Iterative learning control with initial rectifying action for nonlinear continuous systems X.-D. Li 1 T.W.S. Chow 2 J.K.L. Ho 3 J.

Size: px
Start display at page:

Download "Iterative learning control with initial rectifying action for nonlinear continuous systems X.-D. Li 1 T.W.S. Chow 2 J.K.L. Ho 3 J."

Transcription

1 Publishd in IET Control Thory and Applications Rcivd on 24th Dcmbr 27 Rvisd on 21st May 28 doi: 1.149/it-cta:27486 ISSN Itrativ larning control with initial rctifying action for nonlinar continuous systms X.-D. Li 1 T.W.S. Chow 2 J.K.L. Ho 3 J. Zhang 1 1 School of Information Scinc and Tchnology, Sun Yat-Sn Univrsity, Guangzhou, Popl s Rpublic of China 2 Dpartmnt of Elctronic Enginring, City Univrsity of Hong Kong, 83 Tat Ch Avnu, Kowloon, Hong Kong, Popl s Rpublic of China 3 Dpartmnt of Manufacturing Enginring and Enginring Managmnt, City Univrsity of Hong Kong, 83 Tat Ch Avnu, Kowloon, Hong Kong, Popl s Rpublic of China lixd@mail.sysu.du.cn Abstract: A nw itrativ larning control (ILC) mthod with initial rctifying action for nonlinar continuous multivariabl systms is prsntd. Unlik gnral ILC tchniqus, th proposd ILC approach allows initial outputs of an ILC systm at diffrnt itrations to fluctuat randomly around th initial valu of th dsird output. Th proposd stratgy includs an initial rctifying action of ILC on a vry small initial tim intrval, and pursus th rfrnc trajctory tracking byond th initial tim intrval. Th output tracking rror byond th initial tim intrval can b drivn to a rsidual st whos siz dpnds on th stimation rror of input matrix. A numrical xampl is usd to illustrat th ffctivnss of th proposd ILC approach. 1 Introduction Itrativ larning control (ILC) is a vrsatil control tchniqu to improv transint rspons of a systm oprating rptitivly ovr a fixd tim intrval. On of th important faturs of ILC is that it rquirs lss a priori knowldg about th controlld systm in th cours of dsign. This maks ILC incrasingly important in control applications, such as robot manipulators and disk driv systms that ar mostly dsignd for rptitiv tasks. Until now, thr hav bn a lot of ILC algorithms rportd. But most of th xisting ILC works assum that th initial outputs of an ILC systm at diffrnt itrations wr kpt invariant [1, 2], which mans that th ILC systm must hav a fixd initial rror at diffrnt itrations. In som cass, a mor stringnt condition of zro initial rror is vn rquird [3 6]. All of ths hypothsiss ar difficult to b implmntd in practic, as locating opration rptitivly in an ILC application can rsult in irrgular drifts of initial outputs at diffrnt itrations to th initial valu of th dsird output. Clarly, th study of ILC problm applid to dynamical systms with non-fixd initial rrors is ssntial. Th difficulty of ILC with non-fixd initial rror mainly lis in th dynamical complxity of ILC in which initial itrativ rror intracts with not only th systm dynamics but also th itrativ larning procss. L and Bin [7] rportd som novl undsirabl phnomnon du to th mismatch in th initial conditions in ILC procss. Thy pointd out that th control systm could bcom unstabl whn th initial output at ach itration was diffrnt from th prvious initial output. Thr ar a fw rsarch paprs [8 1] discussing th robustnss of ILC algorithms to non-fixd initial rrors, but th bound of robustnss is normally too larg and cannot b adjustd for practically tracking a rfrnc trajctory. As a rsult, an initial rctifying action should b considrd in ILC dsign. It is worth noting that thr hav bn works [11, 12] incorporating an initial rctifying action into ILC dsign to achiv complt tracking of a rfrnc trajctory ovr a spcifid intrval, but thy rquir that th initial rror b a fixd valu. Thy will not work whn a random or nonfixd initial rror is ncountrd. Hithrto, th rsarch on ILC applid to dynamical systms with non-fixd initial rrors still rmains an opn and important issu. Rcntly, a fw studis [13 17] hav bn focussd on th ILC problm of dynamical systms with non-fixd initial rrors. In [13], a mthod calld ILC with multi-modal input was proposd to tackl th ILC problm for linar IET Control Thory Appl., 29, Vol. 3, No. 1, pp doi: 1.149/it-cta:27486 & Th Institution of Enginring and Tchnology 29

