x_ x_1

Size: px
Start display at page:

Download "x_ x_1"

Transcription

1 Control Lyapnov Fnctons: New Ideas From an Old Sorce Randy A. Freeman Department of Electrcal and Compter Engneerng Nortwestern Unversty, Tecnologcal Insttte 5 Serdan Road, Evanston, IL freeman@ece.nw.ed James A. Prmbs Control and Dynamcal Systems Calforna Insttte of Tecnology Pasadena, Calforna 95 jprmbs@ot.caltec.ed Abstract A control desgn metod for nonlnear systems based on control Lyapnov fnctons and nverse optmalty s analyzed. Ts metod s sown to recover te LQ optmal control wen appled to lnear systems. More generally, t s sown to recover te optmal control wenever te level sets of te control Lyapnov fncton matc tose of te optmal vale fncton. Te metod can be readly appled to feedback lnearzable systems, and te resltng nverse optmal control law s generally mc derent from te lnearzng control law. Examples n two dmensons are gven to llstrate bot te strengts and te weaknesses of te metod. Control Lyapnov fnctons We consder sngle-npt, control-ane nonlnear systems of te form _x = f(x) + g(x) () were x IR n s te state vector, IR s te control npt, and f and g are known contnos fnctons. Or goal s to constrct a contnos state feedback law = k(x) sc tat x = s a globally asymptotcally stable eqlbrm pont of te resltng closedloop system. Or control desgn wll be based on knowledge of a control Lyapnov fncton (clf), tat s, a C, proper, postve dente fncton V : IR n! IR + sc tat nf L f V (x) + L g V (x) < () for all x 6= [, ]. Te exstence of a clf for te system () s eqvalent to te exstence of a globally asymptotcally stablzng control law = k(x) wc s smoot everywere except possbly at x = []. Moreover, one can calclate sc a control law k explctly from f, g, and V [3]. We wll say tat V as above s a weak clf wen te neqalty () s non-strct, namely, wen nf L f V (x) + L g V (x) (3) for all x. Te exstence of a weak clf does not garantee global stablzablty as does te exstence of a clf. Neverteless, n many cases a weak clf can ndeed be sed to desgn a globally stablzng control law as we wll see n Secton below. Gven a general system of te form (), t may be df- clt to nd a clf or even to determne weter or not one exsts. Fortnately, tere are sgncant classes of systems for wc te systematc constrcton of a clf s possble. As we wll see n Secton 3, tese nclde te class of (globally) feedback lnearzable systems. Inverse optmalty Once we ave fond a clf V, we can constrct a control law = k(x) sc tat te Lyapnov dervatve V _ s negatve at every pont n te state space. To prevent orselves from makng absrd coces n ts constrcton, we wll nsst tat te control law k be optmal wt respect to some meanngfl cost fnctonal. A meanngfl cost fnctonal s one tat places stable penalty on bot te state varable x and te control varable so tat seless conclsons lke \every stablzng control law s optmal" are avoded. Te problem of assocatng some cost fnctonal wt a control law k or a clf V s known as an nverse optmal control problem [, 5, 6, 7, 8, 9,,,, 3,, 5]. As sown n [5], every clf V s te vale fncton for some meanngfl cost fnctonal. In oter words, every clf solves te Hamlton-Jacob-Bellman (HJB) eqaton assocated wt a meanngfl cost. Moreover, one can compte te resltng (nverse) optmal control law k drectly from V, f, and g wtot recorse to te HJB eqaton. Unfortnately, te constrcton of an nverse optmal control law k s not nqe becase V may be te vale fncton for many derent cost fnctonals, eac of wc may ave a derent optmal control. Neverteless, te nverse optmal constrcton can be sed to narrow down te coces for k to tose wc satsfy an optmalty crteron. One metod for generatng an nverse optmal control law k gven a clf V s trog te pontwse mnmzaton of control eort. It s sown n [5] tat control

