APPROXIMATE OPTIMAL CONTROL OF LINEAR TIME-DELAY SYSTEMS VIA HAAR WAVELETS
|
|
- Leona Waters
- 5 years ago
- Views:
Transcription
1 Journal o Engneerng Sene and ehnology Vol., No. (6) Shool o Engneerng, aylor s Unversty APPROIAE OPIAL CONROL OF LINEAR IE-DELAY SYSES VIA HAAR WAVELES AKBAR H. BORZABADI*, SOLAYAN ASADI Shool o athemats and Computer Sene, Damghan Unversty, Damghan, Iran *Correspondng Author: borzabad@du.a.r Abstrat In ths paper, Haar wavelet benets are appled to the optmal ontrol o lnear tme-delay systems. A dsretzed orm o optmal ontrol problem at olloaton ponts based on some useul propertes o Haar wavelets transorms orgnal problem nto a nonlnear programmng (NLP). he gven numeral examples show the auray o the presented sheme n omparson wth some other methods. Keywords: Haar wavelet, Optmal ontrol problem, Dsretzaton, Lnear tmedelay system, Nonlnear programmng.. Introduton Over the last ew years we have wtnessed an ever nreasng nterest n the study o ontrol proesses governed by derent systems. One o the most mportant o these systems are delay systems. me-delay oten appears n many ontrol systems (suh as arrat, hemal or proess ontrol systems) ether n the state, the ontrol nput, or the measurements. Due to presentng delay and ts mportant onsderaton, n many pratal systems [, ], ontrol o tme-delay systems has been nterested by many engneers and sentst. Sne the analytal methods, espeally n optmal ontrol o tme-delay systems, have less ablty to mplement, the derent numeral methods to overome the problems o exat methods have been devsed. Some o these tehnques nlude, teratve dynam programmng [3], steepest desent based algorthm [4], Chebyshev seres [5], Laguerre polynomals [6], Blo-pulse untons [7], Hybrd o blo-pulse and Legendre polynomals [8], Legendre multwavelets [9], Walsh untons []. Reently, Haar wavelets have been appled extensvely or sgnal proessng n ommunatons and physs researh, and have proved to be a wonderul 486
2 Approxmate Optmal Control o Lnear me-delay Systems va Haar Nomenlatures a Haar oeent H (t) Haar matrx P Operatonal ntegraton matrx D() Delay operatonal matrx (/) /) Null matrx o order ( / ) ( / ) Gree Symbols Integral square error (t) A group o square waves (t-) Delay unton o () t Abbrevatons NLP Nonlnear programmng mathematal tool. Haar wavelets have the smplest orthogonal seres wth ompat support. In haratersts maes Haar wavelets good anddate or applaton to optmal ontrol problems []. he olloaton methods developed to solve optmal ontrol problems generally all nto two ategores, loal olloaton [] and global orthogonal olloaton [3]. In loal olloaton methods, the tme nterval onsdered s dvded nto a seres o subntervals wthn whh the ntegraton rule must be satsed. In reent years, more attenton has been oused on global orthogonal olloaton methods suh as Chebyshev, Legendre and some other. By expandng the state and ontrol varables nto peewse-ontnuous ombnaton o these nterpolatng polynomals and dervatves, then, the obetve unton and system onstrants are all onverted nto algebra equatons wth unnown oeents. In ths paper, we ntrodue an alternatve method to solve the lnear optmal ontrol wth delay systems. We ntrodue the Haar wavelets theory and propertes nludng the Haar wavelets bass and ts ntegral operatonal matrx []. he delay and produt are gven. hen we wll assume that the ontrol varables and dervatve o the state varables n the optmal ontrol problems may be expressed n the orm o Haar wavelets and unnown oeents. By usng the Haar operatonal ntegraton matrx we nd (t). he delay vetor ( t ) and U ( t ) an be alulated by usng the delay operatonal matrx and Haar operatonal ntegraton matrx. hereore, all varables n the tme-delay system are expressed as seres o the Haar amly and operatonal matrx and delay operatonal matrx. Fnally, the tas o ndng the unnown parameters that optmze the desgnate perormane whle satsyng all onstrants s perormed by a nonlnear programmng solver. In ths paper, rst Haar wavelets and ts propertes s ntrodued. hen the approxmaton o a unton by Haar wavelets s dsussed. By ntrodung operatonal ntegraton matrx and delay operatonal matrx, Haar dsretzaton method s establshed. Ater, desrbng the ormulaton o the optmal ontrol problem wth delays, the proposed method s used n the analyss o lnear tmedelay systems. Fnally, by some numeral examples the proeny o the gven approah s examned and ts results ompared wth other methods. Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
3 488 A. H. Borzabad and S. Asad. Haar Wavelets and Its Propertes he orthogonal set o Haar wavelets (t) s a group o square waves wth magntude + or - n some ntervals and zeros elsewhere. ( t) =, <, () t t <, ( t) = t <, () t <, (t) = ( t ) = t <, otherwse. (3) or =, =,,, =,,, nteger m =,( =,,, J ), ndates the level o the wavelet and =,,, s the translaton parameter. axmal level o resoluton s J. he maxmal value o s =. A smple alulaton shows that = l =, ( ) ( ) = t l t l. (4) Consequently, the untons (t) are orthogonal. hs allows us to transorm any unton square ntegrable on the nterval tme [,] nto Haar wavelets seres. 3. Funton Approxmaton by Haar Wavelets We ust ponted out that a square ntegrable unton an be expressed n terms o Haar orthogonal bass on nterval [,]. However, beore the proesson to ths transer, t s neessary to uny the tme nterval. By usng a lnear transormaton, the atual tme t an be expressed as a unton o va t = [( t t ) t ] where t s the ntal tme and t s the nal tme n a square ntegrable unton (t). Any unton () t whh s square ntegrable n the nterval [,] an be expanded n a Haar seres wth an nnte number o terms. ( t ) = a ( t ), =,, <, t [,), (5) = where the Haar oeents a = ( t ) ( ), t dt (6) are determned n suh a way that the ntegral square error Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