2 continuous systms with non-fixd initial rrors. But it is computationally complx bcaus th dtrmind input is, in fact, th synthsis of th multi-modal ILC input with varying initial condition. In [14], undr a spcific condition, an avrag oprator-basd PD-typ ILC controllr for linar continuous systms with non-fixd initial rrors was invstigatd. In [17], an ILC controllr for linar discrt systms with non-fixd initial rrors was invstigatd using 2-D systm thory. Dspit its ability to handl variabl initial conditions, it is only ffctiv whn th tracking tim intrval is sufficintly larg. For ILC on nonlinar systms, Xu and Yan [15] discussd th inhrnt rlationship btwn diffrnt initial conditions and th corrsponding larning convrgnc (or bounddnss) proprty undr a Lyapunov-basd ILC mthod. Howvr, th proposd ILC tchniqu [15] is only suitabl for a class of simpl first-ordr nonlinar continuous systms with unit input gain. Furthrmor, a dirct adaptiv ILC approach basd on a fuzzy nural ntwork was prsntd in [16] for a class of nonlinar systms with non-fixd initial rrors. Using th proposd adaptiv ILC approach, th norm of stat tracking rror will asymptotically convrg to a tunabl rsidual st as itration gos to infinit. Th main objctiv of this papr is to dscrib how an initial rctifying action can b combind into th convntional D- typ ILC tchniqu for nonlinar continuous multivariabl (NCM) systms with non-fixd initial rrors. Byond th dsignatd initial tim intrval, th stablishd ILC tchniqu is abl to driv th output tracking rror to a rsidual st whos siz dpnds on th stimation rror of input matrix. It is also important to not that a prfct rfrnc trajctory tracking byond th initial tim intrval can b achivd whn an accurat knowldg on input matrix at th initial tim intrval is availabl. Th organisation of this papr is as follows. Sction 2 prsnts th ILC problm formulation and th ILC rul with initial rctifying action. Sction 3 invstigats th larning convrgnc of th proposd ILC rul undr nonfixd initial rrors. And th simulation rsults ar illustratd in Sction 4. Finally, Sction 5 concluds this papr. 2 Problm formulation and ILC rul with initial rctifying action Considr th following class of NCM systms prforming rptitiv tasks ovr a fixd tim intrval t [ [, T ] _x k (t) f (x k (t), t) þ B(t) u k (t) y k (t) C(t) x k (t) (1a) (1b) whr k dnots th kth rptitiv opration of th systm; x k (t) [ R n, u k (t) [ R m (m n), and y k (t) [ R p ar th stat, control input and output of th systm, rspctivly; B(t) [ R nm and C(t) [ R pn ar tim-variant matrics; th nonlinar function f (, ) : R n [, T ] 7! R n is locally Lipschitz in x k, that is, for all t [ [, T ] and k, thr xists a constant L f such that kf (x kþ1 (t), t) f (x k (t), t)k L f kx kþ1 (t) x k (t)k (2) whr th norm k.k will b dfind latr. An xampl of systm (1) can b rfrrd to th PM synchronous motor studid in [18]. Givn a rfrnc output trajctory y r (t) and an initial control input u (t) att [ [, T ], an ILC dsign for systm (1) is closly rlatd to its boundary conditions x k () for k, 1, 2... Unlik gnral ILC litraturs, w assum that x k () is boundd and diffrnt for k, 1, 2..., and y k () fluctuats randomly around y r () within a bound in this study. Basd on th givn boundary conditions, our ILC objctiv is to itrativly dtrmin a control input squnc fu k (t)g, t [ [, T ], such that as k gos to infinit, th output tracking rror y r (t) y k (t) ovr a spcifid tim intrval t [ [h, T ] can b drivn to a rsidual st whos siz dpnds on th stimation rror of input matrix B(t), whr h is a spcifid small ral numbr btwn and T. In many ILC applications, th modl information on th controlld systm, spcially th input matrix B(t), can b wll known. In this cas, our ILC dsign with th control objctiv can achiv an ffctiv rfrnc trajctory tracking. Th output tracking rror in ILC procss is dnotd as k (t) y r (t) y k (t) (3) Whn th initial ILC rrors k () for k, 1, 2...ar nonfixd, but boundd, it has bn shown in [9] that a wllknown D-typ ILC rul u kþ1 (t) u k (t) þ K (t)_ k (t) (4) can nsur th bounddnss of th output tracking rror k (t), t [ [, T ]ask gos to infinit. In practic, this bound is usually too larg to b applicabl to track a rfrnc trajctory. In this papr, a rctifying action is thn combind into a D-typ ILC rul (4), and th following ILC rul for control calculation is applid u kþ1 (t) u k (t) þ K (t)_ k (t) þ u h (t) ^B(t) 1 R X k () (5) whr ^B(t) dnots th stimation of B(t); ^B(t) 1 R invrs of ^B(t); and u h ðþ t 8 2 h 1 t <, t [ ½, hþ h :, t [ ½h, T is th right (6) X k () ^B()K () k () þ x k () x kþ1 () (7) For th convninc of convrgnc analysis of th proposd ILC approach, th following dfinitions and lmma on 5 IET Control Thory Appl., 29, Vol. 3, No. 1, pp & Th Institution of Enginring and Tchnology 29 doi: 1.149/it-cta:27486

3 norms ar givn ksk max js ðþ i j 1in kgk max 1im kqðþk t l X n t[ ½,T j1 jg i, j j! lt kqt ðþk, l. whr s [ s (1) s (2) s (n) ] T is a vctor, G [g i, j ] [ R mn is a matrix and q(t), t [ [, T ] is a ral function vctor/matrix. Spcially, in this papr, w us kq(t)k l j t[[h,t ] t[[h,t ] lt kq(t)k (8) to dfin l-norm of q(t) on th tim intrval t [ [h, T ]. On th rlationship btwn th norm k.k and th l-norm k.k l of a vctor x(t), t [ [, T ], w hav th following lmma 1. Lmma 1: t[ ½,T lt kxðþkdt t 1 l kxt ðþk l (9) Th proof of Lmma 1 is an immdiat consqunc of th norm k.k l, and thrfor is omittd. 3 Larning convrgnc undr non-fixd initial rrors In this sction, th convrgnc rsults of ILC rul (5) ar providd in Thorm 1. Thorm 1: For an NCM systm (1), pos that th rfrnc output y r (t) is diffrntiabl, and th initial ILC rror k () varis randomly within a bound. If thr xists a matrix K(t) to mak t[ ½,T ki Ct ðþbt ðþkt ðþkr, 1 (1) and th matrix B(t) att [ [, h] is right invrtibl; thn, th ILC rul (5) can nsur lim k k (t)k l j t[[h,t ] lm C(M E MX þ M MK ) k!1 (1 r)( ) (11) whr B(t) ^B(t) 1 R I þ E(t), t[[,h] ke(t)k M E, t[[,t ] kc(t)k M C, k ^B() B()k M, k kx k () kmx, k kk () k ()k M K,, r, 1, and l is a boundd valu. Espcially, whn th input matrix B(t) at t [ [, h] is accuratly known, w hav lim k!1 k k (t) k l j t[[h,t ]. Proof: From (1) and (5), w hav x kþ1 (t) x k (t) þ _x kþ1 (t) dt _x k (t) dt þ [x kþ1 () x k ()] þ B(t)[u kþ1 (t) u k (t)] dt þ [x kþ1 () x k ()] B(t)K (t)_ k (t) dt þ u h (t)b(t) ^B(t) 1 R dt X k () þ [x kþ1 () x k ()] [ f (x kþ1 (t), t) f (x k (t), t)] dt þ B(t)K (t) k (t) B()K () k () ð t dt k (t) dt þ u h (t)[i þ E(t)]dt X k () þ [x kþ1 () x k ()] (12) On th othr hand, from (1) and (3) kþ1 (t) y r (t) y kþ1 (t) k (t) [y kþ1 (t) y k (t)] k (t) C(t)[x kþ1 (t) x k (t)] (13) Substituting (12) into (13), w hav kþ1 (t) [I C(t)B(t)K (t)] k (t) C(t) þ C(t) C(t) dt k (t)dt u h (t)[i þ E(t)] dt X k () þ C(t)B()K () k () C(t)[x kþ1 () x k ()] (14) As t [ [h, T ], considring that Ð t u h (t)dt Ð h u h (t)dt 1 IET Control Thory Appl., 29, Vol. 3, No. 1, pp doi: 1.149/it-cta:27486 & Th Institution of Enginring and Tchnology 29

