Simulation of wave-body interactions in viscous flow based on explicit wave models
|
|
- Laureen McKinney
- 5 years ago
- Views:
Transcription
1 Smlao of wave-body eracos vscos flow based o eplc wave models Roma Lqe, Berrad Alessadr, Perre Ferra, Loel Geaz Ecole Cerale de Naes LMF/EHGO, UMR 6598 d CNRS,, re de la Noë, F-443 Naes Cede 3, Frace rodco Today wave-body eraco problems ca be solved mercally by sg sofwares based o Reyolds Averaged Naver-Sokes Eqaos (RANSE). So s possble o ake o acco vorcy ad vscosy effecs wc ca flece ydrodyamc loads ad srcre of e flows. However mercal smlaos der vscos flow eory sll lead geerally o large CPU mes becase of grd reqremes o esre a good propagao of cde waves e mesed par of e fld doma. Moreover sccessve wave reflecos o e body ad e oer bodares ca affec e comg wave ra ad redce e seable drao of e mercal smlao. To overcome ese dffcles a orgal meod cosss solvg e dffraced flow oly (Ferra e al., 3). Ts RANS Eqaos are modfed by splg all kows of e problem a sm of a cde erm ad a dffraced erm. Te cde erms are eplcly descrbed by flly o-lear wave models based o poeal flow eory : reglar waves are obaed by a algorm based o e sream fco eory of Reecker & Feo (98) ad rreglar wave ras by a specral formlao (Ferra e al, 3b). Ts oly e par of e grd e vcy of e srcre eeds o be refed ad a sreced grd allows a effce dampg of e dffraced flow far from e body. Here e splg of kows defed prevosly s appled o a vscos flow solver (Alessadr & elommea, 995). Modfed RANS Eqaos verfed by e dffraced flow are amed SWENS (Specral Wave Eplc Naver- Sokes) Eqaos ad ave bee developed prevosly (Ferra e al., 3a). e followg ad 3 resls are preseed order o sow ables of e prese meod. Te flow of a reglar wave ra o a mmersed crclar cylder s frs sded see Ferra e al. (3a) or Lqe e al. (3) Te a 3 case of a vercal cylder waves s sow. bo cases prese resls are compared w mercal ad epermeal daa. efo of SWENS Eqaos for e dffraced problem To cosder e sgle dffraced problem, prmve kows (Caresa compoes of velocy ( ) pressre p ad free-srface elevao ) are decomposed as follows : w {,,3}, = p = p p = {,,3 } Varables w e sbscrps ad represe cde ad dffraced varables respecvely. Ts decomposo s e rodced e se of al eqaos assmg a e cde wave flow flfls e Eler eqaos ad o-lear free srface bodary codos poeal flow eory : - Traspor eqaos : ν ( ) p ( ) ν ν ν ν = ν ν ( ) ρ - Mass coservao : =
2 - Free-srface bodary codos : () kemac codo 3 3 = ()ormal dyamc codo ( ) ( ) g p g p = ν ρ ν ρ ν ρ ν ρ () ageal dyamc codo ( ) = prevos eqaos e erms defed by cde varables (veloces, velocy grades, free-srface elevaos ad free-srface elevao grades ) are eplcly comped kowg kemacs ad erface poso of e cde flow. Ts se of eqaos wll be amed e followg SWENS (Specral Wave Eplc Naver-Sokes) Eqaos ad s solved by a flly-copled vscos fld solver developed by Alessadr & elommea (995). resls A o-lear reglar wave ra propagag above a mmersed orzoal crclar cylder deep waer s smlaed ere followg e mercal sdy of Scøberg & Capl () ad measremes by Capl (). Parameers of compao are ormalsed by akg e cylder rads c ad (c/g) / as leg ad me scales respecvely. Ts e cylder sbmergece s d/c=.5, e aglar freqecy kc=.56 ad e amplde of e fdameal freqecy compoe a/c s.7. W ese parameers, e Kelega-Carpeer mber s KC=.5. Fgre : deals of e grd Fgre : Lef : Free-srface profle beea e cylder (ceered a =). Rg : Forer compoes of e free srface elevao. Symbols : measremes from Capl (); dased le : compao from Scøberg & Capl (); sold le : prese compao.