4 Approxmate Optmal Control o Lnear me-delay Systems va Haar = ( ( t ) a ( )), t dt = (7) s mnmum. Here s vanshed when tends to nnty. Usually, the seres expanson o (5) ontans an nnte number o terms or smooth () t. I () t s a pee wse onstant or may be approxmated as a peewse onstant, then the summaton (5) wll be termnated ater terms, that s, F ( t ) a ( t ) = A ( t ), (8) = where the oeent vetor A = [ a, a,..., a ] and ( ) = [,,..., ] t. Let us dene the olloaton ponts ts = ( s.5) /, ( s =,... ). Wth these hosen olloaton ponts, the unton s dsretzed nto a seres o nodes wth equvalent dstanes. Let the Haar matrx H be the ombnaton o () t at all the olloaton ponts. hus, H t) = [ h,..., h ] ( ( t ) ( t) ( t ) ( ) ( ) ( ) t t t = [ ( ),..., ( )] = t t. (9) ( t ) ( t) ( t ) For example, H = ( t ) ( t) =. hereore, the unton (t) may be approxmated as ( ts ) = H. () 4. Integraton o Haar Wavelets In the wavelet analyss or a dynam system, all untons need to be transormed nto Haar seres. Sne the derentaton o Haar wavelets always results n mpulse untons whh should be avoded, the ntegraton o Haar wavelets s preerred, whh should be expandable nto Haar seres wth Haar oeent matrx P ' ' t ( t ) dt = P( t ), () where P s the operatonal ntegraton matrx whh satses the ollowng reursve ormula, P / H / P =, P = [ ], () H / whh s gven n [4] and ( /) ( /) s a null matrx o order ( / ) ( / ). 5. Delay Operatonal atrx o Haar Wavelets Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
5 49 A. H. Borzabad and S. Asad he delay unton ( t ) s the sht o () t dened n (3) along the tme axs by. he delay operatonal matrx D () s gven by ( t ) D( ) ( t ), t >, t <, (3) [,] s the delay parameter. Frst, we nd the matrx D( ) = [ d ] or. he our bass untons are gven by,,, 3. By (8) and (3) we have ( t ) ( t) ( t ) ( t) = [ d ( )],, =,,3,4, 3( t ) 3( t) ( t ) ( t) 4 4 where ( t ) =, t <, and t <, ( t ) = t <, t <, 4 ( t ) = t <, 4 and 3 t <, 4 3( t ) = 3 t <. 4 o nd the entres d (),, =,,3,4, we use the nner produt. For example =., we have d =< ( t ), ( t ) >= ( t ) ( t ) dt =.9, d3 =< 3( t ), ( t ) >= 3( t ) ( t ) dt =. I we alulate all d () as d and d 3 the 4 4 operatonal matrx D () s obtaned. In partular, we have D4 4(.) = n In a smlar manner, we use the vetor unton () t wth dmenson, n n then delay matrx D () wth n an be obtaned as ollows, = ( ) ( ) = = l =, d l t l t dt l. Note that or any dmenson = then matrx s dagonal. 6. Problem Statement Consder a lnear system wth delays n both the state and ontrol desrbed by Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
6 Approxmate Optmal Control o Lnear me-delay Systems va Haar ( t ) = A( t ) ( t ) B ( t ) ( t ) E ( t ) U ( t ) S ( t ) U ( t ), (4) wth ntal data () =, (5) ( t ) = ( t ), t [,], (6) U ( t ) = ( t ), t [,], (7) where s an m -vetor o state; U s an q -vetor o nput; At (), Bt (), Et () and St () are ontnuous matrx untons o the tme o approprate dmensons, s a onstant speed vetor. and are delays n state and ontrol, respetvely, and the ntal unton () t and () t are ontnuous n ther respetve ntervals. he problem s to mnmze t J = H ( t, ) L( t,, U ) dt, (8) where H s a salar unton o the nal tme t and nal state varables and L( t,, U ) s a salar unton o the tme, state and ontrol U. 7. Haar Dsretzaton and me-delay Systems Analyss We dsretze the untons () t by dvdng the nterval [,], to parts o equal length t =/ and ntrodue the olloaton ponts = (.5) /, =,...,, where s the number o nodes used n the dsretzaton and also s the maxmum wavelet ndex number. We approxmate state varables x () and ontrol varables u () by Haar wavelets wth olloaton ponts,.e., x( ) x ( ), (9) u( ) u ( ), () where = [,..., ] and = [,..., ]. Usng the operatonal ntegraton x x x matrx P dened n () u u u ' ' ' ' x x () x ( ) = x ( ) d x = ( ) d x = P ( ) x. As stated n (), the expanson o the matrx () at the olloaton ponts wll the yeld the Haar matrx H = [ h,..., h ] t ellows that x ( ) = h, u( ) = h, x ( ) = C ph x, =,...,. () x u x Now we ous on the analyss o tme-delay systems. Frst hoose N as ollowng manner, N =.5, (3) =, and let N N. Let ( ) = [ x ( ), x ( ),..., x m ( )], (4) U ( ) = [ u( ), u( ),..., u q ( )], (5) ˆ ( ) = I m ( ), (6) ( ) = I q ( ), (7) Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
7 49 A. H. Borzabad and S. Asad where I m and I q dmensonal dentty matres and denotes roneer produt [5]. By (9)-() eah o x ( t ), =,,..., m and u ( t ), =,,..., q an be wrtten as x ( ) = P ( ) x (), (8) x u ( ) = ( ), (9) u where = [,,..., ] and = [,,..., ]. Usng (3)-(9) x x x x u u u u ˆ ( ) = C ( ), ( ) = ˆ ˆ C P ( ) (), (3) and also U( ) = C U ( ), (3) where C = [,,..., ], C = [,,..., ] x and Pˆ = I m P dsusson n Se.3 and a smlar notaton we an wrte ( ) = ˆ ( ), (3) C ( ) = C ( ). (33) Usng (3), (3) and (3), t an be onluded that ( ) <, ( ) = (34) C ˆ ˆ ( ˆ PD ) ( ) () < t, ( ) <, U ( ) = (35) C U D ( ) ( ) < t, where Dˆ = I m D and D = I q D. Smlarly eah entres o At (), Bt (), Et () and St () may be expanded by (8) and thus A( t ) = A ˆ ( t ), (36) B ( t ) = B ˆ ( t ), (37) E ( t ) = E ( t ), (38) S ( t ) = S ( t ), (39) where a a a b b b m m a a a m b b b m A =, B = a n a n a nm b n b n b nm nm e e e s s s q q e e e q s s s q E =, S =. e n e n e nq s n s n s nq nq nq When the Haar olloaton method s appled n the optmal ontrol problem wth tme-delay system, the varables an be set as the unnown oeents vetor o nm Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