4 from (6), (12) and (14) can b, rspctivly, writtn as x kþ1 (t) x k (t) þ B(t)K (t) k (t) þ ð h dt k (t)dt u h (t)e(t)dt X k () þ [ ^B() B()]K () k () kþ1 (t) [I C(t)B(t)K (t)] k (t) C(t) þ C(t) ð h [f (x kþ1 (t), t) f (x k (t), t)] dt dt k (t)dt C(t) u h (t)e(t)dt X k () C(t)[ ^B() (15) B()]K () k () (16) Now, lt us indpndntly invstigat th proprtis of (15) and (16) on th whol tim intrval t [ [, T ]. Taking th norms on two sids of (15) and (16), rspctivly, w hav kx kþ1 (t) x k (t)k L f kx kþ1 (t) x k (t)k dt þ M 1 k k (t)kþm 2 k k (t)k dt þ M E M X þ M M K (17) k kþ1 (t)k r k k (t)kþm C L f kx kþ1 (t) x k (t)k dt þ M C M 2 k k (t)k dt þ M C M E M X þ M CM M K (18) whr t[[,t ] kb(t)k (t)k M 1, t[[,t ] k[d(b(t)k (t))=dt] km 2, and M E, M, M C, MX, M K, r ar dfind as in Thorm 1. Multiplying (17) and (18) by 2lt, rspctivly, whr l. L f,whav kx kþ1 ðþ x t k ðþk t l L f þ M 1 k k ðþk t l þ M 2 t[ ½,T t[ ½,T lt kx kþ1 ðþ x t k ðþkdt t lt k k ðþkdt t þ M E M X þ M M K (19) k kþ1 ðþk t l r k k ðþk t l þ M C L f lt kx kþ1 ðþ x t k ðþkdt t t[ ½,T t[ ½,T lt k k ðþkdt t þ M C M E MX þ M C M 2 þ M C M M K (2) Applying (9) of Lmma 1 to (19) and (2), w can obtain th following inquality kx kþ1 ðþ x t k t ðþk l lm 1 þ M 2 þ lm EM X k k ðþk t l k kþ1 (t)k l r þ M CM 2 k l k (t)k l þ M CL f l Substituting (21) into (22), w obtain k kþ1 (t)k l rk k (t)k l þ lm CM E M X kx kþ1 (t) x k (t)k l þ lm M K (21) þ M C M E M X þ M CM M K (22) þ lm CM M K (23) whr rr þ(m C M 2 =l)þ(m C L f (M 1 þ(m 2 =l))=(l L f )). Whn r, 1, w can slct l to b sufficintly larg such that r, 1. Equation (23) is a contraction, thrfor lim k k (t)k l lm C(M E MX þ M MK ) k!1 (1 r)( ) (24) On th othr hand, from th dfinition of th l-norm, lim k!1 k k (t)k l j t[[h,t ] lim k!1 k k (t)k l. Considring (24), w hav lim k k (t)k l j t[[h,t ] lm C(M E MX þ M MK ) k!1 (1 r)( ) (25) Furthrmor, if th input matrix B(t) at t [ [, h] is accuratly known, w hav M E M. It can b dirctly drivd from (25) that lim k!1 k k (t)k l j t[[h,t ]. From th abov dduction, it is important to not that (25) is obtaind from th invstigation of systm (15) and (16) on th tim intrval t [ [, T ]. Systm (15) and (16) is not quivalnt to th original systm (12) and (14) at t [ [, T ], but thy ar quivalnt on th tim intrval t [ [h, T ]. Thy should xhibit th sam proprtis at t [ [h, T ]. Thrfor (25) is also suitabl to systm (12) and (14) at t [ [h, T ]. Thorm 1 is provd. A 52 IET Control Thory Appl., 29, Vol. 3, No. 1, pp & Th Institution of Enginring and Tchnology 29 doi: 1.149/it-cta:27486