3 A very refed grd abo 6 pos per waveleg for e rd armoc (fgre ) as bee sed o compe e ger order armoc compoes of e free srface properly. Sc a compao w a 5 odes srcred mooblock grd akes oe week a PC w a processor of.5 GHz. fgre o e lef saaeos free-srface profles obaed by prese compaos are compared w poeal flow compaos made by Scøberg & Capl (). Tese profles are ploed a e sa a wc e dsrbed wave feld wold ave a zero p-crossg a =. Te agreeme s qe good b ere are oceable dffereces : e vscos wave profle as a small pase lag ad s local mama are smaller. Capl () cocldes a vscos effecs wold mpose a ressace o e fld moo wc s lkely o delay e rasmsso of e wave over e cylder, eplag e small pase lag. Fgre o e rg sows e spaal varaos of e frs ree armoc compoes of e free srface elevao. For several locaos e mercal wave ak ese compoes ave bee comped sg a Forer decomposo of e me sory of e free-srface elevao sgal a movg wdow of oe wave perod log. Prese compaos are good agreeme w Capl's epermes especally for e frs armoc compoe (e mos fleced by vscosy effecs). 3 resls Z Z Y X Y X free srface cylder cde wave ra Fgre 3 : Vews of e mes arod e rcaed cylder 3 compaos ave bee r for a rcaed vercal crclar cylder o-lear reglar waves (see e grd o fgre 3). Te perod s.8 s, wave eg.37 m ad wave seepess abo 4.6 %. Te grd as 5 odes ad e reqred CPU me s abo 9 mes CPU per wave perod o a PC w oe processor of.5 GHz. Wave rps (fgre 4) ad armocs of orzoal forces ave bee compared w o-lear poeal flow resls from XWAVE code (Ferra, 998) ad/or epermeal daa from Kroksad & Saberg (995) w a very sasfyg agreeme. Force compoes (N) F (N) F (N) F3 (N) No-lear poeal eory Epermes SWENSE compaos
4 . Wave rp, T=.8 s, H=a=.37 m, β=.5 wave elevao (m) me (s). Wave rp, T=.8 s, H=a=.37 m, β=π/.5 wave elevao (m) me (s). Wave rp, T=.8 s, H=a=.37 m, β=π.5 wave elevao (m) me (s) Fgre 4 : Wave Rps (β= : p wave, β=π/ : sde, β=π : dowwave po of e cylder waerle) dased le : prese meod, sold le : No-lear poeal flow resls Coclso Te dffraco of o-lear reglar wave ras or 3 cases as bee sded w a orgal approac combg a vscos flow solver ad a eplc descrpo of e cde waves. sead of compg e wole velocy, pressre ad free srface felds, e dffraced flow oly s comped solvg SWENS Eqaos (RANS Eqaos were varables ave bee decomposed cde ad dffraced varables). Frs resls are ecoragg ad sow capably of e meod o well smlae wave-body eracos by sppressg sal mercal problems of wave geerao vscos flow solvers. Refereces Alessadr, B., elommea, G. (995), A mlgrd velocy-pressre-free srface elevao flly copled solver for calclao of rble compressble flow arod a ll, 9. Cof. Nm. Me. Lamar ad Trble Flows, Alaa, pp Capl, J. R. (), No-lear Wave eracos w a Sbmerged Horzoal Cylder,. Offsore ad Polar Eg. Cof., Savager, Vol. 3, pp Ferra, P. (998), Flly olear eracos of log-cresed wave packes w a ree dmesoal body, d ONR Symposm o Naval Hydrodyamcs, Wasgo. Ferra, P., Geaz, L., Alessadr, B., Le Tozé,. (3a), A Poeal/RANSE Approac for Reglar Waer Wave ffraco abo Srcres, Sp Tecology Researc, vol. 5, o. 4, pp Ferra, P., Le Tozé,., Pelleer K. (3b), No-lear me doma models for rreglar wave dffraco abo offsore, eraoal Joral for Nmercal Meods Flds, press. Kroksad, J.R.; Sasberg, C.T. (995), Rgg loads model verfed agas epermes, OMAE'95 Coferece, Copeage. Reecker, M.M.; Feo, J.. (98), A Forer appromao meod for seady waer waves, J. Fld Mec. 4, pp Lqe, R., Alessadr, B., Ferra, P., Geaz, L. (3), RANSE Aalyss of flow abo a sbmerged body sg eplc cde wave models, 6 Nmercal Towg Tak Symposm, Rome. Reecker, M.M.; Feo, J.. (98), A Forer appromao meod for seady waer waves, J. Fld Mec. 4, pp Scøberg, T.; Capl, J.R. (), Compao of No-Lear Wave Reflecos ad Trasmssos from a Sbmerged Horzoal Cylder,. Offsore ad Polar Eg. Cof., Savager, vol., pp.8-87.
5
NUMERICAL SOLUTIONS TO ORDINARY DIFFERENTIAL EQUATIONS
NUMERICAL SOLUTIONS TO ORDINARY DIFFERENTIAL EQUATIONS If e eqao coas dervaves of a - order s sad o be a - order dffereal eqao. For eample a secod-order eqao descrbg e oscllao of a weg aced po b a sprg
More informationTheory and application of the generalized integral representation method (GIRM) in advection diffusion problem
Appled ad ompaoal Mahemacs 4; 4: 7-49 blshed ole Ags 4 hp://www.scecepblshggrop.com//acm do:.648/.acm.44.5 IN: 8-565 r; IN: 8-56 Ole Theory ad applcao of he geeralzed egral represeao mehod IRM adveco dffso
More informationComputational Fluid Dynamics CFD. Solving system of equations, Grid generation
Compaoal ld Dyamcs CD Solvg sysem of eqaos, Grd geerao Basc seps of CD Problem Dscrezao Resl Gov. Eq. BC I. Cod. Solo OK??,,... Solvg sysem of eqaos he ype of eqaos decdes solo sraegy Marchg problems Eqlbrm
More informationAnalytical modelling of extruded plates
paper ID: 56 /p. Aalcal modellg of erded plaes C. Pézera, J.-L. Gader Laboraore Vbraos Acosqe, INSA de Lo,5 bs a.j. Cappelle 696 VILLEURBANNE Cede Erded plaes are ofe sed o bld lgh srcres h hgh sffess.
