.og/jounal/jamp hp://dx.doi.og/.4236/jamp.25.356 On he Semi-Discee Davey-Sewason Sysem wih Self-Consisen
More informationInternational Journal of Pure and Applied Sciences and Technology
In. J. Pue Appl. Sci. Technol., 4 (211, pp. 23-29 Inenaional Jounal of Pue and Applied Sciences and Technology ISS 2229-617 Available online a www.ijopaasa.in eseach Pape Opizaion of he Uiliy of a Sucual
More informationOn Energy-Efficient Node Deployment in Wireless Sesnor Networks
I J Communicaions, Newok and Sysem Sciences, 008, 3, 07-83 Published Online Augus 008 in Scies (hp://wwwscipog/jounal/ijcns/) On Enegy-Efficien Node Deploymen in Wieless Sesno Newoks Hui WANG 1, KeZhong
More informationDepartment of Chemical Engineering University of Tennessee Prof. David Keffer. Course Lecture Notes SIXTEEN
D. Keffe - ChE 40: Hea Tansfe and Fluid Flow Deamen of Chemical Enee Uniesi of Tennessee Pof. Daid Keffe Couse Lecue Noes SIXTEEN SECTION.6 DIFFERENTIL EQUTIONS OF CONTINUITY SECTION.7 DIFFERENTIL EQUTIONS
More informationThe k-filtering Applied to Wave Electric and Magnetic Field Measurements from Cluster
The -fileing pplied o Wave lecic and Magneic Field Measuemens fom Cluse Jean-Louis PINÇON and ndes TJULIN LPC-CNRS 3 av. de la Recheche Scienifique 4507 Oléans Fance jlpincon@cns-oleans.f OUTLINS The -fileing
More informationFig. 1S. The antenna construction: (a) main geometrical parameters, (b) the wire support pillar and (c) the console link between wire and coaxial
a b c Fig. S. The anenna consucion: (a) ain geoeical paaees, (b) he wie suppo pilla and (c) he console link beween wie and coaial pobe. Fig. S. The anenna coss-secion in he y-z plane. Accoding o [], he
More informationLecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light
Lecue 5 Chape 3 lecomagneic Theo, Phoons, and Ligh Gauss s Gauss s Faada s Ampèe- Mawell s + Loen foce: S C ds ds S C F dl dl q Mawell equaions d d qv A q A J ds ds In mae fields ae defined hough ineacion
More informationNUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS
Join Inenaional Confeence on Compuing and Decision Making in Civil and Building Engineeing June 14-16, 26 - Monéal, Canada NUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS ABSTRACT
More informationFINITE DIFFERENCE APPROACH TO WAVE GUIDE MODES COMPUTATION
FINITE DIFFERENCE ROCH TO WVE GUIDE MODES COMUTTION Ing.lessando Fani Elecomagneic Gou Deamen of Elecical and Eleconic Engineeing Univesiy of Cagliai iazza d mi, 93 Cagliai, Ialy SUMMRY Inoducion Finie
More informationAST1100 Lecture Notes
AST00 Lecue Noes 5 6: Geneal Relaiviy Basic pinciples Schwazschild geomey The geneal heoy of elaiviy may be summaized in one equaion, he Einsein equaion G µν 8πT µν, whee G µν is he Einsein enso and T
More informationLecture 20: Riccati Equations and Least Squares Feedback Control
34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he
More informationA Weighted Moving Average Process for Forecasting. Shou Hsing Shih Chris P. Tsokos
A Weighed Moving Aveage Pocess fo Foecasing Shou Hsing Shih Chis P. Tsokos Depamen of Mahemaics and Saisics Univesiy of Souh Floida, USA Absac The objec of he pesen sudy is o popose a foecasing model fo
More informationLawsoftheElectroElectricalInduction
Global Jounal of Reseaches in Engineeing: F Elecical and Eleconics Engineeing Volume 15 Issue 9 Vesion 1. Yea 15 Type: Double Blind Pee Reviewed Inenaional Reseach Jounal Publishe: Global Jounals Inc.