5 Rmark 1: Equation (25) shows that th ILC rul (5) is abl to driv th ILC rror at t [ [h, T ] into a bound. But, it is worth noting that aftr th paramtr l is slctd, th bound is mainly dcidd by paramtrs M E and M, which ar rlatd to th stimation rror with rspct to th input matrix B(t). Thrfor compard with th robust ffct of th D-typ ILC rul (4), th bound can b controlld to a much smallr lvl whn B(t) is wll stimatd. This point will b bttr illustratd by th xampl prsntd in th nxt sction. Rmark 2: From th ILC rul (5) and th dfinition (6) of u h (t), it is shown that th ILC rul (5) puts an initial rctifying action on a small initial tim intrval [, h] and pursus th rfrnc trajctory tracking at t [ [h, T ]. Th function u h (t) spcifis th initial rctifying action on [, h]. A lss valu h in u h (t) may rsult in a largr control input. Thus, th slction of h should b don basd on th trad-off btwn th rsulting control input and th tracking rror. In addition, Thorm 1 rquirs that th input matrix B(t) is right invrtibl and stimabl. But th corrsponding tim intrval is only a small initial tim intrval [, h], not th ntir tim intrval [, T]. Also, in ordr to achiv prfct tracking at t [ [h, T ] namly lim k!1 k k (t)k l j t[[h,t ], w nd th input matrix, B(t), to b accuratly known on th initial tim intrval [, h] only. Rmark 3: Rgarding th slction of th larning gain matrix K(t) in th ILC rul (5), Thorm 1 givs us a thortical guidlin that K(t) should satisfy (1). In particular, lt K (t) a( ^C(t) ^B(t)) T [ ^C(t) ^B(t)( ^C(t) ^B(t)) T ] 1 if ^C(t) ^B(t) is of full-row rank, whr ^C(t) and ^B(t) ar stimations to C(t) and B(t), rspctivly. W can find a [ (1, 2 1) and 1 [ (, 1) so that t[[,t ] ki C(t)B(t)K (t)k r, 1. 4 Illustrativ xampl Considr an ILC problm of th following NCM systm d x (1) :5 sin x (1) þ :8 cos x (2) >< dt x (2) 4 5 þ Bt ðþu sin x (1) x (2) >: y Ct ðþ x (1) x (2) (26) 2:5 sin(1t) whr Bt ðþ, C(t) :5t þ : :3t Th dsird output y r (t) is dscribd by th quation y r (t) 15(t t 2 ), t [ [, 1] (27) In ordr to vrify our ILC approach for NCM systms with non-fixd initial rrors, w randomis th initial stats of systm (26) x (1) () and x (2) (), which vary btwn 21 and 1 at diffrnt itrations of ILC procss randomly, as shown in Tabl 1. Th inducd non-fixd initial ILC rrors, k (), ar also listd in Tabl 1. Suppos that th accurat information on paramtrs B(t) and C(t) in systm (26) is unavailabl, and only thir 2:3 :7 sin(1t) stimation ^B(t) and ^C(t) ar givn as :15 1:2 :45t and :6t þ :15 1:2, rspctivly. In th ILC procss of systm (26), w st th initial input of ILC as u (t), t [ [, 1], and h.5. W pursu th tracking of th dsird output y r (t) on th intrval t [ [:5, 1]. Th accuracy of tracking is valuatd by th following maximum absolut rror of tracking EE jy r (t) y(t)j t[[h,1] To bttr illustrat th initial rctifying action of our Tabl 1 Non-fixd initial stats and initial rrors of ILC tracking prformanc at diffrnt itrations k x k () :36 :59 :42 :17 :31 :93 :73 :13 :41 :77 :81 :4 :84 :54 :75 :42 k () k x k () :38 :93 :6 :83 :71 :8 :27 :23 :84 :67 :33 :21 :15 :52 :78 :82 k () IET Control Thory Appl., 29, Vol. 3, No. 1, pp doi: 1.149/it-cta:27486 & Th Institution of Enginring and Tchnology 29

6 Figur 1 Maximum absolut rror of tracking on th intrval t [[.5, 1] at diffrnt itration numbrs using th D-typ ILC rul (4) proposd ILC rul (5) by comparison, first, a D-typ ILC rul (4) without a rctifying action is usd. W st K (t) :6( ^C(t) ^B(t)) T [ ^C(t) ^B(t)( ^C(t) ^B(t)) T ] 1, which maks max t[[,1] ki C(t)B(t)K (t)k, 1. Fig. 1 prsnts th situation of th tracking rror indx EE on th intrval t [ [:5, 1] whn th D-typ ILC rul (4) is xcutd at diffrnt itration numbrs. In Fig. 1, it is shown that th ILC rul (4) is abl to driv th ILC rror into a bound. Th robustnss of th ILC rul (4) to non-fixd initial ILC rrors is thus illustratd. But it is also noticd that th bound is surly too larg for practical application. Nxt, th abov ILC rul (5), which includs an initial rctifying action, is applid. Fig. 2 shows how th tracking rror indx EE on th intrval t [ [:5, 1] varis at diffrnt numbrs of itration. Compard with th rsults shown in Fig. 1, th ILC tracking rror is boundd to a much lowr lvl. Figur 3 Tracking prformanc of th ILC systm outputs on th intrval t [[, 1] at diffrnt itration numbrs using th ILC rul (5) with th known B(t) (Th dottd, dashd dottd and dashd lins rprsnt th systm outputs as th ILC rul (5) is itrativly xcutd two, thr and four tims, rspctivly, and th solid lin rprsnts th dsird output) Finally, givn that th input matrix B(t) is accuratly known on th initial tim intrval [,.5], and th ILC rul (5) is usd, Fig. 3 shows th tracking prformanc of th ILC systm output on th intrval t [ [, 1] whn th ILC rul (5) is itrativly xcutd from th scond to th forth tim. Also, Fig. 4 prsnts th situation of th tracking rror indx EE on th intrval t [ [:5, 1] whn th ILC rul (5) is xcutd at diffrnt itration numbrs. In Fig. 4, it is noticd that th ILC tracking rror on th intrval t [ [:5, 1] can b surly drivn to zro by th ILC rul (5) with th known B(t). A prfct tracking of th dsird output y r (t) on th intrval t [ [:5, 1] is achivd. Th xampl usd in this papr illustrats that th proposd ILC approach for NCM systms with non-fixd Figur 2 Maximum absolut rror of tracking on th intrval t [[.5, 1] at diffrnt itration numbr using th ILC rul (5) Figur 4 Maximum absolut rror of tracking on th intrval t [[.5, 1] at diffrnt itration numbrs using th ILC rul (5) with th known B(t) 54 IET Control Thory Appl., 29, Vol. 3, No. 1, pp & Th Institution of Enginring and Tchnology 29 doi: 1.149/it-cta:27486