2 laws of te form n o k(x) = arg mn jj : L f V(x)+L g V(x)?(x) () are nverse optmal, were (x) s cosen to be contnos, postve dente, and sc tat L f V (x)?(x) wenever L g V (x) =. Ts desgn \parameter" represents te desred amont of negatvty of te closedloop Lyapnov dervatve _ V, and derent coces for reslt n derent nverse optmal control laws k. Te contnty of te control law gven by te formla () depends on te coce for (x). If s cosen so tat te strct neqalty L f V (x) <?(x) olds wenever L g V (x) = and x 6=, ten k wll be contnos except possbly at x = [5]. A coce for resltng n a non-strct neqalty cold lead to a dscontnos control law k, so sc fnctons sold be cosen wt care. Also, n some cases we may want to consder a postve semdente, especally wen V s only a weak clf. We wll now specfy a partclarly nterestng coce for (x). Sppose tat we ws to mnmze a cost fnctonal of te form Z J = q(x) + dt (5) were q s a contnos, postve semdente fncton. Let s coose as follows: q Lf (x) = V (x) + q(x) L g V (x) (6) Wen sbsttted nto te formla (), ts yelds te control law 8 q? L f V + [L f V ] + q [L g V ] >< L g V k(x) = (7) wen L g V (x) 6= >: wen L g V (x) = wc was orgnally proposed n [3]. Ts nverse optmal control law s contnos everywere except possbly at x =. More mportantly, t redces to te optmal control for te cost (5) wenever te clf V as te same level sets as te vale fncton. To see ts, let V? (x) be te vale fncton assocated wt (5), and assme tat t satses te HJB eqaton = mn q(x) + + L f V? (x) + L g V? (x) = q(x) + L f V? (x)? Lg V? (x) (8) Sppose tat V = (V? ) for some smoot class K fncton (n oter words, sppose tat V and V? ave te same level sets). Becase te dervatve s always postve, from (7) and (8) we ave k(x) =? L f V? + p [L f V? ] + q [L g V? ] L g V? =? L f V? + q q + [L gv? ] L g V? =? L f V? + q + [L gv? ] L g V? =? L gv? (x) (9) wen L g V (x) 6=, wc s exactly te optmal control for te cost (5). Wen L g V (x) s zero, ten k(x) = wc stll matces te optmal control becase L g V? (x) s also zero. To smmarze, f te level sets of te clf matc tose of te vale fncton, and f s cosen as n (6), ten te nverse optmal control s n fact te optmal control. As a specal case, sppose tat te system s lnear and te cost s qadratc: _x = Ax + B () Z J = x T Qx + dt () If standard stablzablty and detectablty assmptons are satsed, ten tere exsts a nqe symmetrc postve dente solton P to te Rccat eqaton A T P + P A? P BB T P + Q = () One can verfy tat V (x) = x T P x s a clf for ts lnear system. If we coose as n (6), namely, q (x) = [x T (A T P + P A)x] + [x T Qx][x T P BB T P x] q = [x T (Q?P BB T P )x] + [x T Qx][x T P BB T P x] = x T Q + P BB T P x (3) ten te formla (7) generates te standard LQ lnear optmal feedback law = k(x) =?B T P x. 3 Feedback lnearzable systems Let s llstrate an nverse optmal desgn for te class of (globally) feedback lnearzable systems (see [6]). Sppose tere exsts a deomorpsm = (x) wt () = wc transforms or system nto _ = A + B b() + a() () were te matrx par (A; B) s stablzable and te smoot fnctons a and b are sc tat b() = b () =, a() =, and a() 6= for all (we ave normalzed a and b so tat (A; B) represents te Jacoban lnearzaton of te system). Let Q be sc tat T Q approxmates q(x) n te cost fnctonal (5) arond x =, and let P be te symmetrc postve dente solton to te Rccat eqaton (). Ten te fncton V (x) = (x) T P (x) = T P s a clf for ts system, and te nverse optmal control law () s 8 () ><? k(x) = T P B a() wen () > (5) >: wen ()

3 were te fncton s gven by () = T A T P + P A + T P Bb() + () (6) If s cosen as n (6), ten te control law (5) wll locally approxmate te LQ optmal control?b T P for te lnearzed system. We can compare te nverse optmal control law (5) wt te feedback lnearzng control law gven by k(x) =? b() + BT P a() (7) x_ 5 3 Altog bot control laws (5) and (7) globally asymptotcally stablze te system () and locally mnmze te cost (5), te nverse optmal control law (5) s (globally) optmal wt respect to a meanngfl cost fnctonal, wereas te feedback lnearzng control law (7) s not (n general). For example, te feedback lnearzng control law for te system _x =?x 3 + (8) wold cancel te stablzng nonlnearty?x 3, bt te nverse optmal control law wold not becase sc a cancellaton s contrary to meanngfl optmalty. Unfortnately, one-dmensonal examples are not rc enog to llstrate potental ptfalls of te clf desgn metod, prmarly becase all clf's for a scalar system possess essentally te same level sets. Examples n two dmensons We wll rst consder te feedback lnearzable system _x = x (9) _x =?x + x sn(x + x ) + () One can verfy tat te control law? =?x e x +x () mnmzes te cost fnctonal Z J = x + dt () and tat te assocated vale fncton s V? (x) = e x +x? (3) Te Rccat eqaton () yelds P = I, wc means te feedback lnearzng control law (7) s FL =?x + sn(x + x ) () Altog ts control law s not te same as te optmal control law (), t as te same qaltatve sape. Let s now try an nverse optmal desgn sng te clf V (x) = x T P x = x + x. Ts s actally a weak clf for x_ Fgre : Te vale fncton V? (x) from (9). ts system becase te neqalty n () s non-strct wen x =. Neverteless, we can proceed wt te nverse optmal desgn provded we do te followng: rst, we mst coose to be postve semdente and ceck tat te resltng control law s contnos; second, we mst make sre tat LaSalle's teorem apples so tat we can conclde global asymptotc stablty. Keepng tese catons n mnd, we see tat n (6) s (x) = x sn(x + x ) + (x) (5) One can verfy tat te coce = x recovers te feedback lnearzng control law (). Also, te coce = x cos(x + x ) from (6) recovers te optmal control law (); ts was to be expected becase te vale fncton V? and te clf V bot ave crcles as level sets. We next consder an example for wc te level sets of te vale fncton are far from beng ellpsod: _x = x (6) _x =?e x (x + x ) + x e x+3x + e x+x (7) One can verfy tat te control law? =?x e x+x (8) mnmzes te cost fnctonal () and tat te assocated vale fncton s V? (x) = x +? e?x ( + x ) (9) Ts vale fncton s smoot and postve dente, bt t s not proper as can be seen from te noncompactness of some of ts level sets (Fgre ). Ts no clf wll ave te same level sets as V?, and t remans to be seen weter or not some clf desgn can recover te optmal control.