More informationCyclone. Anti-cyclone
Adveco Cycloe A-cycloe Lorez (963) Low dmesoal aracors. Uclear f hey are a good aalogy o he rue clmae sysem, bu hey have some appealg characerscs. Dscusso Is he al codo balaced? Is here a al adjusme
More informationArtificial Neural Networks Approach for Solving Stokes Problem
Appled Mahemacs, 00,, 88-9 do:0436/am004037 Pblshed Ole Ocober 00 (hp://wwwscrporg/joral/am) Arfcal Neral Neworks Approach for Solvg Sokes Problem Absrac Modjaba Bama, Asghar Keraecha, Sohrab Effa Deparme
More informationIntroduction to Mathematical Modeling and Computation
Ole Lecre Noe Irodco o Mahemacal Modelg ad Compao Verso.0 Aprl 08 Saor Yamamoo Professor Dr. Eg. Laboraory of Mahemacal Modelg ad Compao Dep. of Comper ad Mahemacal Sceces oho Uversy Seda 980-8579 Japa
More informationCIVL 7/8111 Time-Dependent Problems - 1-D Diffusion Equation 1/21
CIV 7/8 me-depede Problems - -D Dffso Eqao / e prevos ree capers deal eclsvely w seadysae problems, a s, problems were me dd o eer eplcly o e formlao or solo of e problem. e ypes of problems cosdered Capers
More information3D Hydrodynamic Model Development and Verification
Porlad Sae Uers PDXScolar Cl ad Eromeal Eeer Maser's Proec Repors Cl ad Eromeal Eeer 06 3D drodamc Model Deelopme ad Verfcao sse A. M. Al-Zbad Porlad Sae Uers albad0@mal.com Le s o o access o s docme beefs
More informationFORCED VIBRATION of MDOF SYSTEMS
FORCED VIBRAION of DOF SSES he respose of a N DOF sysem s govered by he marx equao of moo: ] u C] u K] u 1 h al codos u u0 ad u u 0. hs marx equao of moo represes a sysem of N smulaeous equaos u ad s me
More information1D Lagrangian Gas Dynamics. g t
Te KT Dfferece Sceme for Te KT Dfferece Sceme for D Laraa Gas Damcs t 0 t 0 0 0 t 0 Dfferece Sceme for D Dfferece Sceme for D Laraa Gas Damcs 0 t m 0 / / F F t t 0 / / F F t 0 / F F t Dfferece Sceme for
More informationTime-Domain Finite Element Method in Electromagnetics A Brief Review
Tme-Doma Fe leme ehod lecromagecs A ref Revew y D. Xe Ph.D. Tme doma compao of awell eqaos s reqred elecromagec radao scaerg ad propagao problems. I addo s ofe more ecoomcal o ge freqecy doma resls va
More informationA New Modified Approach for solving sevenorder Sawada-Kotara equations
Shraz Uversy of Techology From he SelecedWors of Habbolla Lafzadeh A New Modfed Approach for solvg seveorder Sawada-Koara eqaos Habbolla Lafzadeh, Shraz Uversy of Techology Avalable a: hps://wors.bepress.com/habb_lafzadeh//
More informationNUMERICAL EVALUATION of DYNAMIC RESPONSE
NUMERICAL EVALUATION of YNAMIC RESPONSE Aalycal solo of he eqao of oo for a sgle degree of freedo syse s sally o ossble f he excao aled force or grod accelerao ü g -vares arbrarly h e or f he syse s olear.
More informationNumerical Simulations of Unsteady Navier-Stokes Equations for Incompressible Newtonian Fluids using FreeFem++ based on Finite Element Method
Aals of Pre ad Aled Maemacs Vol. 6 o. 4 7-84 ISS: 79-87X P 79-888ole Pblsed o 7 Ma 4 www.researcmasc.org Aals of mercal Smlaos of Usead aver-soes Eqaos for Icomressble ewoa Flds sg FreeFem based o Fe Eleme
More informationFALL HOMEWORK NO. 6 - SOLUTION Problem 1.: Use the Storage-Indication Method to route the Input hydrograph tabulated below.
Jorge A. Ramírez HOMEWORK NO. 6 - SOLUTION Problem 1.: Use he Sorage-Idcao Mehod o roue he Ipu hydrograph abulaed below. Tme (h) Ipu Hydrograph (m 3 /s) Tme (h) Ipu Hydrograph (m 3 /s) 0 0 90 450 6 50
More informationPattern Formation in Chemical Reactions
Paer Formao Cemcal Reacos See Backreedy BSc Compg Sesso 003/004 Te caddae cofrms a e work sbmed s er ow ad e approprae cred as bee ge were referece ad bee made o e work of oers. I dersad a falre o arbe
More informationGAS DISTRIBUTION CONTROL SYSTEM USING MAGNETIC FLUID SENSORS
Romaa Repors Physcs, Vol. 58, No., P. 7 49, 6 GAS DSTRBUTON CONTROL SYSTE USNG AGNETC FLUD SENSORS N.C. POPA, J.J. ROUSSEAU, A. SBLN, J.P. CHATELON, D. JAON, F. ROYER, S. ROBERT, F. CHOUEKAN Romaa Academy
More informationFor the plane motion of a rigid body, an additional equation is needed to specify the state of rotation of the body.
The kecs of rgd bodes reas he relaoshps bewee he exeral forces acg o a body ad he correspodg raslaoal ad roaoal moos of he body. he kecs of he parcle, we foud ha wo force equaos of moo were requred o defe
More informationPartial Molar Properties of solutions
Paral Molar Properes of soluos A soluo s a homogeeous mxure; ha s, a soluo s a oephase sysem wh more ha oe compoe. A homogeeous mxures of wo or more compoes he gas, lqud or sold phase The properes of a
More informationHydraulic Model of Dam Break Using Navier Stokes Equation with Arbitrary Lagrangian-Eulerian Approach
IACIT Ieraoal Joral of Egeerg ad Tecolog ol. 8 No. 4 Ags 6 dralc odel of Dam Break Usg Naer okes Eqao Arbrar Lagraga-Elera Aroac Alreza Lorasb oarram Dolasa Prooz ad Alreza Laae Absrac Te lqd flo ad e
More informationThe ray paths and travel times for multiple layers can be computed using ray-tracing, as demonstrated in Lab 3.