8 Approxmate Optmal Control o Lnear me-delay Systems va Haar the dervatve o the state varables and ontrol varables together wth ntal and nal tmes, that s [ C, C,..., C, C,..., C, t, t ]. U U Consder the ost untonal (8) by = (, ( )) ( ) (, ˆˆ J H t t t L C P ( ), C ( )) dt. U Sne the Haar wavelets are expeted to be onstant steps at eah tme nterval, the above equaton an be smpled as ˆˆ U = J = H ( t, ( )) ( t t ) L(, C P ( ), C ( )), By substtutng, U, and n (4) and usng (3)-(39), or =,..., N, we have ˆ ˆ C ( ) = ( ˆ ˆ t t )(( A ( ))( C P( ) ( )) ()) ˆ ( ) ( ) ( ( ))( B ( )) ( ) ( )), E CU S and also or = N,..., N, ˆ ˆ C ( ) = ( ˆ ˆ t t )(( A ( ))( C P( ) ( )) ()) ˆ ˆ ˆ ˆ B ( )( C PD ( ) ( ) ()) ( E ( ))( CU ( )) S ( ) ( )). Also or = N,...,, ˆ ˆ C ( ) = ( ˆ ˆ t t )(( A ( ))( C P( ) ( )) ()) ˆ ( )( ˆ ˆ ( ) ˆ B C PD ( ) ()) ( E ( ))( C ( )) U S ( )( CU D( ) ( ))). Note that n (9) we ponted that or =,...,, ( ) = h. Sne the rst and last olloaton ponts are not set as the ntal and nal tme, the ntal and nal state varables are alulated aordng to = () /, = ( ) /. In ths way, the optmal ontrol o tme-delay systems transormed nto NLP or LP problem. 8. Numeral Results In ths seton, he results o applyng the method n three numeral examples are presented. Example 8. Consder the ollowng optmal ontrol problem o lnear tmedelay system x ( t ) = 4 tx ( t ) x ( t / ) u( t ), x ( t ) =, / t, wth assoated quadrat ost untonal to be mnmzed J = (4 ( ) 4 ( )). x t u t dt Usng the Haar wavelets olloaton method wth =6 olloaton pont and by (7) and (3)-(39) we have =, x x u h = 4 ( Ph x ()) h, =,,..., N, h = 4 ( Ph x ()) ( PD ( ) h x ()) h, = N,...,, x x x u Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
9 494 A. H. Borzabad and S. Asad J Ph x h = (4( x ()) 4( u ) ), = where x and u are the unnown varables o NLP and by (3) N =8. he obtaned mnmum value o the ost untonal s J = whh s muh better than J = 5.73, reported n [9]. Agan the results has been examned usng 3 olloaton ponts. In Fgs. and, one an observe the dagram o approxmate optmal ontrol and state untons, respetvely. Fg.. he approxmate optmal ontrol nput n Example 8.. Fg.. he approxmate optmal traetory n Example 8.. Example 8. Consder the problem o mnmzng J = () () ( u ( t )) dt, (4) subet to the system o the delayed derental equatons ( t) = ( ) ( ) ( ),, t t u t t (4) Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
10 Approxmate Optmal Control o Lnear me-delay Systems va Haar ( t) = x ( t) x( t), () =, ( t) =, t. (4) As prevous example, the mnmzaton o J subet to (4) and (4) has been obtaned usng the proposed method. Usng 6 olloaton ponts or Haar wavelets dsretzaton method, the optmal value s obtaned J =.6986, whh s better than J = and J = 3.399, reported n [9] and [6], respetvely. he ontrol varable ut () and the state varables x () t, x () t or two derent number o olloaton ponts, = 6 and = 3, depted n Fgs. 3 and 4, respetvely. Fg. 3. he approxmate optmal ontrol nput n Example 8.. Fg. 4. he approxmate optmal traetory n Example 8.. Example 8.3 In ths example, the delay s onsdered n ontrol and state varables. he problem s mnmzaton o the untonal Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
11 496 A. H. Borzabad and S. Asad J = ( ( ) ( )), x t u t dt subet to delayed derental equaton x ( t ) = x ( t ) x ( t ) u( t ) u ( t ), 3 3 x ( t ) =, t [,], 3 u ( t ) =, t [,]. 3 Usng 6 olloaton ponts n Haar wavelets dsretzaton method the optmal value s obtaned J =.4. hs value ompares well wth those gven n []. he near optmal ontrol and state varables whh are obtaned by the Haar wavelet dsretzaton method are shown n Fgs. 5 and 6 or =6 and = 3, respetvely. Fg. 5. he approxmate optmal ontrol nput n Example 8.3. Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
12 Approxmate Optmal Control o Lnear me-delay Systems va Haar Fg. 6. he approxmate optmal traetory n Example Conlusons In ths paper usng the propertes o Haar wavelets, a olloaton based method s presented or the resoluton o optmal ontrol governed by lnear tme delay systems. he gven manner s based on onvertng the orgnal problem to a nonlnear programmng problem. One nterestng advantage o the proposed method s ts smplty. he numeral results show that nreasng the number o ponts, t s possble to mprove the obetve unton as well as the onvergene o approxmate soluton o the problem may lead to the exat optmal soluton. Also the derved results ndate the that the proposed approah leads to nd the traetory and ontrol untons that the orrespondng obetve unton s better than some other methods. Reerenes. Jamshd,.; and Wang, C.. (984). A omputatonal algorthm or largesale nonlnear tme-delay systems. IEEE ransatons on Systems an and Cybernets, 4(), -9.. Rabah, R.; and Slyar, G. (7). On exat ontrollablty o lnear tme delay systems o natural type, Applatons o me Delay Systems, Leture Notes n Control and Inormaton Senes, 35, Dadebo, S.; and Luus, R. (99). Optmal ontrol o tme-delay systems by dynam programmng. Journal o Optmzaton heory and Applatons, 3(), Furutaa, K.; Yamataa,.; and Sato, Y. (988). Computaton o optmal ontrol or lnear systems wth delay. Internatonal Journal o Control, 48(), Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
13 498 A. H. Borzabad and S. Asad 5. Horng, I.R.; and Chou, J.H. (985). Analyss, parameter estmaton and optmal ontrol o tme-delay systems va Chebyshev seres. Internatonal Journal o Control, 4(5), Kung, F.C.; and Lee, H. (983). Soluton and parameter estmaton o lnearnvarant delay systems usng Laguerre polynomal expanson. ransatons ASE Journal o Dynam Systems, easurement and Control, 5(4), Hwang, C.; and Shh, Y.P. (985). Optmal ontrol o delay systems va blo pulse unton. Journal o Optmzaton heory and Applatons, 45(), Wang,.. (7). Numeral solutons o optmal ontrol or tme delay systems by hybrd o blo-pulse untons and legendre polynomals. Appled athemats and Computaton, 84(), Khellat, F. (9). Optmal Control o Lnear me-delayed Systems by Lnear Legendre ul-twavelets. Journal o Optmzaton heory and Applatons, 43(), 7-.. Palansamy, K.R.; and Rao, G.P. (983). Optmal ontrol o lnear systems wth delays n state and ontrol va Walsh untons. IEEE Proeedngs, 3(6), Da, R.; and Cohran, J.E. Jr. (9). Wavelet Colloaton ethod or Optmal ontrol Problems. Journal o Optmmzaton heory and Applatons, 43(), Hargraves, C.R.; and Pars, S.W. (987). Dret traetory optmzaton usng nonlnear programmng and olloaton. Journal o Gudane, Control and Dynams, (4), Fahroo,.; and Ross, I.. (). Dret traetory optmzaton by a hebyshev pseudospetral method. Journal o Gudane, Control and Dynams, 5(), Gu, J.S.; and Jang W.S. (996). he Haar Wavelet operaton matrx o ntegraton. Internatonal Journal o Systems Sene, 7(7), Lanaster, P. (969). heory o atres. New Yor: Aadem Press. 6. eo, K.L.; Wong, K.H.; and Clements, D.J. (984). Optmal ontrol omputaton or lnear tme-lag systems wth lnear termnal onstrans. Journal o Optmzaton heory and Applatons, 44(3), Journal o Engneerng Sene and ehnology Otober 6, Vol. ()