More informationOn The Estimation of Two Missing Values in Randomized Complete Block Designs
Mahemaical Theoy and Modeling ISSN 45804 (Pape ISSN 505 (Online Vol.6, No.7, 06 www.iise.og On The Esimaion of Two Missing Values in Randomized Complee Bloc Designs EFFANGA, EFFANGA OKON AND BASSE, E.
More information336 ERIDANI kfk Lp = sup jf(y) ; f () jj j p p whee he supemum is aken ove all open balls = (a ) inr n, jj is he Lebesgue measue of in R n, () =(), f
TAMKANG JOURNAL OF MATHEMATIS Volume 33, Numbe 4, Wine 2002 ON THE OUNDEDNESS OF A GENERALIED FRATIONAL INTEGRAL ON GENERALIED MORREY SPAES ERIDANI Absac. In his pape we exend Nakai's esul on he boundedness
More informationDYNAMIC ANALYSIS AND CONTROL OF ACTIVE ENGINE MOUNT SYSTEM
To be submied o Jounal of Auomobile Engineeing DYNAMIC ANALYSIS AND CONTROL OF ACTIVE ENGINE MOUNT SYSTEM by Yong-Wook Lee and Chong-Won Lee Cene fo Noise and Vibaion Conol (NOVIC) Depamen of Mechanical
More informationSynchronization of Fractional Chaotic Systems via Fractional-Order Adaptive Controller
Synchonizaion of Facional Chaoic Sysems via Facional-Ode Adapive Conolle S.H. Hosseinnia*, R. Ghadei*, A. Ranjba N.*, J. Sadai*, S. Momani** * Noshivani Univesiy of Technology, Faculy of Elecical Compue
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More informationExponential and Logarithmic Equations and Properties of Logarithms. Properties. Properties. log. Exponential. Logarithmic.
Eponenial and Logaihmic Equaions and Popeies of Logaihms Popeies Eponenial a a s = a +s a /a s = a -s (a ) s = a s a b = (ab) Logaihmic log s = log + logs log/s = log - logs log s = s log log a b = loga
More informationMIMO Cognitive Radio Capacity in. Flat Fading Channel. Mohan Premkumar, Muthappa Perumal Chitra. 1. Introduction
Inenaional Jounal of Wieless Communicaions, ewoking and Mobile Compuing 07; 4(6): 44-50 hp://www.aasci.og/jounal/wcnmc ISS: 38-37 (Pin); ISS: 38-45 (Online) MIMO Cogniive adio Capaciy in Fla Fading Channel
More informationThe shortest path between two truths in the real domain passes through the complex domain. J. Hadamard
Complex Analysis R.G. Halbud R.Halbud@ucl.ac.uk Depamen of Mahemaics Univesiy College London 202 The shoes pah beween wo uhs in he eal domain passes hough he complex domain. J. Hadamad Chape The fis fundamenal
More informationSliding Mode Controller for Unstable Systems
S. SIVARAMAKRISHNAN e al., Sliding Mode Conroller for Unsable Sysems, Chem. Biochem. Eng. Q. 22 (1) 41 47 (28) 41 Sliding Mode Conroller for Unsable Sysems S. Sivaramakrishnan, A. K. Tangirala, and M.