C. Trael me cures for mulple reflecors The ray pahs ad rael mes for mulple layers ca be compued usg ray-racg, as demosraed Lab. MATLAB scrp reflec_layers_.m performs smple ray racg. (m) ref(ms) ref(ms)
More informationDetermination of Antoine Equation Parameters. December 4, 2012 PreFEED Corporation Yoshio Kumagae. Introduction
refeed Soluos for R&D o Desg Deermao of oe Equao arameers Soluos for R&D o Desg December 4, 0 refeed orporao Yosho Kumagae refeed Iroduco hyscal propery daa s exremely mpora for performg process desg ad
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
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 informationSuppose we have observed values t 1, t 2, t n of a random variable T.
Sppose we have obseved vales, 2, of a adom vaable T. The dsbo of T s ow o belog o a cea ype (e.g., expoeal, omal, ec.) b he veco θ ( θ, θ2, θp ) of ow paamees assocaed wh s ow (whee p s he mbe of ow paamees).
More informationSecond-Order Asymptotic Expansion for the Ruin Probability of the Sparre Andersen Risk Process with Reinsurance and Stronger Semiexponential Claims
Ieraoal Joral of Sascs ad Acaral Scece 7; (: 4-45 p://www.scecepblsggrop.com/j/jsas do:.648/j.jsas.7. Secod-Order Asympoc Expaso for e R Probably of e Sparre Aderse Rs Process w Resrace ad Sroger Semexpoeal
More informationSolution of Impulsive Differential Equations with Boundary Conditions in Terms of Integral Equations
Joural of aheacs ad copuer Scece (4 39-38 Soluo of Ipulsve Dffereal Equaos wh Boudary Codos Ters of Iegral Equaos Arcle hsory: Receved Ocober 3 Acceped February 4 Avalable ole July 4 ohse Rabba Depare
More information4. Runge-Kutta Formula For Differential Equations. A. Euler Formula B. Runge-Kutta Formula C. An Example for Fourth-Order Runge-Kutta Formula
NCTU Deprme o Elecrcl d Compuer Egeerg Seor Course By Pro. Yo-Pg Ce. Ruge-Ku Formul For Derel Equos A. Euler Formul B. Ruge-Ku Formul C. A Emple or Four-Order Ruge-Ku Formul
More informationHYDROSTATIC HEAD CORRECTION
XVI IMKO World oress Measureme - Suppors Scece - Improves Tecoloy - Proecs vrome... ad Provdes mployme - Now ad e Fuure Vea, AUSTIA,, Sepember 5-8 YDOSTATI AD OTION W. Kolacza Seco for e, Area, Ale, Poomery,
More informationReal-Time Systems. Example: scheduling using EDF. Feasibility analysis for EDF. Example: scheduling using EDF
EDA/DIT6 Real-Tme Sysems, Chalmers/GU, 0/0 ecure # Updaed February, 0 Real-Tme Sysems Specfcao Problem: Assume a sysem wh asks accordg o he fgure below The mg properes of he asks are gve he able Ivesgae
More informationFinal Exam Applied Econometrics
Fal Eam Appled Ecoomercs. 0 Sppose we have he followg regresso resl: Depede Varable: SAT Sample: 437 Iclded observaos: 437 Whe heeroskedasc-cosse sadard errors & covarace Varable Coeffce Sd. Error -Sasc
More informationKey words: Fractional difference equation, oscillatory solutions,
OSCILLATION PROPERTIES OF SOLUTIONS OF FRACTIONAL DIFFERENCE EQUATIONS Musafa BAYRAM * ad Ayd SECER * Deparme of Compuer Egeerg, Isabul Gelsm Uversy Deparme of Mahemacal Egeerg, Yldz Techcal Uversy * Correspodg
More informationEffects of initial compression stress on wave propagation in carbon nanotubes
Effecs f al cmpress sress wave prpaga carb abes M. M. Selm * S. Abe ad K. Hargaya eparme f Maemacs A-Aflaj cmmy Cllege Kg Sad Uversy Al-Aflaj 7- Sad Araba Naeclgy esearc Ise AIST Tsba 5-5 Japa Absrac A
More informationPEGN 513 Reservoir Simulation I Fall 2009
Hmer #3 l The smples rm r aerld a lear cre ally saraed h l ad a resdal aer sara h gravy r capllary eecs s represeed by he -dmesal Bcley-Levere maeral balace eqa () Eplc sl Csderg he space dscreza sh Fgre
More information4. Runge-Kutta Formula For Differential Equations
NCTU Deprme o Elecrcl d Compuer Egeerg 5 Sprg Course by Pro. Yo-Pg Ce. Ruge-Ku Formul For Derel Equos To solve e derel equos umerclly e mos useul ormul s clled Ruge-Ku ormul
More informationOn an algorithm of the dynamic reconstruction of inputs in systems with time-delay
Ieraoal Joural of Advaces Appled Maemacs ad Mecacs Volume, Issue 2 : (23) pp. 53-64 Avalable ole a www.jaamm.com IJAAMM ISSN: 2347-2529 O a algorm of e dyamc recosruco of pus sysems w me-delay V. I. Maksmov
More informationThe textbook expresses the stock price as the present discounted value of the dividend paid and the price of the stock next period.
ublc Affars 974 Meze D. Ch Fall Socal Sceces 748 Uversy of Wscos-Madso Sock rces, News ad he Effce Markes Hypohess (rev d //) The rese Value Model Approach o Asse rcg The exbook expresses he sock prce
More informationFresnel Equations cont.