4 x x tme tme x x tme tme tme Fgre : Soltons to (6){(7) from ntal condton (?; ) wt optmal control (8) (sold), nverse optmal control (3) (dased), and feedback lnearzng control (7) (dotted). We wll now try te clf desgn otlned n Secton 3. We let (A; B) be te lnearzaton of te system (6){(7) abot zero: A = ; B = (3)? Wt Q cosen accordng to te cost (), te solton to te Rccat eqaton () s P = I. Ts we wll se te weak clf V (x) = x T P x = x + x. We wll coose as n (6) so tat or control law s gven by te formla (7). For ts example we ave L f V (x) = x x p(x ) + e x+3x? e x (3) L g V (x) = x e x+x (3) were p(x ) represents te smoot fncton p(x ) =? ex x (33) (te apparent snglarty at x = s removable). Upon sbstttng tese expressons nto (7) sng q(x) = x, we obtan te followng control law: k(x) =? x e x?x?x p + e x+3x? e x (3) + qx p + x p e x+3x? e x + e x +3x + e x Ts control law s contnos even tog we sed only a weak clf n te formla (7). Moreover, k(x) = wen x = wc means LaSalle's teorem garantees te global asymptotc stablty of te closed-loop system. Note tat ts nverse optmal control (3) concdes wt te optmal control (8) at ponts were eter x = or x = tme Fgre 3: Soltons to (6){(7) from ntal condton (; ) wt optmal control (8) (sold), nverse optmal control (3) (dased), and feedback lnearzng control (7) (dotted). Fgre sows smlaton reslts for te system (6){ (7) from te ntal condton (?; ). Not srprsngly, te optmal control (8) (sold lne), wc generates a cost () of J = from ts ntal condton, yelds better reslts tan eter te nverse optmal control (3) (dased lne, J = 39) or te feedback lnearzng control (7) (dotted lne, J = 38). In fact, te nverse optmal control generates te gest cost from ts ntal condton. Ts does not contradct nverse optmalty becase ts control (3) optmzes a derent, nspeced cost fnctonal. Fgre 3 sows smlaton reslts from te ntal condton (; ); ere te costs are J = (optmal), J = : (nverse optmal), and J = :5 (feedback lnearzaton). Note tat all tree controllers provde nearly te same performance for small ntal condtons. We conclde ts secton by sowng ow an alternatve clf desgn can recover te optmal control (8) for ts system (6){(7). Recall tat we cannot se te vale fncton (9) as or clf becase t s not a proper fncton (some of ts level sets are not compact). However, we sold be able to nd a vald clf wose level sets look more lke te ones n Fgre tan lke te crclar level sets of te clf sed above. Rater tan coose or clf trog feedback lnearzaton as above, we wll take te system nonlneartes nto accont drng or constrcton of te clf. We rst rewrte te system (6){(7) as follows: _x = x (35) _x =?e x (x + x ) + e x+x ( + x e x+x ) (36) We next observe tat te system obtaned by droppng te second term n (36), namely, _x = x (37)

5 x_ x_ Fgre : Te clf V (x) from () wt c =. _x =?e x (x + x ) (38) s already globally asymptotcally stable. Any Lyapnov fncton for ts trncated system (37){(38) wll be a clf for te complete system (35){(36); or strategy s to nd sc a fncton. Let te fncton W (x) be gven by W (x) = x (x + x ) (39) We dene a C fncton : IR! IR + wt dervatve as follows: (s) = (s) = ( s +s wen s wen s < ( s(+s) wen s (+s) wen s < () () Te dervatve satses (s) = for s and < (s) < for s >. Frtermore, we ave (s)! as s!. It follows tat te fncton V dened by V (x) = (c + )V? (x) + (W (x)) () s C, postve dente, and radally nbonded, were c > s a desgn parameter. One can verfy tat V s n fact a Lyapnov fncton for te trncated system (37){(38), wc means we may se V as a clf n or control desgn. Te level sets of V, sown n Fgre, are smlar n sape to tose of te vale fncton V?. Te rst step n te constrcton of te control law from te clf V s to compte te dervatve of V along soltons to te orgnal system (35){(36): _V = L f V (x) + L g V (x) =?x [c +? (W )]? (W )e x (x + x )? (W )e x W + e x+x ( + x e x+x ) (c + )x e?x + (W )(x + x ) (3) From ts expresson we can conclde tat V s a weak clf: te control =? x e x+x renders V _ negatve semdente. We ave left to coose te fncton n te formla () for te nverse optmal control law. Coosng as n (6) sold prodce a near-optmal control law becase te level sets of or new clf () closely matc tose of te vale fncton (9). Indeed, smlatons from te ntal condton (?; ) sow tat te cost () generated by ts new nverse optmal control s J = : wc s only slgtly ger tan te optmal cost J =. A derent coce for, namely, (x) =?L f V (x) + x e x+x L g V (x) = x [c +? (W )] + (W )e x (x + x ) + (W )e x W + x e x+x L g V (x) () wll exactly recover te optmal control (8). One can verfy tat ts coce () s postve semdente and s terefore a vald coce n te nverse optmal desgn. Te conclson drawn from tese examples s tat te qalty of te clf desgn wt nverse optmalty can depend eavly on te coce for te clf V and te desred sze of ts dervatve. Fndng te best clf for a gven cost wold reqre solvng an HJB eqaton, a task wc te nverse optmal desgn s meant to avod. Wat we need, terefore, are metods for mprovng te coce for te clf wen te controller desgns t generates are nsatsfactory. 5 Dscsson Te Lyapnov desgn dscssed n ts paper conssts of two basc steps: Step #: Step #: nd a clf V se te clf to constrct an nverse optmal control law k Wle a clf wll always exst wenever te system s stablzable, te task of constrctng a clf n Step # may not be feasble for a general nonlnear system. For ts reason, Lyapnov desgn s best sted to systems avng specal strctres wc we know ow to explot (e.g. te feedback lnearzable systems of Secton 3). If a clf cannot be fond for te complete system, t may be possble to \decentralze" te problem, nd clf's for te separate sbsystems, and se varos nterconnecton/small-gan teorems [7, 8, 9, ] to prove te stablty of te complete system. For tose classes of systems for wc metods for constrctng clf's are avalable, great care sold be taken to explot desgn exbltes n Step # so tat good coces for te control law k are possble n Step #. We ave sown tat f te level sets of te clf matc tose of te vale fncton, ten te nverse optmal desgn, wt cosen as n (6), s n fact optmal. Moreover, for feedback lnearzable systems we can always