More informationSub Module 2.6. Measurement of transient temperature
Mechanical Measuremens Prof. S.P.Venkaeshan Sub Module 2.6 Measuremen of ransien emperaure Many processes of engineering relevance involve variaions wih respec o ime. The sysem properies like emperaure,
More informationResearch Article Stress Analysis of Nonhomogeneous Rotating Disc with Arbitrarily Variable Thickness Using Finite Element Method
Reseach Jounal of Applied Sciences, Engineeing and Technology 7(15): 3114-315, 014 DOI:10.1906/jase.7.650 ISSN: 040-7459; e-issn: 040-7467 014 Maxwell Scienific Publicaion Cop. Submied: Ocobe 09, 013 Acceped:
More informationANALYTICAL SOLUTION FOR EDDY CURRENT PROBLEM, USING SPACE EIGENFUNCTIONS EXPANSION
ANALYTICAL SOLUTION FOR EDDY CURRENT PROBLEM, USING SPACE EIGENFUNCTIONS EXPANSION MARILENA STĂNCULESCU, MIHAI MARICARU, VALERIU ŞTEFAN-MINCULETE, STELIAN MARINESCU, IOAN FLOREA HĂNŢILĂ Key wods: Analyical
More informationd 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3
and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or
More informationModelling Hydromechanical Dilation Geomaterial Cavitation and Localization
Modelling Hydomechanical Dilaion Geomaeial Caviaion and Localizaion Y. Sieffe, O. Buzzi, F. Collin and R. Chambon Absac This pape pesens an exension of he local second gadien model o muliphasic maeials
More informationDiscretization of Fractional Order Differentiator and Integrator with Different Fractional Orders
Inelligen Conol and Auomaion, 207, 8, 75-85 hp://www.scip.og/jounal/ica ISSN Online: 253-066 ISSN Pin: 253-0653 Disceizaion of Facional Ode Diffeeniao and Inegao wih Diffeen Facional Odes Qi Zhang, Baoye
More informationMeasures the linear dependence or the correlation between r t and r t-p. (summarizes serial dependence)
. Definiions Saionay Time Seies- A ime seies is saionay if he popeies of he pocess such as he mean and vaiance ae consan houghou ime. i. If he auocoelaion dies ou quickly he seies should be consideed saionay
More informationDynamic Operational Optimization of Air Source Heat Pump Heating System with the Consideration of Energy Saving
Pepins of he 9h Inenaional Symposium on Advanced Conol of Chemical Pocesses The Inenaional Fedeaion of Auomaic Conol June 7-1, 15, Whisle, Biish Columbia, Canada TuA.6 Dynamic Opeaional Opimiaion of Ai
More informationMECHANICS OF MATERIALS Poisson s Ratio
Fouh diion MCHANICS OF MATRIALS Poisson s Raio Bee Johnson DeWolf Fo a slende ba subjeced o aial loading: 0 The elongaion in he -diecion is accompanied b a conacion in he ohe diecions. Assuming ha he maeial
More informationP h y s i c s F a c t s h e e t
P h y s i c s F a c s h e e Sepembe 2001 Numbe 20 Simple Hamonic Moion Basic Conceps This Facshee will:! eplain wha is mean by simple hamonic moion! eplain how o use he equaions fo simple hamonic moion!
More informationThe Global Trade and Environment Model: GTEM
The Global Tade and Envionmen Model: A pojecion of non-seady sae daa using Ineempoal GTEM Hom Pan, Vivek Tulpulé and Bian S. Fishe Ausalian Bueau of Agiculual and Resouce Economics OBJECTIVES Deive an
More informationVehicle Arrival Models : Headway
Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where
More informationLECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1.
LECTURE 5 ] DESCRIPTION OF PARTICLE MOTION IN SPACE -The displcemen, veloci nd cceleion in -D moion evel hei veco nue (diecion) houh he cuion h one mus p o hei sin. Thei full veco menin ppes when he picle
More informationModeling and Control of an Autothermal Reforming (ATR) Reactor for Fuel Cell Applications
Modelin and Conol of an Auohemal Refomin AR Reaco fo Fuel Cell Applicaion Donald J. Chmieleki and Yonyou u Depamen of Chemical & Bioloical Enineein Illinoi Iniue of echnoloy, Chicao, IL Denni Papadia Chemical
More informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More informationEvaluating the Economic Impacts of a Disaster: A CGE Application to the Tokai Region of Japan
Evaluaing he Economic Impacs of a Disase: A CGE Applicaion o he Tokai Region of Japan Hioyuki SHIBUSAWA * Absac Naual disases have a negaive effec on people and he egional economy. The cenal and egional
More information