Journal of Engineering and Applied Sciences. Ultraspherical Integration Method for Solving Beam Bending Boundary Value Problem
Journal of Engneerng and Appled Senes Volue: Edton: Year: 4 Pages: 7 4 Ultraspheral Integraton Method for Solvng Bea Bendng Boundary Value Proble M El-Kady Matheats Departent Faulty of Sene Helwan UnverstyEgypt
More informationController Design for Networked Control Systems in Multiple-packet Transmission with Random Delays
Appled Mehans and Materals Onlne: 03-0- ISSN: 66-748, Vols. 78-80, pp 60-604 do:0.408/www.sentf.net/amm.78-80.60 03 rans eh Publatons, Swtzerland H Controller Desgn for Networed Control Systems n Multple-paet
More informationOn Generalized Fractional Hankel Transform
Int. ournal o Math. nalss Vol. 6 no. 8 883-896 On Generaled Fratonal ankel Transorm R. D. Tawade Pro.Ram Meghe Insttute o Tehnolog & Researh Badnera Inda rajendratawade@redmal.om. S. Gudadhe Dept.o Mathemats
More informationChapter 3 Differentiation and Integration
MEE07 Computer Modelng Technques n Engneerng Chapter Derentaton and Integraton Reerence: An Introducton to Numercal Computatons, nd edton, S. yakowtz and F. zdarovsky, Mawell/Macmllan, 990. Derentaton
More informationALGEBRAIC SCHUR COMPLEMENT APPROACH FOR A NON LINEAR 2D ADVECTION DIFFUSION EQUATION
st Annual Internatonal Interdsplnary Conferene AIIC 03 4-6 Aprl Azores Portugal - Proeedngs- ALGEBRAIC SCHUR COMPLEMENT APPROACH FOR A NON LINEAR D ADVECTION DIFFUSION EQUATION Hassan Belhad Professor
More informationLecture-7. Homework (Due 2/13/03)
Leture-7 Ste Length Seleton Homewor Due /3/3 3. 3. 3.5 3.6 3.7 3.9 3. Show equaton 3.44 he last ste n the roo o heorem 3.6. see sldes Show that >.5, the lne searh would exlude the mnmzer o a quadrat, and
More informationDOAEstimationforCoherentSourcesinBeamspace UsingSpatialSmoothing
DOAEstmatonorCoherentSouresneamspae UsngSpatalSmoothng YnYang,ChunruWan,ChaoSun,QngWang ShooloEletralandEletronEngneerng NanangehnologalUnverst,Sngapore,639798 InsttuteoAoustEngneerng NorthwesternPoltehnalUnverst,X
More informationrepresents the amplitude of the signal after modulation and (t) is the phase of the carrier wave.
1 IQ Sgnals general overvew 2 IQ reevers IQ Sgnals general overvew Rado waves are used to arry a message over a dstane determned by the ln budget The rado wave (alled a arrer wave) s modulated (moded)
More informationOPTIMISATION. Introduction Single Variable Unconstrained Optimisation Multivariable Unconstrained Optimisation Linear Programming
OPTIMIATION Introducton ngle Varable Unconstraned Optmsaton Multvarable Unconstraned Optmsaton Lnear Programmng Chapter Optmsaton /. Introducton In an engneerng analss, sometmes etremtes, ether mnmum or
More information36.1 Why is it important to be able to find roots to systems of equations? Up to this point, we have discussed how to find the solution to
ChE Lecture Notes - D. Keer, 5/9/98 Lecture 6,7,8 - Rootndng n systems o equatons (A) Theory (B) Problems (C) MATLAB Applcatons Tet: Supplementary notes rom Instructor 6. Why s t mportant to be able to
More informationTransfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system
Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng
More informationSolving Fractional Nonlinear Fredholm Integro-differential Equations via Hybrid of Rationalized Haar Functions
ISSN 746-7659 England UK Journal of Informaton and Computng Scence Vol. 9 No. 3 4 pp. 69-8 Solvng Fractonal Nonlnear Fredholm Integro-dfferental Equatons va Hybrd of Ratonalzed Haar Functons Yadollah Ordokhan
More informationFAULT DETECTION AND IDENTIFICATION BASED ON FULLY-DECOUPLED PARITY EQUATION
Control 4, Unversty of Bath, UK, September 4 FAUL DEECION AND IDENIFICAION BASED ON FULLY-DECOUPLED PARIY EQUAION C. W. Chan, Hua Song, and Hong-Yue Zhang he Unversty of Hong Kong, Hong Kong, Chna, Emal:
More information425. Calculation of stresses in the coating of a vibrating beam
45. CALCULAION OF SRESSES IN HE COAING OF A VIBRAING BEAM. 45. Calulaton of stresses n the oatng of a vbratng beam M. Ragulsks,a, V. Kravčenken,b, K. Plkauskas,, R. Maskelunas,a, L. Zubavčus,b, P. Paškevčus,d
More informationEEE 241: Linear Systems
EEE : Lnear Systems Summary #: Backpropagaton BACKPROPAGATION The perceptron rule as well as the Wdrow Hoff learnng were desgned to tran sngle layer networks. They suffer from the same dsadvantage: they
More informationAdaptive Multilayer Neural Network Control of Blood Pressure
Proeedng of st Internatonal Symposum on Instrument Sene and Tenology. ISIST 99. P4-45. 999. (ord format fle: ISIST99.do) Adaptve Multlayer eural etwork ontrol of Blood Pressure Fe Juntao, Zang bo Department
More informationInstance-Based Learning and Clustering
Instane-Based Learnng and Clusterng R&N 04, a bt of 03 Dfferent knds of Indutve Learnng Supervsed learnng Bas dea: Learn an approxmaton for a funton y=f(x based on labelled examples { (x,y, (x,y,, (x n,y
More informationLecture 12: Discrete Laplacian
Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly
More informationhapter 6 System Norms 6. Introducton s n the matrx case, the measure on a system should be nduced from the space of sgnals t operates on. hus, the sze
Lectures on Dynamc Systems and ontrol Mohammed Dahleh Munther. Dahleh George Verghese Department of Electrcal Engneerng and omputer Scence Massachuasetts Insttute of echnology c hapter 6 System Norms 6.