6 nd a clf wose level sets matc tose of te vale fncton n a negborood of te eqlbrm, and te resltng nverse optmal desgn s locally optmal. In most cases, owever, te level sets wll not matc globally, and te smplest coces n te clf desgn metod may generate control laws wc are far from optmal for large devatons from te eqlbrm. In sc cases, non-obvos coces n te clf desgn may be reqred to approac global optmalty. Peraps te greatest advantage of te Lyapnov desgn metod s ts ablty to accont for ncertanty n te fnctons f and g n te system descrpton (). Indeed, te nverse optmal desgn dscssed n ts paper was orgnally developed for ncertan nonlnear systems admttng \robst" clf's (rclf's) [5]. Altog feedback lnearzaton metods do not easly yeld rclf's for ncertan systems, more powerfl backsteppng metods can often be sccessflly appled []. However, backsteppng desgn metods are extremely exble, and agan te smplest desgn coces n Step # may exclde all good control laws n Step # []. Mc as yet to be dscovered abot ow to make smart coces n Lyapnov desgn. Please see ttp://ot.caltec.ed/ doyle for frter detals and a comparson of reslts on several examples. Acknowledgments: Te ators wold lke to tank Jon Doyle for s contrbtons to dscssons wc revealed tat (6) s a partclarly nterestng coce n te proposed desgn metod. References [] Z. Artsten, \Stablzaton wt relaxed controls," Nonlnear Anal., vol. 7, no., pp. 63{73, 983. [] E. D. Sontag, \A Lyapnov-lke caracterzaton of asymptotc controllablty," SIAM J. Contr. Optmz., vol., no. 3, pp. 6{7, 983. [3] E. D. Sontag, \A `nversal' constrcton of Artsten's teorem on nonlnear stablzaton," Syst. Contr. Lett., vol. 3, no., pp. 7{3, 989. [] R. E. Kalman, \Wen s a lnear control system optmal?," Trans. ASME Ser. D: J. Basc Eng., vol. 86, pp. {, 96. [5] B. D. O. Anderson and J. B. Moore, Lnear Optmal Control. Englewood Cls, New Jersey: Prentce- Hall, 97. [6] B. P. Molnar, \Te stable reglator problem and ts nverse," IEEE Trans. Atomat. Contr., vol. 8, pp. 5{59, Oct [7] P. J. Moylan and B. D. O. Anderson, \Nonlnear reglator teory and an nverse optmal control problem," IEEE Trans. Atomat. Contr., vol. 8, pp. 6{ 6, Oct [8] P. J. Moylan, \Implcatons of passvty n a class of nonlnear systems," IEEE Trans. Atomat. Contr., vol. 9, pp. 373{38, Ag. 97. [9] D. H. Jacobson, Extensons of Lnear-Qadratc Contol, Optmzaton and Matrx Teory. London: Academc Press, 977. [] C. A. Harvey and G. Sten, \Qadratc wegts for asymptotc reglator propertes," IEEE Trans. Atomat. Contr., vol. 3, pp. 378{387, Jne 978. [] D. H. Jacobson, D. H. Martn, M. Pacter, and T. Gevec, Extensons of Lnear-Qadratc Contol Teory, vol. 7 of Lectre Notes n Control and Informaton Scences. Berln: Sprnger-Verlag, 98. [] S. T. Glad, \Robstness of nonlnear state feedback A srvey," Atomatca, vol. 3, no., pp. 5{35, 987. [3] K. E. Lenz, P. P. Kargonekar, and J. C. Doyle, \Wen s a controller H -optmal?," Mat. Control Sgnals Systems, vol., pp. 7{, 988. [] J. Feng and M. C. Smt, \Wen s a controller optmal n te sense of H loop-sapng?," IEEE Trans. Atomat. Contr., vol., pp. 6{39, Dec [5] R. A. Freeman and P. V. Kokotovc, \Inverse optmalty n robst stablzaton," SIAM J. Contr. Optmz., vol. 3, pp. 365{39, Jly 996. [6] R. A. Freeman and P. V. Kokotovc, \Optmal nonlnear controllers for feedback lnearzable systems," n Proceedngs of te 995 Amercan Control Conference, (Seattle, Wasngton), pp. 7{76, Jne 995. [7] Z.-P. Jang, A. R. Teel, and L. Praly, \Smallgan teorem for ISS systems and applcatons," Mat. Control Sgnals Systems, vol. 7, pp. 95{, 99. [8] I. M. Y. Mareels and D. J. Hll, \Monotone stablty of nonlnear feedback systems," J. Mat. Syst. Estm. Contr., vol., pp. 75{9, 99. [9] A. R. Teel, \A nonlnear small gan teorem for te analyss of control systems wt satraton," IEEE Trans. Atomat. Contr.. To appear. [] E. D. Sontag, \Frter facts abot npt to state stablzaton," IEEE Trans. Atomat. Contr., vol. 35, pp. 73{76, Apr. 99. [] R. A. Freeman and P. V. Kokotovc, Robst Nonlnear Control Desgn. Boston: Brkaser, 996. [] R. A. Freeman and P. V. Kokotovc, \Desgn of `softer' robst nonlnear control laws," Atomatca, vol. 9, no. 6, pp. 5{37, 993.