7 initial rrors is vry ffctiv. It can ovrcom random initial rrors of ILC systms and can succssfully track th dsird output trajctory byond a small initial tim intrval aftr a small numbr of itrations. 5 Conclusion This papr introducs an initial rctifying action into th convntional D-typ ILC mthod for NCM systms. Th stablishd ILC tchniqu allows th initial output of th ILC systm at diffrnt itrations fluctuating randomly around th initial valu of th dsird output. Th usd ILC stratgy is to st a vry small initial tim intrval and to pursu th rfrnc trajctory tracking byond th initial tim intrval. Th output tracking rror byond th initial tim intrval can b drivn to a rsidual st whos siz dpnds on th stimation rror of input matrix. It is worth noting that whn an accurat knowldg on th input matrix on th initial tim intrval is availabl, a prfct rfrnc trajctory tracking byond th initial tim intrval can vn b achivd. Compard with th convntional ILC mthods, th robustnss of th proposd ILC systm is gratly improvd. 6 Acknowldgmnt This work is portd in part by th National Natural Scinc Foundation of China undr Grant , and in part by th Rsarch Grants Council of th Hong Kong Spcial Administrativ Rgion, China undr Projct No. 8734/CityU. 7 Rfrncs [1] KUREK J.E., ZAREMBA M.B.: Itrativ larning control synthsis basd on 2-D systm thory, IEEE Trans. Autom. Control, 1993, 38, pp [2] LI X.-D., HO J.K.L., CHOW T.W.S.: Itrativ larning control for linar tim-variant discrt systms basd on 2-D systm thory, IEE Proc. Control Thory Appl., 25, 152, (1), pp [3] CHIEN C.J.: A discrt itrativ larning control for a class of nonlinar tim-varying systms, IEEE Trans. Autom. Control, 1998, 43, pp [4] HUANG S.N., TAN K.K., LEE T.H.: Ncssary and sufficint condition for convrgnc of itrativ larning algorithm, Automatica, 22, 38, pp [5] LI X.-D., CHOW T.W.S., HO J.K.L.: 2-D systm thory basd itrativ larning control for linar continuous systms with tim-dlays, IEEE Trans. Circuit Syst., I, 25, 52, (7), pp [6] JIANG P., CHEN H., BAMFORTH L.C.A.: A univrsal itrativ larning stabilizr for a class of MIMO systms, Automatica, 26, 42, pp [7] LEE H.S., BIEN Z.: Initial condition problm of larning control, IEE Proc.-D, 1991, 138, pp [8] ARIMOTO S.: Robustnss of larning control for robot manipulators, Proc. IEEE Int. Conf. Robot. Autom., 199, 3, pp [9] HEINZINGER G., FENWICK D., PADEN B., MIYAZAKI F.: Stability of larning control with disturbancs and uncrtain initial conditions, IEEE Trans. Autom. Control, 1992, 37, pp [1] WANG D.: Convrgnc and robustnss of discrt tim nonlinar systms with itrativ larning control, Automatica, 1998, 34, (11), pp [11] SUN M., WANG D.: Itrativ larning control with initial rctifying action, Automatica, 22, 38, (7), pp [12] SUN M., WANG D.: Initial condition issus on itrativ larning control for non-linar systms with tim dlay, Int. J. Syst. Sci., 21, 32, (11), pp [13] LEE H.S., BIEN Z.: Study on robustnss of itrativ larning control with non-zro initial rror, Int. J. Control, 1996, 64, (3), pp [14] PARK K.-H.: An avrag oprator-basd PD-typ itrativ larning control for variabl initial stat rror, IEEE Trans. Autom. Control, 25, 5, (6), pp [15] XU J.-X., YAN R.: On initial conditions in itrativ larning control, IEEE Trans. Autom. Control, 25, 5, (9), pp [16] WANG Y.-C., CHIEN C.-J., TENG C.-C.: Dirct adaptiv itrativ larning control of nonlinar systms using an output-rcurrnt fuzzy nural ntwork, IEEE Trans. Syst., Man, Cybrn. B, Cybrn., 24, 34, (3), pp [17] FANG Y., CHOW T.W.S.: 2-D analysis for itrativ larning controllr for discrt-tim systms with variabl initial conditions, IEEE Trans. Circuit Syst., I: Fundamntal Thory Appl., 23, 5, (5), pp [18] QIAN W., PANDA S.K., XU J.-X.: Spd rippl minimization in PM synchronous motor using itrativ larning control, IEEE Trans. Enrgy Convrs., 25, 2, (1), pp IET Control Thory Appl., 29, Vol. 3, No. 1, pp doi: 1.149/it-cta:27486 & Th Institution of Enginring and Tchnology 29

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

Two Products Manufacturer s Production Decisions with Carbon Constraint

Two Products Manufacturer s Production Decisions with Carbon Constraint Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint

More information

Sliding Mode Flow Rate Observer Design

Sliding Mode Flow Rate Observer Design Sliding Mod Flow Rat Obsrvr Dsign Song Liu and Bin Yao School of Mchanical Enginring, Purdu Univrsity, Wst Lafaytt, IN797, USA liu(byao)@purdudu Abstract Dynamic flow rat information is ndd in a lot of

More information

10. The Discrete-Time Fourier Transform (DTFT)

10. The Discrete-Time Fourier Transform (DTFT) Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w

More information

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero. SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain

More information

Derangements and Applications

Derangements and Applications 2 3 47 6 23 Journal of Intgr Squncs, Vol. 6 (2003), Articl 03..2 Drangmnts and Applications Mhdi Hassani Dpartmnt of Mathmatics Institut for Advancd Studis in Basic Scincs Zanjan, Iran mhassani@iasbs.ac.ir

More information

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

ECE602 Exam 1 April 5, You must show ALL of your work for full credit. ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b

More information

Application of Vague Soft Sets in students evaluation

Application of Vague Soft Sets in students evaluation Availabl onlin at www.plagiarsarchlibrary.com Advancs in Applid Scinc Rsarch, 0, (6):48-43 ISSN: 0976-860 CODEN (USA): AASRFC Application of Vagu Soft Sts in studnts valuation B. Chtia*and P. K. Das Dpartmnt

More information

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL

More information

Numerical considerations regarding the simulation of an aircraft in the approaching phase for landing

Numerical considerations regarding the simulation of an aircraft in the approaching phase for landing INCAS BULLETIN, Volum, Numbr 1/ 1 Numrical considrations rgarding th simulation of an aircraft in th approaching phas for landing Ionl Cristinl IORGA ionliorga@yahoo.com Univrsity of Craiova, Alxandru

More information

Basic Polyhedral theory

Basic Polyhedral theory Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist

More information

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a 204 Intrnational Confrnc on Computr Scinc and Elctronic Tchnology (ICCSET 204) Rotor Stationary Control Analysis Basd on Coupling KdV Equation Finit Stady Analysis Liu Dalong,a, Xu Lijuan2,a Dpartmnt of

More information

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction Int. J. Opn Problms Compt. Math., Vol., o., Jun 008 A Pry-Prdator Modl with an Altrnativ Food for th Prdator, Harvsting of Both th Spcis and with A Gstation Priod for Intraction K. L. arayan and. CH. P.