Lecure 12 Chaper 4 Fresel quaos co. Toal eral refleco ad evaesce waves Opcal properes of meals Laer: Famlar aspecs of he eraco of lgh ad maer Fresel quaos r 2 Usg Sell s law, we ca re-wre: r s s r a a
More informationSYRIAN SEISMIC CODE :
SYRIAN SEISMIC CODE 2004 : Two sac mehods have bee ssued Syra buldg code 2004 o calculae he laeral sesmc forces he buldg. The Frs Sac Mehod: I s he same mehod he prevous code (995) wh few modfcaos. I s
More informationMultiphase Flow Simulation Based on Unstructured Grid
200 Tuoral School o Flud Dyamcs: Topcs Turbulece Uversy of Marylad, May 24-28, 200 Oule Bacgroud Mulphase Flow Smulao Based o Usrucured Grd Bubble Pacg Mehod mehod Based o he Usrucured Grd Remar B CHEN,
More informationChapter 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 informationSolution to Some Open Problems on E-super Vertex Magic Total Labeling of Graphs
Aalable a hp://paed/aa Appl Appl Mah ISS: 9-9466 Vol 0 Isse (Deceber 0) pp 04- Applcaos ad Appled Maheacs: A Ieraoal Joral (AAM) Solo o Soe Ope Probles o E-sper Verex Magc Toal Labelg o Graphs G Marh MS
More information3/3/2014. CDS M Phil Econometrics. Heteroskedasticity is a problem where the error terms do not have a constant variance.
3/3/4 a Plla N OS Volao of Assmpos Assmpo of Sphercal Dsrbaces Var T T I Var O Cov, j, j,..., Therefore he reqreme for sphercal dsrbaces s ad j I O homoskedascy No aocorrelao Heeroskedascy: Defo Heeroscedascy
More informationHYPOTHESIS TESTING. four steps
Irodcio o Saisics i Psychology PSY 20 Professor Greg Fracis Lecre 24 Correlaios ad proporios Ca yo read my mid? Par II HYPOTHESIS TESTING for seps. Sae he hypohesis. 2. Se he crierio for rejecig H 0. 3.
More informationDensity estimation III.
Lecure 4 esy esmao III. Mlos Hauskrec mlos@cs..edu 539 Seo Square Oule Oule: esy esmao: Mamum lkelood ML Bayesa arameer esmaes MP Beroull dsrbuo. Bomal dsrbuo Mulomal dsrbuo Normal dsrbuo Eoeal famly Eoeal
More informationMultiple Choice Test. Chapter Adequacy of Models for Regression
Multple Choce Test Chapter 06.0 Adequac of Models for Regresso. For a lear regresso model to be cosdered adequate, the percetage of scaled resduals that eed to be the rage [-,] s greater tha or equal to
More informationAn Expansion of the Derivation of the Spline Smoothing Theory Alan Kaylor Cline
A Epaso of the Derato of the Sple Smoothg heory Ala Kaylor Cle he classc paper "Smoothg by Sple Fctos", Nmersche Mathematk 0, 77-83 967) by Chrsta Resch showed that atral cbc sples were the soltos to a
More informationNumerical Techniques for Conservation Laws with Source Terms
Nmercal Techqe or Coerao Law wh Sorce Term by J Hdo Projec Speror Dr. P.K. Sweby Pro. M.J. Bae Abrac h derao we wll dc he e derece mehod or appromag coerao law wh a orce erm pree whch codered o be a kow
More informationLeast Squares Fitting (LSQF) with a complicated function Theexampleswehavelookedatsofarhavebeenlinearintheparameters
Leas Squares Fg LSQF wh a complcaed fuco Theeampleswehavelookedasofarhavebeelearheparameers ha we have bee rg o deerme e.g. slope, ercep. For he case where he fuco s lear he parameers we ca fd a aalc soluo
More informationResearch Article Cubic B-spline for the Numerical Solution of Parabolic Integro-differential Equation with a Weakly Singular Kernel
Researc Jornal of Appled Scences, Engneerng and Tecnology 7(): 65-7, 4 DOI:.96/afs.7.5 ISS: 4-7459; e-iss: 4-7467 4 Mawell Scenfc Pblcaon Corp. Sbmed: Jne 8, Acceped: Jly 9, Pblsed: Marc 5, 4 Researc Arcle
More informationOptimal Eye Movement Strategies in Visual Search (Supplement)
Opmal Eye Moveme Sraeges Vsual Search (Suppleme) Jr Naemk ad Wlso S. Gesler Ceer for Percepual Sysems ad Deparme of Psychology, Uversy of exas a Aus, Aus X 787 Here we derve he deal searcher for he case
More informationThe textbook expresses the stock price as the present discounted value of the dividend paid and the price of the stock next period.
coomcs 435 Meze. Ch Fall 07 Socal Sceces 748 Uversy of Wscos-Madso Sock rces, News ad he ffce Markes Hypohess The rese Value Model Approach o Asse rcg The exbook expresses he sock prce as he prese dscoued
More information(1) Cov(, ) E[( E( ))( E( ))]
Impac of Auocorrelao o OLS Esmaes ECON 3033/Evas Cosder a smple bvarae me-seres model of he form: y 0 x The four key assumpos abou ε hs model are ) E(ε ) = E[ε x ]=0 ) Var(ε ) =Var(ε x ) = ) Cov(ε, ε )
More information4. THE DENSITY MATRIX
4. THE DENSTY MATRX The desy marx or desy operaor s a alerae represeao of he sae of a quaum sysem for whch we have prevously used he wavefuco. Alhough descrbg a quaum sysem wh he desy marx s equvale o
More informationMechanical Design Technology (Free-form Surface) April 28, /12
Mechacal Desg echolog Free-form Srface Prof. amos Mrakam Assgme #: Free-form Srface Geerao Make a program ha geeraes a bcbc eer srface from 4 4 defg polgo e pos ad dsplas he srface graphcall a a ha allos
More informationand regular solutions of a boundary value problem are established in a weighted Sobolev space.