, 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

, 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 information

Lecture: Financing Based on Market Values II

Lecture: Financing Based on Market Values II Lectre: Fnancng Based on Market Vales II Ltz Krscwtz & Andreas Löler Dsconted Cas Flow, Secton 2.4.4 2.4.5, Otlne 2.4.4 Mles-Ezzell- and Modglan-Mller Mles-Ezzell adjstment Modglan-Mller adjstment 2.4.5

More information

AE/ME 339. K. M. Isaac. 8/31/2004 topic4: Implicit method, Stability, ADI method. Computational Fluid Dynamics (AE/ME 339) MAEEM Dept.

AE/ME 339. K. M. Isaac. 8/31/2004 topic4: Implicit method, Stability, ADI method. Computational Fluid Dynamics (AE/ME 339) MAEEM Dept. AE/ME 339 Comptatonal Fld Dynamcs (CFD) Comptatonal Fld Dynamcs (AE/ME 339) Implct form of dfference eqaton In the prevos explct method, the solton at tme level n,,n, depended only on the known vales of,

More information

Exact Solutions for Nonlinear D-S Equation by Two Known Sub-ODE Methods

Exact Solutions for Nonlinear D-S Equation by Two Known Sub-ODE Methods Internatonal Conference on Compter Technology and Scence (ICCTS ) IPCSIT vol. 47 () () IACSIT Press, Sngapore DOI:.7763/IPCSIT..V47.64 Exact Soltons for Nonlnear D-S Eqaton by Two Known Sb-ODE Methods

More information

SE Story Shear Frame. Final Project. 2 Story Bending Beam. m 2. u 2. m 1. u 1. m 3. u 3 L 3. Given: L 1 L 2. EI ω 1 ω 2 Solve for m 2.

SE Story Shear Frame. Final Project. 2 Story Bending Beam. m 2. u 2. m 1. u 1. m 3. u 3 L 3. Given: L 1 L 2. EI ω 1 ω 2 Solve for m 2. SE 8 Fnal Project Story Sear Frame Gven: EI ω ω Solve for Story Bendng Beam Gven: EI ω ω 3 Story Sear Frame Gven: L 3 EI ω ω ω 3 3 m 3 L 3 Solve for Solve for m 3 3 4 3 Story Bendng Beam Part : Determnng

More information

Stanford University CS254: Computational Complexity Notes 7 Luca Trevisan January 29, Notes for Lecture 7

Stanford University CS254: Computational Complexity Notes 7 Luca Trevisan January 29, Notes for Lecture 7 Stanford Unversty CS54: Computatonal Complexty Notes 7 Luca Trevsan January 9, 014 Notes for Lecture 7 1 Approxmate Countng wt an N oracle We complete te proof of te followng result: Teorem 1 For every

More information

The Bellman Equation

The Bellman Equation The Bellman Eqaton Reza Shadmehr In ths docment I wll rovde an elanaton of the Bellman eqaton, whch s a method for otmzng a cost fncton and arrvng at a control olcy.. Eamle of a game Sose that or states

More information

The Finite Element Method: A Short Introduction

The Finite Element Method: A Short Introduction Te Fnte Element Metod: A Sort ntroducton Wat s FEM? Te Fnte Element Metod (FEM) ntroduced by engneers n late 50 s and 60 s s a numercal tecnque for solvng problems wc are descrbed by Ordnary Dfferental

More information

On Pfaff s solution of the Pfaff problem

On Pfaff s solution of the Pfaff problem Zur Pfaff scen Lösung des Pfaff scen Probles Mat. Ann. 7 (880) 53-530. On Pfaff s soluton of te Pfaff proble By A. MAYER n Lepzg Translated by D. H. Delpenc Te way tat Pfaff adopted for te ntegraton of

More information

Shuai Dong. Isaac Newton. Gottfried Leibniz

Shuai Dong. Isaac Newton. Gottfried Leibniz Computatonal pyscs Sua Dong Isaac Newton Gottred Lebnz Numercal calculus poston dervatve ntegral v velocty dervatve ntegral a acceleraton Numercal calculus Numercal derentaton Numercal ntegraton Roots

More information

COMP4630: λ-calculus

COMP4630: λ-calculus COMP4630: λ-calculus 4. Standardsaton Mcael Norrs Mcael.Norrs@ncta.com.au Canberra Researc Lab., NICTA Semester 2, 2015 Last Tme Confluence Te property tat dvergent evaluatons can rejon one anoter Proof

More information

Multivariate Ratio Estimator of the Population Total under Stratified Random Sampling

Multivariate Ratio Estimator of the Population Total under Stratified Random Sampling Open Journal of Statstcs, 0,, 300-304 ttp://dx.do.org/0.436/ojs.0.3036 Publsed Onlne July 0 (ttp://www.scrp.org/journal/ojs) Multvarate Rato Estmator of te Populaton Total under Stratfed Random Samplng