More information

Supplementary Materials

Supplementary Materials 6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

More information

2.3 Matrix Formulation

2.3 Matrix Formulation 23 Matrix Formulation 43 A mor complicatd xampl ariss for a nonlinar systm of diffrntial quations Considr th following xampl Exampl 23 x y + x( x 2 y 2 y x + y( x 2 y 2 (233 Transforming to polar coordinats,

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Construction of asymmetric orthogonal arrays of strength three via a replacement method isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy

More information

1 Minimum Cut Problem

1 Minimum Cut Problem CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical

More information

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK Data Assimilation 1 Alan O Nill National Cntr for Earth Obsrvation UK Plan Motivation & basic idas Univariat (scalar) data assimilation Multivariat (vctor) data assimilation 3d-Variational Mthod (& optimal

More information

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018 Propositional Logic Combinatorial Problm Solving (CPS) Albrt Olivras Enric Rodríguz-Carbonll May 17, 2018 Ovrviw of th sssion Dfinition of Propositional Logic Gnral Concpts in Logic Rduction to SAT CNFs

More information

General Notes About 2007 AP Physics Scoring Guidelines

General Notes About 2007 AP Physics Scoring Guidelines AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation

More information

u 3 = u 3 (x 1, x 2, x 3 )

u 3 = u 3 (x 1, x 2, x 3 ) Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.

More information

GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia

GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES Eduard N. Klnov* Rostov-on-Don, Russia Th articl considrs phnomnal gomtry figurs bing th carrirs of valu spctra for th pairs of th rmaining additiv

More information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

Model-based Scheduling for Networked Control Systems

Model-based Scheduling for Networked Control Systems Modl-basd Schduling for Ntworkd Control Systms Han Yu, Eloy Garcia and Panos J. Antsaklis Abstract In this papr, w introduc a modl-basd schduling stratgy to achiv ultimat bounddnss stability in th snsor-actuator

More information

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH. C:\Dallas\0_Courss\03A_OpSci_67\0 Cgh_Book\0_athmaticalPrliminaris\0_0 Combath.doc of 8 COPUTER GENERATED HOLOGRAS Optical Scincs 67 W.J. Dallas (onday, April 04, 005, 8:35 A) PART I: CHAPTER TWO COB ATH

More information

Cramér-Rao Inequality: Let f(x; θ) be a probability density function with continuous parameter

Cramér-Rao Inequality: Let f(x; θ) be a probability density function with continuous parameter WHEN THE CRAMÉR-RAO INEQUALITY PROVIDES NO INFORMATION STEVEN J. MILLER Abstract. W invstigat a on-paramtr family of probability dnsitis (rlatd to th Parto distribution, which dscribs many natural phnomna)

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information

Computing and Communications -- Network Coding

Computing and Communications -- Network Coding 89 90 98 00 Computing and Communications -- Ntwork Coding Dr. Zhiyong Chn Institut of Wirlss Communications Tchnology Shanghai Jiao Tong Univrsity China Lctur 5- Nov. 05 0 Classical Information Thory Sourc

More information

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is Procdings of IC-IDC0 EFFECTS OF STOCHASTIC PHASE SPECTRUM DIFFERECES O PHASE-OLY CORRELATIO FUCTIOS PART I: STATISTICALLY COSTAT PHASE SPECTRUM DIFFERECES FOR FREQUECY IDICES Shunsu Yamai, Jun Odagiri,

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

More information

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

More information

Another view for a posteriori error estimates for variational inequalities of the second kind

Another view for a posteriori error estimates for variational inequalities of the second kind Accptd by Applid Numrical Mathmatics in July 2013 Anothr viw for a postriori rror stimats for variational inqualitis of th scond kind Fi Wang 1 and Wimin Han 2 Abstract. In this papr, w giv anothr viw

More information

Lecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac.

Lecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac. Lctur 2: Discrt-Tim Signals & Systms Rza Mohammadkhani, Digital Signal Procssing, 2015 Univrsity of Kurdistan ng.uok.ac.ir/mohammadkhani 1 Signal Dfinition and Exampls 2 Signal: any physical quantity that

More information

Higher order derivatives

Higher order derivatives Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of

More information

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002 3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or

More information

What are those βs anyway? Understanding Design Matrix & Odds ratios

What are those βs anyway? Understanding Design Matrix & Odds ratios Ral paramtr stimat WILD 750 - Wildlif Population Analysis of 6 What ar thos βs anyway? Undrsting Dsign Matrix & Odds ratios Rfrncs Hosmr D.W.. Lmshow. 000. Applid logistic rgrssion. John Wily & ons Inc.

More information

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation. Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform

More information

On spanning trees and cycles of multicolored point sets with few intersections

On spanning trees and cycles of multicolored point sets with few intersections On spanning trs and cycls of multicolord point sts with fw intrsctions M. Kano, C. Mrino, and J. Urrutia April, 00 Abstract Lt P 1,..., P k b a collction of disjoint point sts in R in gnral position. W

More information

Limiting value of higher Mahler measure

Limiting value of higher Mahler measure Limiting valu of highr Mahlr masur Arunabha Biswas a, Chris Monico a, a Dpartmnt of Mathmatics & Statistics, Txas Tch Univrsity, Lubbock, TX 7949, USA Abstract W considr th k-highr Mahlr masur m k P )

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals

More information

10. Limits involving infinity

10. Limits involving infinity . Limits involving infinity It is known from th it ruls for fundamntal arithmtic oprations (+,-,, ) that if two functions hav finit its at a (finit or infinit) point, that is, thy ar convrgnt, th it of

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

Estimation of apparent fraction defective: A mathematical approach

Estimation of apparent fraction defective: A mathematical approach Availabl onlin at www.plagiarsarchlibrary.com Plagia Rsarch Library Advancs in Applid Scinc Rsarch, 011, (): 84-89 ISSN: 0976-8610 CODEN (USA): AASRFC Estimation of apparnt fraction dfctiv: A mathmatical

More information

On the Hamiltonian of a Multi-Electron Atom

On the Hamiltonian of a Multi-Electron Atom On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making

More information

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN Intrnational Journal of Scintific & Enginring Rsarch, Volum 6, Issu 7, July-25 64 ISSN 2229-558 HARATERISTIS OF EDGE UTSET MATRIX OF PETERSON GRAPH WITH ALGEBRAI GRAPH THEORY Dr. G. Nirmala M. Murugan

More information

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full

More information

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim. MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function

More information

Symmetric centrosymmetric matrix vector multiplication

Symmetric centrosymmetric matrix vector multiplication Linar Algbra and its Applications 320 (2000) 193 198 www.lsvir.com/locat/laa Symmtric cntrosymmtric matrix vctor multiplication A. Mlman 1 Dpartmnt of Mathmatics, Univrsity of San Francisco, San Francisco,