Ieraoal Joral of heorecal ad Appled Mahemacs 5; (: -9 Pblshed ole Je 5 5 (hp://www.scecepblshggrop.com/j/jam do:.648/j.jam.5. he olvably of a New Bodary Vale Problem wh ervaves o he Bodary Codos for Forward-
More informationSOLUTION OF PARABOLA EQUATION BY USING REGULAR,BOUNDARY AND CORNER FUNCTIONS
SOLUTION OF PAABOLA EQUATION BY USING EGULA,BOUNDAY AND CONE FUNCTIONS Dr. Hayder Jabbar Abood, Dr. Ifchar Mdhar Talb Deparme of Mahemacs, College of Edcao, Babylo Uversy. Absrac:- we solve coverge seqece
More informationON TOTAL TIME ON TEST TRANSFORM ORDER ABSTRACT
V M Chacko E CONVE AND INCREASIN CONVE OAL IME ON ES RANSORM ORDER R&A # 4 9 Vol. Decembe ON OAL IME ON ES RANSORM ORDER V. M. Chacko Depame of Sascs S. homas Collee hss eala-68 Emal: chackovm@mal.com
More informationImplementation of a Slip Boundary Condition in a Finite Volume Code Aimed to Predict Fluid Flows
II Coerêca Nacoal de Méodos Nmércos em Mecâca de Fldos e Termodâmca Uversdade de Avero 8-9 de Mao de 008 Imlemeao o a Sl Bodary Codo a Fe Volme Code Amed o Predc Fld Flows Ferrás L.L. Nóbrega J.M. Pho
More informationB-spline curves. 1. Properties of the B-spline curve. control of the curve shape as opposed to global control by using a special set of blending
B-sple crve Copyrght@, YZU Optmal Desg Laboratory. All rghts reserved. Last pdated: Yeh-Lag Hs (--9). ote: Ths s the corse materal for ME Geometrc modelg ad compter graphcs, Ya Ze Uversty. art of ths materal
More informationDiscretization Methods in Fluid Dynamics
Corse : Fld Mechacs ad Eergy Coverso Dscretzato Methods Fld Dyamcs Mayak Behl B-tech. 3 rd Year Departmet of Chemcal Egeerg Ida Isttte of Techology Delh Spervsor: Dr. G.Bswas Ida Isttte of Techology Kapr
More informationLeast squares and motion. Nuno Vasconcelos ECE Department, UCSD
Leas squares ad moo uo Vascocelos ECE Deparme UCSD Pla for oda oda we wll dscuss moo esmao hs s eresg wo was moo s ver useful as a cue for recogo segmeao compresso ec. s a grea eample of leas squares problem
More informationFault Tolerant Computing. Fault Tolerant Computing CS 530 Probabilistic methods: overview
Probably 1/19/ CS 53 Probablsc mehods: overvew Yashwa K. Malaya Colorado Sae Uversy 1 Probablsc Mehods: Overvew Cocree umbers presece of uceray Probably Dsjo eves Sascal depedece Radom varables ad dsrbuos
More informationDifferential Equation of Eigenvalues for Sturm Liouville Boundary Value Problem with Neumann Boundary Conditions
Ierol Reserc Jorl o Aled d Bsc Sceces 3 Avlle ole www.rjs.co ISSN 5-838X / Vol 4 : 997-33 Scece Exlorer Plcos Derel Eqo o Eevles or Sr Lovlle Bodry Vle Prole w Ne Bodry Codos Al Kll Gold Dere o Mecs Azr
More informationDiscrete Adomian Decomposition Method for. Solving Burger s-huxley Equation
It. J. Cotemp. Math. Sceces, Vol. 8, 03, o. 3, 63-63 HIKARI Ltd, www.m-har.com http://dx.do.org/0.988/jcms.03.3570 Dscrete Adoma Decomposto Method for Solvg Brger s-hxley Eqato Abdlghafor M. Al-Rozbaya
More informationCompare and Evaluate Equations in Velocity-Depth Distribution of Open Channels
Crret World Evromet Vol. 0(Specal Isse ), 88-93 (05) Compare ad Evalate Eqatos Velocty-Depth Dstrbto of Ope Chaels Zad Sara ad Nemat Amr Reza Gradate stdet of Costrcto of Hydralc Strctres of North Tehra
More information828. Piecewise exact solution of nonlinear momentum conservation equation with unconditional stability for time increment
88. Pecewse exact solto of olear mometm coservato eqato wth codtoal stablty for tme cremet Chaghwa Jag, Hyoseob Km, Sokhwa Cho 3, Jho Km 4 Korea Itellectal Property Offce, Daejeo, Korea, 3 Kookm Uversty,
More informationThe Poisson Process Properties of the Poisson Process
Posso Processes Summary The Posso Process Properes of he Posso Process Ierarrval mes Memoryless propery ad he resdual lfeme paradox Superposo of Posso processes Radom seleco of Posso Pos Bulk Arrvals ad
More informationThe 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 informationNumerical Analysis Formulae Booklet
Numercal Aalyss Formulae Booklet. Iteratve Scemes for Systems of Lear Algebrac Equatos:.... Taylor Seres... 3. Fte Dfferece Approxmatos... 3 4. Egevalues ad Egevectors of Matrces.... 3 5. Vector ad Matrx
More informationFundamentals of Regression Analysis
Fdametals of Regresso Aalyss Regresso aalyss s cocered wth the stdy of the depedece of oe varable, the depedet varable, o oe or more other varables, the explaatory varables, wth a vew of estmatg ad/or
More informationSystematic Configuration Procedure of LMI-Based Linear Anti-windup Synthesis
Sysemac Cofgrao Procere of LMI-Base Lear A-p Syhess a a a Jgcheg Wag Absrac I hs paper, a ovel sysemac cofgrao procere choosg parameers s presee for he syhess of lear a-p scheme by revsg he orgal goal
More informationQR factorization. Let P 1, P 2, P n-1, be matrices such that Pn 1Pn 2... PPA
QR facorzao Ay x real marx ca be wre as AQR, where Q s orhogoal ad R s upper ragular. To oba Q ad R, we use he Householder rasformao as follows: Le P, P, P -, be marces such ha P P... PPA ( R s upper ragular.