More information

Solution for singularly perturbed problems via cubic spline in tension

Solution for singularly perturbed problems via cubic spline in tension ISSN 76-769 England UK Journal of Informaton and Computng Scence Vol. No. 06 pp.6-69 Soluton for sngularly perturbed problems va cubc splne n tenson K. Aruna A. S. V. Rav Kant Flud Dynamcs Dvson Scool

More information

Iranian Journal of Mathematical Chemistry, Vol. 5, No.2, November 2014, pp

Iranian Journal of Mathematical Chemistry, Vol. 5, No.2, November 2014, pp Iranan Journal of Matematcal Cemstry, Vol. 5, No.2, November 204, pp. 85 90 IJMC Altan dervatves of a grap I. GUTMAN (COMMUNICATED BY ALI REZA ASHRAFI) Faculty of Scence, Unversty of Kragujevac, P. O.

More information

Image classification. Given the bag-of-features representations of images from different classes, how do we learn a model for distinguishing i them?

Image classification. Given the bag-of-features representations of images from different classes, how do we learn a model for distinguishing i them? Image classfcaton Gven te bag-of-features representatons of mages from dfferent classes ow do we learn a model for dstngusng tem? Classfers Learn a decson rule assgnng bag-offeatures representatons of

More information

Overlapping Control Structure based on Adaptive Control for Water Distribution Network

Overlapping Control Structure based on Adaptive Control for Water Distribution Network Recent Advances n Systems Scence and Matematcal Modellng Overlappng Control Strctre based on Adaptve Control for Water Dstrbton Networ ERUJI SEKOZAWA Gradate Scool of Engneerng Kanagawa Unversty -6-, Roabas,

More information

Introduction. - The Second Lyapunov Method. - The First Lyapunov Method

Introduction. - The Second Lyapunov Method. - The First Lyapunov Method Stablty Analyss A. Khak Sedgh Control Systems Group Faculty of Electrcal and Computer Engneerng K. N. Toos Unversty of Technology February 2009 1 Introducton Stablty s the most promnent characterstc of

More information

Multigrid Methods and Applications in CFD

Multigrid Methods and Applications in CFD Multgrd Metods and Applcatons n CFD Mcael Wurst 0 May 009 Contents Introducton Typcal desgn of CFD solvers 3 Basc metods and ter propertes for solvng lnear systems of equatons 4 Geometrc Multgrd 3 5 Algebrac

More information

1 Introducton Nonlnearty crtera of Boolean functons Cryptograpc transformatons sould be nonlnear to be secure aganst varous attacks. For example, te s

1 Introducton Nonlnearty crtera of Boolean functons Cryptograpc transformatons sould be nonlnear to be secure aganst varous attacks. For example, te s KUIS{94{000 Nonlnearty crtera of Boolean functons HIROSE Souc IKEDA Katsuo Tel +81 75 753 5387 Fax +81 75 751 048 E-mal frose, kedag@kus.kyoto-u.ac.jp July 14, 1994 1 Introducton Nonlnearty crtera of Boolean

More information

Competitive Experimentation and Private Information

Competitive Experimentation and Private Information Compettve Expermentaton an Prvate Informaton Guseppe Moscarn an Francesco Squntan Omtte Analyss not Submtte for Publcaton Dervatons for te Gamma-Exponental Moel Dervaton of expecte azar rates. By Bayes

More information

Numerical Simulation of One-Dimensional Wave Equation by Non-Polynomial Quintic Spline

Numerical Simulation of One-Dimensional Wave Equation by Non-Polynomial Quintic Spline IOSR Journal of Matematcs (IOSR-JM) e-issn: 78-578, p-issn: 319-765X. Volume 14, Issue 6 Ver. I (Nov - Dec 018), PP 6-30 www.osrournals.org Numercal Smulaton of One-Dmensonal Wave Equaton by Non-Polynomal

More information

THE GUARANTEED COST CONTROL FOR UNCERTAIN LARGE SCALE INTERCONNECTED SYSTEMS

THE GUARANTEED COST CONTROL FOR UNCERTAIN LARGE SCALE INTERCONNECTED SYSTEMS Copyrght 22 IFAC 5th rennal World Congress, Barcelona, Span HE GUARANEED COS CONROL FOR UNCERAIN LARGE SCALE INERCONNECED SYSEMS Hroak Mukadan Yasuyuk akato Yoshyuk anaka Koch Mzukam Faculty of Informaton

More information

Solving Singularly Perturbed Differential Difference Equations via Fitted Method

Solving Singularly Perturbed Differential Difference Equations via Fitted Method Avalable at ttp://pvamu.edu/aam Appl. Appl. Mat. ISSN: 193-9466 Vol. 8, Issue 1 (June 013), pp. 318-33 Applcatons and Appled Matematcs: An Internatonal Journal (AAM) Solvng Sngularly Perturbed Dfferental

More information

CS 3750 Machine Learning Lecture 6. Monte Carlo methods. CS 3750 Advanced Machine Learning. Markov chain Monte Carlo

CS 3750 Machine Learning Lecture 6. Monte Carlo methods. CS 3750 Advanced Machine Learning. Markov chain Monte Carlo CS 3750 Machne Learnng Lectre 6 Monte Carlo methods Mlos Haskrecht mlos@cs.ptt.ed 5329 Sennott Sqare Markov chan Monte Carlo Importance samplng: samples are generated accordng to Q and every sample from