More information

On the irreducibility of some polynomials in two variables

On the irreducibility of some polynomials in two variables ACTA ARITHMETICA LXXXII.3 (1997) On th irrducibility of som polynomials in two variabls by B. Brindza and Á. Pintér (Dbrcn) To th mmory of Paul Erdős Lt f(x) and g(y ) b polynomials with intgral cofficints

More information

Gradient-based step response identification of low-order model for time delay systems Rui Yan, Fengwei Chen, Shijian Dong, Tao Liu*

Gradient-based step response identification of low-order model for time delay systems Rui Yan, Fengwei Chen, Shijian Dong, Tao Liu* Gradint-basd stp rspons idntification of low-ordr modl for tim dlay systms Rui Yan, Fngwi Chn, Shijian Dong, ao Liu* Institut of Advancd Control chnology, Dalian Univrsity of chnology, Dalian, 64, P R

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance TECHNICAL NTE 30 Dsign Guidlins for Quartz Crystal scillators Introduction A CMS Pirc oscillator circuit is wll known and is widly usd for its xcllnt frquncy stability and th wid rang of frquncis ovr which

More information

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

First derivative analysis

First derivative analysis Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points

More information

Chapter 6. The Discrete Fourier Transform and The Fast Fourier Transform

Chapter 6. The Discrete Fourier Transform and The Fast Fourier Transform Pusan ational Univrsity Chaptr 6. Th Discrt Fourir Transform and Th Fast Fourir Transform 6. Introduction Frquncy rsponss of discrt linar tim invariant systms ar rprsntd by Fourir transform or z-transforms.

More information

Approximation and Inapproximation for The Influence Maximization Problem in Social Networks under Deterministic Linear Threshold Model

Approximation and Inapproximation for The Influence Maximization Problem in Social Networks under Deterministic Linear Threshold Model 20 3st Intrnational Confrnc on Distributd Computing Systms Workshops Approximation and Inapproximation for Th Influnc Maximization Problm in Social Ntworks undr Dtrministic Linar Thrshold Modl Zaixin Lu,

More information

CS 361 Meeting 12 10/3/18

CS 361 Meeting 12 10/3/18 CS 36 Mting 2 /3/8 Announcmnts. Homwork 4 is du Friday. If Friday is Mountain Day, homwork should b turnd in at my offic or th dpartmnt offic bfor 4. 2. Homwork 5 will b availabl ovr th wknd. 3. Our midtrm

More information

ABEL TYPE THEOREMS FOR THE WAVELET TRANSFORM THROUGH THE QUASIASYMPTOTIC BOUNDEDNESS

ABEL TYPE THEOREMS FOR THE WAVELET TRANSFORM THROUGH THE QUASIASYMPTOTIC BOUNDEDNESS Novi Sad J. Math. Vol. 45, No. 1, 2015, 201-206 ABEL TYPE THEOREMS FOR THE WAVELET TRANSFORM THROUGH THE QUASIASYMPTOTIC BOUNDEDNESS Mirjana Vuković 1 and Ivana Zubac 2 Ddicatd to Acadmician Bogoljub Stanković

More information

ON A SECOND ORDER RATIONAL DIFFERENCE EQUATION

ON A SECOND ORDER RATIONAL DIFFERENCE EQUATION Hacttp Journal of Mathmatics and Statistics Volum 41(6) (2012), 867 874 ON A SECOND ORDER RATIONAL DIFFERENCE EQUATION Nourssadat Touafk Rcivd 06:07:2011 : Accptd 26:12:2011 Abstract In this papr, w invstigat

More information

MA 262, Spring 2018, Final exam Version 01 (Green)

MA 262, Spring 2018, Final exam Version 01 (Green) MA 262, Spring 218, Final xam Vrsion 1 (Grn) INSTRUCTIONS 1. Switch off your phon upon ntring th xam room. 2. Do not opn th xam booklt until you ar instructd to do so. 3. Bfor you opn th booklt, fill in

More information

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS Stig Holst ABB Automation Products Swdn Bapuji S Palki ABB Utilitis India This papr rports

More information

Where k is either given or determined from the data and c is an arbitrary constant.

Where k is either given or determined from the data and c is an arbitrary constant. Exponntial growth and dcay applications W wish to solv an quation that has a drivativ. dy ky k > dx This quation says that th rat of chang of th function is proportional to th function. Th solution is

More information

Recursive Estimation of Dynamic Time-Varying Demand Models

Recursive Estimation of Dynamic Time-Varying Demand Models Intrnational Confrnc on Computr Systms and chnologis - CompSysch 06 Rcursiv Estimation of Dynamic im-varying Dmand Modls Alxandr Efrmov Abstract: h papr prsnts an implmntation of a st of rcursiv algorithms

More information

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming CPSC 665 : An Algorithmist s Toolkit Lctur 4 : 21 Jan 2015 Lcturr: Sushant Sachdva Linar Programming Scrib: Rasmus Kyng 1. Introduction An optimization problm rquirs us to find th minimum or maximum) of

More information

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation Diffrnc -Analytical Mthod of Th On-Dimnsional Convction-Diffusion Equation Dalabav Umurdin Dpartmnt mathmatic modlling, Univrsity of orld Economy and Diplomacy, Uzbistan Abstract. An analytical diffrncing

More information

Rational Approximation for the one-dimensional Bratu Equation

Rational Approximation for the one-dimensional Bratu Equation Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in

More information

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim (implicit in notation and n a positiv intgr, lt ν(n dnot th xponnt of p in n, and U(n n/p ν(n, th unit

More information

cycle that does not cross any edges (including its own), then it has at least

cycle that does not cross any edges (including its own), then it has at least W prov th following thorm: Thorm If a K n is drawn in th plan in such a way that it has a hamiltonian cycl that dos not cross any dgs (including its own, thn it has at last n ( 4 48 π + O(n crossings Th

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

More information

PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS

PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS 1 Dharmndra

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

More information

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values Dnamic Macroconomic Thor Prof. Thomas Lux Bifurcation Thor Bifurcation: qualitativ chang in th natur of th solution occurs if a paramtr passs through a critical point bifurcation or branch valu. Local