More informationModule 3: Element Properties Lecture 1: Natural Coordinates
Module 3: Element Propertes Lecture : Natural Coordnates Natural coordnate system s bascally a local coordnate system whch allows the specfcaton of a pont wthn the element by a set of dmensonless numbers
More informationPhysics 2B Chapter 17 Notes - Calorimetry Spring 2018
Physs 2B Chapter 17 Notes - Calormetry Sprng 2018 hermal Energy and Heat Heat Capaty and Spe Heat Capaty Phase Change and Latent Heat Rules or Calormetry Problems hermal Energy and Heat Calormetry lterally
More informationLecture 2 Solution of Nonlinear Equations ( Root Finding Problems )
Lecture Soluton o Nonlnear Equatons Root Fndng Problems Dentons Classcaton o Methods Analytcal Solutons Graphcal Methods Numercal Methods Bracketng Methods Open Methods Convergence Notatons Root Fndng
More informationSome remarks about the transformation of Charnes and Cooper by Ezio Marchi *)
Some remars about the transformaton of Charnes an Cooper b Eo Marh * Abstrat In ths paper we eten n a smple wa the transformaton of Charnes an Cooper to the ase where the funtonal rato to be onsere are
More informationStatistical Analysis of Environmental Data - Academic Year Prof. Fernando Sansò CLUSTER ANALYSIS
Statstal Analyss o Envronmental Data - Aadem Year 008-009 Pro. Fernando Sansò EXERCISES - PAR CLUSER ANALYSIS Supervsed Unsupervsed Determnst Stohast Determnst Stohast Dsrmnant Analyss Bayesan Herarhal
More informationLinear Feature Engineering 11
Lnear Feature Engneerng 11 2 Least-Squares 2.1 Smple least-squares Consder the followng dataset. We have a bunch of nputs x and correspondng outputs y. The partcular values n ths dataset are x y 0.23 0.19
More informationU.C. Berkeley CS294: Beyond Worst-Case Analysis Luca Trevisan September 5, 2017
U.C. Berkeley CS94: Beyond Worst-Case Analyss Handout 4s Luca Trevsan September 5, 07 Summary of Lecture 4 In whch we ntroduce semdefnte programmng and apply t to Max Cut. Semdefnte Programmng Recall that
More informationChapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems
Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons
More information1 Convex Optimization
Convex Optmzaton We wll consder convex optmzaton problems. Namely, mnmzaton problems where the objectve s convex (we assume no constrants for now). Such problems often arse n machne learnng. For example,
More informationDifference Equations
Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1
More informationAPPENDIX A Some Linear Algebra
APPENDIX A Some Lnear Algebra The collecton of m, n matrces A.1 Matrces a 1,1,..., a 1,n A = a m,1,..., a m,n wth real elements a,j s denoted by R m,n. If n = 1 then A s called a column vector. Smlarly,
More informationProblem Set 9 Solutions
Desgn and Analyss of Algorthms May 4, 2015 Massachusetts Insttute of Technology 6.046J/18.410J Profs. Erk Demane, Srn Devadas, and Nancy Lynch Problem Set 9 Solutons Problem Set 9 Solutons Ths problem
More informationIntroduction to Molecular Spectroscopy
Chem 5.6, Fall 004 Leture #36 Page Introduton to Moleular Spetrosopy QM s essental for understandng moleular spetra and spetrosopy. In ths leture we delneate some features of NMR as an ntrodutory example
More informationAPPROXIMATE PRICES OF BASKET AND ASIAN OPTIONS DUPONT OLIVIER. Premia 14
APPROXIMAE PRICES OF BASKE AND ASIAN OPIONS DUPON OLIVIER Prema 14 Contents Introducton 1 1. Framewor 1 1.1. Baset optons 1.. Asan optons. Computng the prce 3. Lower bound 3.1. Closed formula for the prce
More informationCHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE
CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE Analytcal soluton s usually not possble when exctaton vares arbtrarly wth tme or f the system s nonlnear. Such problems can be solved by numercal tmesteppng
More informationJSM Survey Research Methods Section. Is it MAR or NMAR? Michail Sverchkov
JSM 2013 - Survey Researh Methods Seton Is t MAR or NMAR? Mhal Sverhkov Bureau of Labor Statsts 2 Massahusetts Avenue, NE, Sute 1950, Washngton, DC. 20212, Sverhkov.Mhael@bls.gov Abstrat Most methods that
More informationGlobal Sensitivity. Tuesday 20 th February, 2018
Global Senstvty Tuesday 2 th February, 28 ) Local Senstvty Most senstvty analyses [] are based on local estmates of senstvty, typcally by expandng the response n a Taylor seres about some specfc values
More informationA Hybrid Variational Iteration Method for Blasius Equation
Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method
More informationTenth Order Compact Finite Difference Method for Solving Singularly Perturbed 1D Reaction - Diffusion Equations
Internatonal Journal of Engneerng & Appled Senes (IJEAS) Vol.8, Issue (0)5- Tent Order Compat Fnte Dfferene Metod for Solvng Sngularl Perturbed D Reaton - Dffuson Equatons Faska Wondmu Galu, Gemes Fle
More informationCIVL 8/7117 Chapter 10 - Isoparametric Formulation 42/56
CIVL 8/77 Chapter 0 - Isoparametrc Formulaton 4/56 Newton-Cotes Example Usng the Newton-Cotes method wth = ntervals (n = 3 samplng ponts), evaluate the ntegrals: x x cos dx 3 x x dx 3 x x dx 4.3333333
More informationInterval Valued Neutrosophic Soft Topological Spaces
8 Interval Valued Neutrosoph Soft Topologal njan Mukherjee Mthun Datta Florentn Smarandah Department of Mathemats Trpura Unversty Suryamannagar gartala-7990 Trpura Indamal: anjan00_m@yahooon Department