More information

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system

Transfer 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 information

TR/95 February Splines G. H. BEHFOROOZ* & N. PAPAMICHAEL

TR/95 February Splines G. H. BEHFOROOZ* & N. PAPAMICHAEL TR/9 February 980 End Condtons for Interpolatory Quntc Splnes by G. H. BEHFOROOZ* & N. PAPAMICHAEL *Present address: Dept of Matematcs Unversty of Tabrz Tabrz Iran. W9609 A B S T R A C T Accurate end condtons

More information

Y = X + " E [X 0 "] = 0 K E ["" 0 ] = = 2 I N : 2. So, you get an estimated parameter vector ^ OLS = (X 0 X) 1 X 0 Y:

Y = X +  E [X 0 ] = 0 K E [ 0 ] = = 2 I N : 2. So, you get an estimated parameter vector ^ OLS = (X 0 X) 1 X 0 Y: 1 Ecent OLS 1. Consder te model Y = X + " E [X 0 "] = 0 K E ["" 0 ] = = 2 I N : Ts s OLS appyland! OLS s BLUE ere. 2. So, you get an estmated parameter vector ^ OLS = (X 0 X) 1 X 0 Y: 3. You know tat t

More information

BAR & TRUSS FINITE ELEMENT. Direct Stiffness Method

BAR & TRUSS FINITE ELEMENT. Direct Stiffness Method BAR & TRUSS FINITE ELEMENT Drect Stness Method FINITE ELEMENT ANALYSIS AND APPLICATIONS INTRODUCTION TO FINITE ELEMENT METHOD What s the nte element method (FEM)? A technqe or obtanng approxmate soltons

More information

Traceability and uncertainty for phase measurements

Traceability and uncertainty for phase measurements Traceablty and ncertanty for phase measrements Karel Dražl Czech Metrology Insttte Abstract In recent tme the problems connected wth evalatng and expressng ncertanty n complex S-parameter measrements have

More information

5 The Laplace Equation in a convex polygon

5 The Laplace Equation in a convex polygon 5 Te Laplace Equaton n a convex polygon Te most mportant ellptc PDEs are te Laplace, te modfed Helmoltz and te Helmoltz equatons. Te Laplace equaton s u xx + u yy =. (5.) Te real and magnary parts of an

More information

Problem Set 4: Sketch of Solutions

Problem Set 4: Sketch of Solutions Problem Set 4: Sketc of Solutons Informaton Economcs (Ec 55) George Georgads Due n class or by e-mal to quel@bu.edu at :30, Monday, December 8 Problem. Screenng A monopolst can produce a good n dfferent

More information

Solutions to selected problems from homework 1.

Solutions to selected problems from homework 1. Jan Hagemejer 1 Soltons to selected problems from homeork 1. Qeston 1 Let be a tlty fncton hch generates demand fncton xp, ) and ndrect tlty fncton vp, ). Let F : R R be a strctly ncreasng fncton. If the

More information

princeton univ. F 17 cos 521: Advanced Algorithm Design Lecture 7: LP Duality Lecturer: Matt Weinberg

princeton 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 information

Lecture 10 Support Vector Machines II

Lecture 10 Support Vector Machines II Lecture 10 Support Vector Machnes II 22 February 2016 Taylor B. Arnold Yale Statstcs STAT 365/665 1/28 Notes: Problem 3 s posted and due ths upcomng Frday There was an early bug n the fake-test data; fxed

More information

Exam 1 Review Solutions

Exam 1 Review Solutions Exam Review Solutions Please also review te old quizzes, and be sure tat you understand te omework problems. General notes: () Always give an algebraic reason for your answer (graps are not sufficient),

More information

Lagrange Multipliers Kernel Trick

Lagrange Multipliers Kernel Trick Lagrange Multplers Kernel Trck Ncholas Ruozz Unversty of Texas at Dallas Based roughly on the sldes of Davd Sontag General Optmzaton A mathematcal detour, we ll come back to SVMs soon! subject to: f x

More information

MEMBRANE ELEMENT WITH NORMAL ROTATIONS

MEMBRANE ELEMENT WITH NORMAL ROTATIONS 9. MEMBRANE ELEMENT WITH NORMAL ROTATIONS Rotatons Mst Be Compatble Between Beam, Membrane and Shell Elements 9. INTRODUCTION { XE "Membrane Element" }The comple natre of most bldngs and other cvl engneerng

More information

Modeling Mood Variation and Covariation among Adolescent Smokers: Application of a Bivariate Location-Scale Mixed-Effects Model

Modeling Mood Variation and Covariation among Adolescent Smokers: Application of a Bivariate Location-Scale Mixed-Effects Model Modelng Mood Varaton and Covaraton among Adolescent Smokers: Applcaton of a Bvarate Locaton-Scale Mxed-Effects Model Oksana Pgach, PhD, Donald Hedeker, PhD, Robn Mermelsten, PhD Insttte for Health Research

More information

A Spline based computational simulations for solving selfadjoint singularly perturbed two-point boundary value problems

A Spline based computational simulations for solving selfadjoint singularly perturbed two-point boundary value problems ISSN 746-769 England UK Journal of Informaton and Computng Scence Vol. 7 No. 4 pp. 33-34 A Splne based computatonal smulatons for solvng selfadjont sngularly perturbed two-pont boundary value problems

More information

Not-for-Publication Appendix to Optimal Asymptotic Least Aquares Estimation in a Singular Set-up