More information

5.80 Small-Molecule Spectroscopy and Dynamics

5.80 Small-Molecule Spectroscopy and Dynamics MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts

More information

Problem Set 6 Solutions

Problem Set 6 Solutions 6.04/18.06J Mathmatics for Computr Scinc March 15, 005 Srini Dvadas and Eric Lhman Problm St 6 Solutions Du: Monday, March 8 at 9 PM in Room 3-044 Problm 1. Sammy th Shark is a financial srvic providr

More information

REPRESENTATIONS OF LIE GROUPS AND LIE ALGEBRAS

REPRESENTATIONS OF LIE GROUPS AND LIE ALGEBRAS REPRESENTATIONS OF LIE GROUPS AND LIE ALGEBRAS JIAQI JIANG Abstract. This papr studis th rlationship btwn rprsntations of a Li group and rprsntations of its Li algbra. W will mak th corrspondnc in two

More information

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1 F110 Spktrala transformr för Mdia Solutions to Stiglitz, Chaptr 1 Prfac This documnt contains solutions to slctd problms from Kn Stiglitz s book: A Digital Signal Procssing Primr publishd by Addison-Wsly.

More information

Mutually Independent Hamiltonian Cycles of Pancake Networks

Mutually Independent Hamiltonian Cycles of Pancake Networks Mutually Indpndnt Hamiltonian Cycls of Pancak Ntworks Chng-Kuan Lin Dpartmnt of Mathmatics National Cntral Univrsity, Chung-Li, Taiwan 00, R O C discipl@ms0urlcomtw Hua-Min Huang Dpartmnt of Mathmatics

More information

Estimation of odds ratios in Logistic Regression models under different parameterizations and Design matrices

Estimation of odds ratios in Logistic Regression models under different parameterizations and Design matrices Advancs in Computational Intllignc, Man-Machin Systms and Cybrntics Estimation of odds ratios in Logistic Rgrssion modls undr diffrnt paramtrizations and Dsign matrics SURENDRA PRASAD SINHA*, LUIS NAVA

More information

Abstract Interpretation: concrete and abstract semantics

Abstract Interpretation: concrete and abstract semantics Abstract Intrprtation: concrt and abstract smantics Concrt smantics W considr a vry tiny languag that manags arithmtic oprations on intgrs valus. Th (concrt) smantics of th languags cab b dfind by th funzcion

More information

3-2-1 ANN Architecture

3-2-1 ANN Architecture ARTIFICIAL NEURAL NETWORKS (ANNs) Profssor Tom Fomby Dpartmnt of Economics Soutrn Mtodist Univrsity Marc 008 Artificial Nural Ntworks (raftr ANNs) can b usd for itr prdiction or classification problms.

More information

1973 AP Calculus AB: Section I

1973 AP Calculus AB: Section I 97 AP Calculus AB: Sction I 9 Minuts No Calculator Not: In this amination, ln dnots th natural logarithm of (that is, logarithm to th bas ).. ( ) d= + C 6 + C + C + C + C. If f ( ) = + + + and ( ), g=

More information

Deift/Zhou Steepest descent, Part I

Deift/Zhou Steepest descent, Part I Lctur 9 Dift/Zhou Stpst dscnt, Part I W now focus on th cas of orthogonal polynomials for th wight w(x) = NV (x), V (x) = t x2 2 + x4 4. Sinc th wight dpnds on th paramtr N N w will writ π n,n, a n,n,

More information

Anti-Synchronization of Tigan and Li Systems with Unknown Parameters via Adaptive Control

Anti-Synchronization of Tigan and Li Systems with Unknown Parameters via Adaptive Control An Intrnational Journal of Optimization and Control: Thoris & Applications Vol., No.1, pp.17-8 (01) IJOCTA ISSN: 146-0957 ISSN: 146-570 http://www.ijocta.com Anti-Synchronization of Tigan and Li Systms

More information

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark Answr omwork 5 PA527 Fall 999 Jff Stark A patint is bing tratd with Drug X in a clinical stting. Upon admiion, an IV bolus dos of 000mg was givn which yildd an initial concntration of 5.56 µg/ml. A fw

More information

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C Tchniqus of Intgration c Donald Kridr and Dwight Lahr In this sction w ar going to introduc th first approachs to valuating an indfinit intgral whos intgrand dos not hav an immdiat antidrivativ. W bgin

More information

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013 18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:

More information

Full Order Observer Controller Design for Two Interacting Tank System Based on State Space Approach

Full Order Observer Controller Design for Two Interacting Tank System Based on State Space Approach Intrnational Journal of Application or Innovation in Enginring & Managmnt (IJAIEM) Wb Sit: www.ijaim.org Email: ditor@ijaim.org Volum 6, Issu 7, July 07 ISSN 39-4847 Full Ordr Obsrvr Controllr Dsign for

More information

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1 Chaptr 11 Th singular sris Rcall that by Thorms 10 and 104 togthr provid us th stimat 9 4 n 2 111 Rn = SnΓ 2 + on2, whr th singular sris Sn was dfind in Chaptr 10 as Sn = q=1 Sq q 9, with Sq = 1 a q gcda,q=1

More information

Learning Spherical Convolution for Fast Features from 360 Imagery

Learning Spherical Convolution for Fast Features from 360 Imagery Larning Sphrical Convolution for Fast Faturs from 36 Imagry Anonymous Author(s) 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 3 3 33 34 35 In this fil w provid additional dtails to supplmnt th main papr

More information

Scattering States of l-wave Schrödinger Equation with Modified Rosen Morse Potential

Scattering States of l-wave Schrödinger Equation with Modified Rosen Morse Potential Commun. Thor. Phys. 66 06 96 00 Vol. 66, No., August, 06 Scattring Stats of l-wav Schrödingr Equation with Modifid Rosn Mors Potntial Wn-Li Chn í,, Yan-Wi Shi á, and Gao-Fng Wi Ôô, Gnral Education Cntr,

More information

Exponential inequalities and the law of the iterated logarithm in the unbounded forecasting game

Exponential inequalities and the law of the iterated logarithm in the unbounded forecasting game Ann Inst Stat Math (01 64:615 63 DOI 101007/s10463-010-03-5 Exponntial inqualitis and th law of th itratd logarithm in th unboundd forcasting gam Shin-ichiro Takazawa Rcivd: 14 Dcmbr 009 / Rvisd: 5 Octobr

More information