More informationbe a second-order and mean-value-zero vector-valued process, i.e., for t E
CONFERENCE REPORT 617 DSCUSSON OF TWO PROCEDURES FOR EXPANDNG A VECTOR-VALUED STOCHASTC PROCESS N AN ORTHONORMAL WAY by R. GUTkRREZ and M. J. VALDERRAMA 1. ntroducton Snce K. Karhunen [l] and M. Lo&e [2]
More informationPhase Transition in Collective Motion
Phase Transton n Colletve Moton Hefe Hu May 4, 2008 Abstrat There has been a hgh nterest n studyng the olletve behavor of organsms n reent years. When the densty of lvng systems s nreased, a phase transton
More informationChapter Newton s Method
Chapter 9. Newton s Method After readng ths chapter, you should be able to:. Understand how Newton s method s dfferent from the Golden Secton Search method. Understand how Newton s method works 3. Solve
More informationECEN 5005 Crystals, Nanocrystals and Device Applications Class 19 Group Theory For Crystals
ECEN 5005 Crystals, Nanocrystals and Devce Applcatons Class 9 Group Theory For Crystals Dee Dagram Radatve Transton Probablty Wgner-Ecart Theorem Selecton Rule Dee Dagram Expermentally determned energy
More information: Numerical Analysis Topic 2: Solution of Nonlinear Equations Lectures 5-11:
764: Numercal Analyss Topc : Soluton o Nonlnear Equatons Lectures 5-: UIN Malang Read Chapters 5 and 6 o the tetbook 764_Topc Lecture 5 Soluton o Nonlnear Equatons Root Fndng Problems Dentons Classcaton
More informationCollege of Computer & Information Science Fall 2009 Northeastern University 20 October 2009
College of Computer & Informaton Scence Fall 2009 Northeastern Unversty 20 October 2009 CS7880: Algorthmc Power Tools Scrbe: Jan Wen and Laura Poplawsk Lecture Outlne: Prmal-dual schema Network Desgn:
More informationNumerical Heat and Mass Transfer
Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and
More informationMMA and GCMMA two methods for nonlinear optimization
MMA and GCMMA two methods for nonlnear optmzaton Krster Svanberg Optmzaton and Systems Theory, KTH, Stockholm, Sweden. krlle@math.kth.se Ths note descrbes the algorthms used n the author s 2007 mplementatons
More informationSome modelling aspects for the Matlab implementation of MMA
Some modellng aspects for the Matlab mplementaton of MMA Krster Svanberg krlle@math.kth.se Optmzaton and Systems Theory Department of Mathematcs KTH, SE 10044 Stockholm September 2004 1. Consdered optmzaton
More informationClustering. CS4780/5780 Machine Learning Fall Thorsten Joachims Cornell University
Clusterng CS4780/5780 Mahne Learnng Fall 2012 Thorsten Joahms Cornell Unversty Readng: Mannng/Raghavan/Shuetze, Chapters 16 (not 16.3) and 17 (http://nlp.stanford.edu/ir-book/) Outlne Supervsed vs. Unsupervsed
More informationClustering-Inverse: A Generalized Model for Pattern-Based Time Series Segmentation*
Journal of Intellgent Learnng ystems and Applatons, 2, 3, 26-36 do:.4236/lsa.2.34 ublshed Onlne February 2 (http://www.r.org/ournal/lsa) Clusterng-Inverse: A Generalzed Model for attern-based Tme eres
More informationELEKTRYKA 2016 Zeszyt 3-4 ( )
ELEKTRYKA 206 Zeszyt 3-4 (239-240) Rok LXII Waldemar BAUER, Jerzy BARANOWSKI, Tomasz DZIWIŃSKI, Paweł PIĄTEK, Marta ZAGÓROWSKA AGH Unversty of Sene and Tehnology, Kraków OUSTALOUP PARALLEL APPROXIMATION
More informationComplex Variables. Chapter 18 Integration in the Complex Plane. March 12, 2013 Lecturer: Shih-Yuan Chen
omplex Varables hapter 8 Integraton n the omplex Plane March, Lecturer: Shh-Yuan hen Except where otherwse noted, content s lcensed under a BY-N-SA. TW Lcense. ontents ontour ntegrals auchy-goursat theorem
More informationHongyi Miao, College of Science, Nanjing Forestry University, Nanjing ,China. (Received 20 June 2013, accepted 11 March 2014) I)ϕ (k)
ISSN 1749-3889 (prnt), 1749-3897 (onlne) Internatonal Journal of Nonlnear Scence Vol.17(2014) No.2,pp.188-192 Modfed Block Jacob-Davdson Method for Solvng Large Sparse Egenproblems Hongy Mao, College of
More informationNumerical Methods Solution of Nonlinear Equations
umercal Methods Soluton o onlnear Equatons Lecture Soluton o onlnear Equatons Root Fndng Prolems Dentons Classcaton o Methods Analytcal Solutons Graphcal Methods umercal Methods Bracketng Methods Open
More informationCHAPTER 4d. ROOTS OF EQUATIONS
CHAPTER 4d. ROOTS OF EQUATIONS A. J. Clark School o Engneerng Department o Cvl and Envronmental Engneerng by Dr. Ibrahm A. Assakka Sprng 00 ENCE 03 - Computaton Methods n Cvl Engneerng II Department o
More informationImproving the Performance of Fading Channel Simulators Using New Parameterization Method
Internatonal Journal of Eletrons and Eletral Engneerng Vol. 4, No. 5, Otober 06 Improvng the Performane of Fadng Channel Smulators Usng New Parameterzaton Method Omar Alzoub and Moheldn Wanakh Department
More informationprinceton univ. F 17 cos 521: Advanced Algorithm Design Lecture 7: LP Duality Lecturer: Matt Weinberg
prnceton unv. F 17 cos 521: Advanced Algorthm Desgn Lecture 7: LP Dualty Lecturer: Matt Wenberg Scrbe: LP Dualty s an extremely useful tool for analyzng structural propertes of lnear programs. Whle there
More informationLinear Approximation with Regularization and Moving Least Squares
Lnear Approxmaton wth Regularzaton and Movng Least Squares Igor Grešovn May 007 Revson 4.6 (Revson : March 004). 5 4 3 0.5 3 3.5 4 Contents: Lnear Fttng...4. Weghted Least Squares n Functon Approxmaton...