More informationMathematical Formulation
Mahemacal Formulao The purpose of a fe fferece equao s o appromae he paral ffereal equao (PE) whle maag he physcal meag. Eample PE: p c k FEs are usually formulae by Taylor Seres Epaso abou a po a eglecg
More information2.160 System Identification, Estimation, and Learning Lecture Notes No. 17 April 24, 2006
.6 System Idetfcato, Estmato, ad Learg Lectre Notes No. 7 Aprl 4, 6. Iformatve Expermets. Persstece of Exctato Iformatve data sets are closely related to Persstece of Exctato, a mportat cocept sed adaptve
More informationConservative and Easily Implemented Finite Volume Semi-Lagrangian WENO Methods for 1D and 2D Hyperbolic Conservation Laws
Joural of Appled Mahemacs ad Physcs, 07, 5, 59-8 hp://www.scrp.org/oural/amp ISSN Ole: 37-4379 ISSN Pr: 37-435 Coservave ad Easly Implemeed Fe Volume Sem-Lagraga WENO Mehods for D ad D Hyperbolc Coservao
More informationLecture 3 Probability review (cont d)
STATS 00: Itroducto to Statstcal Iferece Autum 06 Lecture 3 Probablty revew (cot d) 3. Jot dstrbutos If radom varables X,..., X k are depedet, the ther dstrbuto may be specfed by specfyg the dvdual dstrbuto
More informationAML710 CAD LECTURE 12 CUBIC SPLINE CURVES. Cubic Splines Matrix formulation Normalised cubic splines Alternate end conditions Parabolic blending
CUIC SLINE CURVES Cubc Sples Marx formulao Normalsed cubc sples Alerae ed codos arabolc bledg AML7 CAD LECTURE CUIC SLINE The ame sple comes from he physcal srume sple drafsme use o produce curves A geeral
More informationFREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM
Joural of Appled Matematcs ad Computatoal Mecacs 04, 3(4), 7-34 FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM Ata Cekot, Stasław Kukla Isttute of Matematcs, Czestocowa Uversty of Tecology Częstocowa,
More informationProcessing of Information with Uncertain Boundaries Fuzzy Sets and Vague Sets
Processg of Iformato wth Ucerta odares Fzzy Sets ad Vage Sets JIUCHENG XU JUNYI SHEN School of Electroc ad Iformato Egeerg X'a Jaotog Uversty X'a 70049 PRCHIN bstract: - I the paper we aalyze the relatoshps
More informationCONSISTENT EARTHQUAKE ACCELERATION AND DISPLACEMENT RECORDS
APPENDX J CONSSTENT EARTHQUAKE ACCEERATON AND DSPACEMENT RECORDS Earhqake Acceleraons can be Measred. However, Srcres are Sbjeced o Earhqake Dsplacemens J. NTRODUCTON { XE "Acceleraon Records" }A he presen
More informationInternational Journal of Theoretical and Applied Mathematics
Ieraoal Joral of heorecal ad Appled Maheacs 5; (: - Pblshed ole Je 3 5 (hp://wwwscecepblshggropco/j/ja do: 648/jja5 he Solvably of a New Bodary Vale Proble wh ervaves o he Bodary Codos for Forward- Backward
More informationu(x, t) = u 0 (x ct). This Riemann invariant u is constant along characteristics λ with x = x 0 +ct (u(x, t) = u 0 (x 0 )):
x, t, h x The Frst-Order Wave Eqato The frst-order wave advecto eqato s c > 0 t + c x = 0, x, t = 0 = 0x. The solto propagates the tal data 0 to the rght wth speed c: x, t = 0 x ct. Ths Rema varat s costat
More informationIdeal multigrades with trigonometric coefficients
Ideal multgrades wth trgoometrc coeffcets Zarathustra Brady December 13, 010 1 The problem A (, k) multgrade s defed as a par of dstct sets of tegers such that (a 1,..., a ; b 1,..., b ) a j = =1 for all
More informationC-1: Aerodynamics of Airfoils 1 C-2: Aerodynamics of Airfoils 2 C-3: Panel Methods C-4: Thin Airfoil Theory
ROAD MAP... AE301 Aerodyamcs I UNIT C: 2-D Arfols C-1: Aerodyamcs of Arfols 1 C-2: Aerodyamcs of Arfols 2 C-3: Pael Methods C-4: Th Arfol Theory AE301 Aerodyamcs I Ut C-3: Lst of Subects Problem Solutos?