More informationU.C. Berkeley CS294: Spectral Methods and Expanders Handout 8 Luca Trevisan February 17, 2016
U.C. Berkeley CS94: Spectral Methods and Expanders Handout 8 Luca Trevsan February 7, 06 Lecture 8: Spectral Algorthms Wrap-up In whch we talk about even more generalzatons of Cheeger s nequaltes, and
More informationFall 2012 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede
Fall 0 Analyss of Expermental easurements B. Esensten/rev. S. Errede We now reformulate the lnear Least Squares ethod n more general terms, sutable for (eventually extendng to the non-lnear case, and also
More information, rst we solve te PDE's L ad L ad n g g (x) = ; = ; ; ; n () (x) = () Ten, we nd te uncton (x), te lnearzng eedbac and coordnates transormaton are gve
Freedom n Coordnates Transormaton or Exact Lnearzaton and ts Applcaton to Transent Beavor Improvement Kenj Fujmoto and Tosaru Suge Dvson o Appled Systems Scence, Kyoto Unversty, Uj, Kyoto, Japan suge@robotuassyoto-uacjp
More informationQuantum Mechanics for Scientists and Engineers. David Miller
Quantum Mechancs for Scentsts and Engneers Davd Mller Types of lnear operators Types of lnear operators Blnear expanson of operators Blnear expanson of lnear operators We know that we can expand functons
More informationOutline. Clustering: Similarity-Based Clustering. Supervised Learning vs. Unsupervised Learning. Clustering. Applications of Clustering
Clusterng: Smlarty-Based Clusterng CS4780/5780 Mahne Learnng Fall 2013 Thorsten Joahms Cornell Unversty Supervsed vs. Unsupervsed Learnng Herarhal Clusterng Herarhal Agglomeratve Clusterng (HAC) Non-Herarhal
More informationcan be decomposed into r augmenting cycles and the sum of the costs of these cycles equals, c . But since is optimum, we must have c
Ameran Internatonal Journal of Researh n Sene, Tehnology, Engneerng & Mathemats Avalable onlne at http://www.asr.net ISSN (Prnt): 8-9, ISSN (Onlne): 8-8, ISSN (CD-ROM): 8-69 AIJRSTEM s a refereed, ndexed,
More information4DVAR, according to the name, is a four-dimensional variational method.
4D-Varatonal Data Assmlaton (4D-Var) 4DVAR, accordng to the name, s a four-dmensonal varatonal method. 4D-Var s actually a drect generalzaton of 3D-Var to handle observatons that are dstrbuted n tme. The
More informationA new mixed integer linear programming model for flexible job shop scheduling problem
A new mxed nteger lnear programmng model for flexble job shop shedulng problem Mohsen Zaee Department of Industral Engneerng, Unversty of Bojnord, 94531-55111 Bojnord, Iran Abstrat. In ths paper, a mxed
More informationA computer-aided optimization method of bending beams
WSES Internatonal Conferene on ENGINEERING MECHNICS, STRUCTURES, ENGINEERING GEOLOGY (EMESEG '8), Heraklon, Crete Island, Greee, July 22-24, 28 omputer-aded optmzaton method of bendng beams CRMEN E. SINGER-ORCI
More informationCISE301: Numerical Methods Topic 2: Solution of Nonlinear Equations
CISE3: Numercal Methods Topc : Soluton o Nonlnear Equatons Dr. Amar Khoukh Term Read Chapters 5 and 6 o the tetbook CISE3_Topc c Khoukh_ Lecture 5 Soluton o Nonlnear Equatons Root ndng Problems Dentons
More informationTracking with Kalman Filter
Trackng wth Kalman Flter Scott T. Acton Vrgna Image and Vdeo Analyss (VIVA), Charles L. Brown Department of Electrcal and Computer Engneerng Department of Bomedcal Engneerng Unversty of Vrgna, Charlottesvlle,
More informationLecture 26 Finite Differences and Boundary Value Problems
4//3 Leture 6 Fnte erenes and Boundar Value Problems Numeral derentaton A nte derene s an appromaton o a dervatve - eample erved rom Talor seres 3 O! Negletng all terms ger tan rst order O O Tat s te orward
More informationSolutions HW #2. minimize. Ax = b. Give the dual problem, and make the implicit equality constraints explicit. Solution.
Solutons HW #2 Dual of general LP. Fnd the dual functon of the LP mnmze subject to c T x Gx h Ax = b. Gve the dual problem, and make the mplct equalty constrants explct. Soluton. 1. The Lagrangan s L(x,
More informationCubic Trigonometric B-Spline Applied to Linear Two-Point Boundary Value Problems of Order Two
World Academy of Scence Engneerng and echnology Internatonal Journal of Mathematcal and omputatonal Scences Vol: No:0 00 ubc rgonometrc B-Splne Appled to Lnear wo-pont Boundary Value Problems of Order
More information1 Derivation of Point-to-Plane Minimization
1 Dervaton of Pont-to-Plane Mnmzaton Consder the Chen-Medon (pont-to-plane) framework for ICP. Assume we have a collecton of ponts (p, q ) wth normals n. We want to determne the optmal rotaton and translaton
More informationSingle Variable Optimization
8/4/07 Course Instructor Dr. Raymond C. Rump Oce: A 337 Phone: (95) 747 6958 E Mal: rcrump@utep.edu Topc 8b Sngle Varable Optmzaton EE 4386/530 Computatonal Methods n EE Outlne Mathematcal Prelmnares Sngle
More informationLecture 2: Gram-Schmidt Vectors and the LLL Algorithm
NYU, Fall 2016 Lattces Mn Course Lecture 2: Gram-Schmdt Vectors and the LLL Algorthm Lecturer: Noah Stephens-Davdowtz 2.1 The Shortest Vector Problem In our last lecture, we consdered short solutons to
More informationC/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1
C/CS/Phy9 Problem Set 3 Solutons Out: Oct, 8 Suppose you have two qubts n some arbtrary entangled state ψ You apply the teleportaton protocol to each of the qubts separately What s the resultng state obtaned
More informationModule 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur
Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:
More informationThe calculation of ternary vapor-liquid system equilibrium by using P-R equation of state
The alulaton of ternary vapor-lqud syste equlbru by usng P-R equaton of state Y Lu, Janzhong Yn *, Rune Lu, Wenhua Sh and We We Shool of Cheal Engneerng, Dalan Unversty of Tehnology, Dalan 11601, P.R.Chna
More information2 Finite difference basics
Numersche Methoden 1, WS 11/12 B.J.P. Kaus 2 Fnte dfference bascs Consder the one- The bascs of the fnte dfference method are best understood wth an example. dmensonal transent heat conducton equaton T
More informationMagnitude Approximation of IIR Digital Filter using Greedy Search Method
Ranjt Kaur, Damanpreet Sngh Magntude Approxmaton of IIR Dgtal Flter usng Greedy Searh Method RANJIT KAUR, DAMANPREET SINGH Department of Eletrons & Communaton, Department of Computer Sene & Engnnerng Punjab
More informationExample: (13320, 22140) =? Solution #1: The divisors of are 1, 2, 3, 4, 5, 6, 9, 10, 12, 15, 18, 20, 27, 30, 36, 41,
The greatest common dvsor of two ntegers a and b (not both zero) s the largest nteger whch s a common factor of both a and b. We denote ths number by gcd(a, b), or smply (a, b) when there s no confuson
More informationUniform bounds on the 1-norm of the inverse of lower triangular Toeplitz matrices
Unform bounds on the -norm of the nverse of lower trangular Toepltz matres X Lu S MKee J Y Yuan X Y Yuan Aprl 2, 2 Abstrat A unform bound of the norm s gven for the nverse of lower trangular Toepltz matres
More informationMEM 255 Introduction to Control Systems Review: Basics of Linear Algebra
MEM 255 Introducton to Control Systems Revew: Bascs of Lnear Algebra Harry G. Kwatny Department of Mechancal Engneerng & Mechancs Drexel Unversty Outlne Vectors Matrces MATLAB Advanced Topcs Vectors A
More informationImplicit Integration Henyey Method
Implct Integraton Henyey Method In realstc stellar evoluton codes nstead of a drect ntegraton usng for example the Runge-Kutta method one employs an teratve mplct technque. Ths s because the structure
More informationAvailable online at ScienceDirect. Energy Procedia 70 (2015 )
Avalable onlne at www.senedret.om SeneDret Energy Proeda 70 015 371 378 Internatonal Conerene on Solar Heatng and Coolng or Buldngs and Industry, SHC 014 The eet o measurement unertanty and envronment
More informationThe Similar Structure Method for Solving Boundary Value Problems of a Three Region Composite Bessel Equation
The Smlar Struture Method for Solvng Boundary Value Problems of a Three Regon Composte Bessel Equaton Mngmng Kong,Xaou Dong Center for Rado Admnstraton & Tehnology Development, Xhua Unversty, Chengdu 69,
More informationThe corresponding link function is the complementary log-log link The logistic model is comparable with the probit model if
SK300 and SK400 Lnk funtons for bnomal GLMs Autumn 08 We motvate the dsusson by the beetle eample GLMs for bnomal and multnomal data Covers the followng materal from hapters 5 and 6: Seton 5.6., 5.6.3,
More informationwhere the sums are over the partcle labels. In general H = p2 2m + V s(r ) V j = V nt (jr, r j j) (5) where V s s the sngle-partcle potental and V nt
Physcs 543 Quantum Mechancs II Fall 998 Hartree-Fock and the Self-consstent Feld Varatonal Methods In the dscusson of statonary perturbaton theory, I mentoned brey the dea of varatonal approxmaton schemes.
More informationLECTURE 9 CANONICAL CORRELATION ANALYSIS
LECURE 9 CANONICAL CORRELAION ANALYSIS Introducton he concept of canoncal correlaton arses when we want to quantfy the assocatons between two sets of varables. For example, suppose that the frst set of
More informationASSESSMENT OF UNCERTAINTY IN ESTIMATION OF STORED AND RECOVERABLE THERMAL ENERGY IN GEOTHERMAL RESERVOIRS BY VOLUMETRIC METHODS
PROCEEDINGS, Thrty-Fourth Workshop on Geothermal Reservor Engneerng Stanord Unversty, Stanord, Calorna, February 9-11, 009 SGP-TR-187 ASSESSMENT OF UNCERTAINTY IN ESTIMATION OF STORED AND RECOVERABLE THERMAL
More informationPrediction of Solid Paraffin Precipitation Using Solid Phase Equation of State
Predton of old Paraffn Preptaton Usng old Phase Equaton of tate Proeedngs of European Congress of Chemal Engneerng (ECCE-6) Copenhagen, 16- eptember 7 Predton of old Paraffn Preptaton Usng old Phase Equaton
More informationQuantum Mechanics for Scientists and Engineers
Quantu Mechancs or Scentsts and Engneers Sangn K Advanced Coputatonal Electroagnetcs Lab redkd@yonse.ac.kr Nov. 4 th, 26 Outlne Quantu Mechancs or Scentsts and Engneers Blnear expanson o lnear operators
More informationFinite Difference Method
7/0/07 Instructor r. Ramond Rump (9) 747 698 rcrump@utep.edu EE 337 Computatonal Electromagnetcs (CEM) Lecture #0 Fnte erence Method Lecture 0 These notes ma contan coprghted materal obtaned under ar use
More information6.3.4 Modified Euler s method of integration
6.3.4 Modfed Euler s method of ntegraton Before dscussng the applcaton of Euler s method for solvng the swng equatons, let us frst revew the basc Euler s method of numercal ntegraton. Let the general from
More informationMachine Learning: and 15781, 2003 Assignment 4
ahne Learnng: 070 and 578, 003 Assgnment 4. VC Dmenson 30 onts Consder the spae of nstane X orrespondng to all ponts n the D x, plane. Gve the VC dmenson of the followng hpothess spaes. No explanaton requred.
More informationCS 331 DESIGN AND ANALYSIS OF ALGORITHMS DYNAMIC PROGRAMMING. Dr. Daisy Tang
CS DESIGN ND NLYSIS OF LGORITHMS DYNMIC PROGRMMING Dr. Dasy Tang Dynamc Programmng Idea: Problems can be dvded nto stages Soluton s a sequence o decsons and the decson at the current stage s based on the
More information1 Matrix representations of canonical matrices
1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:
More informationME 501A Seminar in Engineering Analysis Page 1
umercal Solutons of oundary-value Problems n Os ovember 7, 7 umercal Solutons of oundary- Value Problems n Os Larry aretto Mechancal ngneerng 5 Semnar n ngneerng nalyss ovember 7, 7 Outlne Revew stff equaton
More informationSolutions to Problem Set 6
Solutons to Problem Set 6 Problem 6. (Resdue theory) a) Problem 4.7.7 Boas. n ths problem we wll solve ths ntegral: x sn x x + 4x + 5 dx: To solve ths usng the resdue theorem, we study ths complex ntegral:
More information