More informationP-Convexity Property in Musielak-Orlicz Function Space of Bohner Type
J N Sce & Mh Res Vol 3 No (7) -7 Alble ole h://orlwlsogocd/deh/sr P-Coey Proery Msel-Orlcz Fco Sce o Boher ye Yl Rodsr Mhecs Edco Deree Fcly o Ss d echology Uerss sl Neger Wlsogo Cerl Jdoes Absrcs Corresodg
More informationBeam Warming Second-Order Upwind Method
Beam Warmg Secod-Order Upwd Method Petr Valeta Jauary 6, 015 Ths documet s a part of the assessmet work for the subject 1DRP Dfferetal Equatos o Computer lectured o FNSPE CTU Prague. Abstract Ths documet
More informationSolution set Stat 471/Spring 06. Homework 2
oluo se a 47/prg 06 Homework a Whe he upper ragular elemes are suppressed due o smmer b Le Y Y Y Y A weep o he frs colum o oba: A ˆ b chagg he oao eg ad ec YY weep o he secod colum o oba: Aˆ YY weep o
More informationEfficient Estimators for Population Variance using Auxiliary Information
Global Joural of Mahemacal cece: Theor ad Praccal. IN 97-3 Volume 3, Number (), pp. 39-37 Ieraoal Reearch Publcao Houe hp://www.rphoue.com Effce Emaor for Populao Varace ug Aular Iformao ubhah Kumar Yadav
More informationSliding mode: Basic theory and new perspectives
Dep o Elecrcal ad Elecroc Eg. Uversy o Caglar 5 h Worshop o Srcral Dyamcal Sysems: Compaoal Aspecs Capolo (BA) Ialy Sldg mode: Basc heory ad ew perspecves Elo USAI esa@dee.ca. SDS 8 - Capolo (BA) Je 8
More informationOn the Formulation of a Hybrid Discontinuous Galerkin Finite Element. Method (DG-FEM) for Multi-layered Shell Structures.
O he Formlao of a Hybr Dcoo Galer Fe Eleme Meho DG-FEM for Ml-layere Shell Srcre Tay L The bme o he facly of he Vrga Polyechc Ie a Sae Uvery paral flfllme of he reqreme for he egree of Maer of Scece I
More informationRECURSIVE IDENTIFICATION BASED ON NONLINEAR STATE SPACE MODELS APPLIED TO DRUM-BOILER DYNAMICS WITH NONLINEAR OUTPUT EQUATIONS
005 Amerca Corol Coferece Je 8-0, 005 Porlad, OR, UA FrC54 RECURVE DENFCAON BAED ON NONLNEAR AE PACE MODEL APPLED O DRUM-BOLER DYNAMC WH NONLNEAR OUPU EQUAON orbjör Wgre, eor Member, EEE Abrac he paper
More informationAn Alternative Strategy for the Solution of Heat and Incompressible Fluid Flow Problems via Finite Volume Method
A Alteratve Strategy for the Solto of Heat ad Icompressble Fld Flow Problems va Fte Volme Method Masod Nckaee a, Al Ashrafzadeh b, Stefa Trek a a Isttte of Appled Mathematcs, Dortmd Uversty of Techology,
More informationPrediction of Wing Downwash Using CFD
Predcon of Wng Downwash Usng CFD Mohammed MAHDI* *Correspondng ahor Aeronacal Research Cener-Sdan P.O. Bo 334 momahad7@homal.com DOI:.3/66-8.5.7.. 3 rd Inernaonal Worshop on Nmercal Modellng n Aerospace
More information8. Queueing systems lect08.ppt S Introduction to Teletraffic Theory - Fall
8. Queueg sysems lec8. S-38.45 - Iroduco o Teleraffc Theory - Fall 8. Queueg sysems Coes Refresher: Smle eleraffc model M/M/ server wag laces M/M/ servers wag laces 8. Queueg sysems Smle eleraffc model
More informationNumericalSimulationofWaveEquation
Global Joral of Scece Froter Research: A Physcs ad Space Scece Volme 4 Isse 7 Verso. Year 4 Type : Doble Bld Peer Revewed Iteratoal Research Joral Pblsher: Global Jorals Ic. (USA Ole ISSN: 49-466 & Prt
More informationDISTURBANCE TERMS. is a scalar and x i
DISTURBANCE TERMS I a feld of research desg, we ofte have the qesto abot whether there s a relatoshp betwee a observed varable (sa, ) ad the other observed varables (sa, x ). To aswer the qesto, we ma
More informationd dt d d dt dt Also recall that by Taylor series, / 2 (enables use of sin instead of cos-see p.27 of A&F) dsin
Learzato of the Swg Equato We wll cover sectos.5.-.6 ad begg of Secto 3.3 these otes. 1. Sgle mache-fte bus case Cosder a sgle mache coected to a fte bus, as show Fg. 1 below. E y1 V=1./_ Fg. 1 The admttace
More informationImprovement of Two-Equation Turbulence Model with Anisotropic Eddy-Viscosity for Hybrid Rocket Research
evenh Inernaonal onference on ompaonal Fld Dynamcs (IFD7), Bg Island, awa, Jly 9-, IFD7-9 Improvemen of Two-Eqaon Trblence Model wh Ansoropc Eddy-Vscosy for ybrd oce esearch M. Mro * and T. hmada ** orrespondng
More informationCS 1675 Introduction to Machine Learning Lecture 12 Support vector machines
CS 675 Itroducto to Mache Learg Lecture Support vector maches Mlos Hauskrecht mlos@cs.ptt.edu 539 Seott Square Mdterm eam October 9, 7 I-class eam Closed book Stud materal: Lecture otes Correspodg chapters
More information