Not-for-Publication Appendix to Optimal Asymptotic Least Aquares Estimation in a Singular Set-up Not-for-Publcaton Aendx to Otmal Asymtotc Least Aquares Estmaton n a Sngular Set-u Antono Dez de los Ros Bank of Canada dezbankofcanada.ca December 214 A Proof of Proostons A.1 Proof of Prooston 1 Ts roof

More information

Kernel Methods and SVMs Extension

Kernel Methods and SVMs Extension Kernel Methods and SVMs Extenson The purpose of ths document s to revew materal covered n Machne Learnng 1 Supervsed Learnng regardng support vector machnes (SVMs). Ths document also provdes a general

More information

SEMI-GLOBAL EXPONENTIAL STABILIZATION OF LINEAR SYSTEMS SUBJECT TO \INPUT SATURATION" VIA LINEAR FEEDBACKS. Zongli Lin & Ali Saberi

SEMI-GLOBAL EXPONENTIAL STABILIZATION OF LINEAR SYSTEMS SUBJECT TO \INPUT SATURATION VIA LINEAR FEEDBACKS. Zongli Lin & Ali Saberi Appeared n Systems & Control Letters, vol 1, pp-9, 199 SEMI-GLOBAL EXPONENTIAL STABILIZATION OF LINEAR SYSTEMS SUBJECT TO \INPUT SATURATION" VIA LINEAR FEEDBACKS Zongl Ln & Al Saber School of Electrcal

More information

Adaptive Dynamic Programming (ADP) For Discrete-Time Systems

Adaptive Dynamic Programming (ADP) For Discrete-Time Systems F.L. Lews & Dragna rabe Moncref-O Donnell Endowed Car ead Controls & Sensors Grop Atomaton & Robotcs Researc Insttte ARRI e Unversty of eas at Arlngton Adaptve Dynamc Programmng ADP For Dscrete-me Systems

More information

Correlation Clustering with Noisy Input

Correlation Clustering with Noisy Input Correlaton Clsterng wth Nosy Inpt Clare Mathe Warren Schdy Brown Unversty SODA 2010 Nosy Correlaton Clsterng Model Unknown base clsterng B of n obects Nose: each edge s controlled by an adversary wth probablty

More information

3/31/ = 0. φi φi. Use 10 Linear elements to solve the equation. dx x dx THE PETROV-GALERKIN METHOD

3/31/ = 0. φi φi. Use 10 Linear elements to solve the equation. dx x dx THE PETROV-GALERKIN METHOD THE PETROV-GAERKIN METHO Consder the Galern solton sng near elements of the modfed convecton-dffson eqaton α h d φ d φ + + = α s a parameter between and. If α =, we wll have the dscrete Galern form of

More information

SUBSYSTEM STABILIZATION APPROACH TO ROBUST DECENTRALIZED INVENTORY CONTROL IN SUPPLY NETWORKS

SUBSYSTEM STABILIZATION APPROACH TO ROBUST DECENTRALIZED INVENTORY CONTROL IN SUPPLY NETWORKS 5 94 24 «Ñèñòåìíûå òåõíîëîãèè» UDK 68.5.5.24 Y.I. Dorofeev SUBSYSEM SABILIZAION AOACH O OBUS DECENALIZED INVENOY CONOL IN SULY NEWOKS Abstract. A problem of the robst decentralzed nventory control strategy

More information

On a nonlinear compactness lemma in L p (0, T ; B).

On a nonlinear compactness lemma in L p (0, T ; B). On a nonlnear compactness lemma n L p (, T ; B). Emmanuel Matre Laboratore de Matématques et Applcatons Unversté de Haute-Alsace 4, rue des Frères Lumère 6893 Mulouse E.Matre@ua.fr 3t February 22 Abstract

More information

Nonlinear Programming Formulations for On-line Applications

Nonlinear Programming Formulations for On-line Applications Nonlnear Programmng Formlatons for On-lne Applcatons L. T. Begler Carnege Mellon Unversty Janary 2007 Jont work wth Vctor Zavala and Carl Lard NLP for On-lne Process Control Nonlnear Model Predctve Control

More information

U.C. Berkeley CS294: Beyond Worst-Case Analysis Luca Trevisan September 5, 2017

U.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 information

COSC 6374 Parallel Computation

COSC 6374 Parallel Computation COSC 67 Parallel Comptaton Partal Derental Eqatons Edgar Gabrel Fall 0 Nmercal derentaton orward derence ormla From te denton o dervatves one can derve an appromaton or te st dervatve Te same ormla can

More information

Nonlinear Network Structures for Optimal Control

Nonlinear Network Structures for Optimal Control tomaton & Robotcs Research Insttte RRI Nonlnear Network Strctres for Optmal Control Frank. ews and Mrad Mrad b-khalaf dvanced Controls, Sensors, and MEMS CSM grop System Cost f + g 0 [ ] V Q + dt he Usal

More information

A New Recursive Method for Solving State Equations Using Taylor Series

A New Recursive Method for Solving State Equations Using Taylor Series I J E E E C Internatonal Journal of Electrcal, Electroncs ISSN No. (Onlne) : 77-66 and Computer Engneerng 1(): -7(01) Specal Edton for Best Papers of Mcael Faraday IET Inda Summt-01, MFIIS-1 A New Recursve

More information

Function Composition and Chain Rules

Function Composition and Chain Rules Function Composition and s James K. Peterson Department of Biological Sciences and Department of Matematical Sciences Clemson University Marc 8, 2017 Outline 1 Function Composition and Continuity 2 Function

More information

College of Computer & Information Science Fall 2009 Northeastern University 20 October 2009

College 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 information

3.4 Worksheet: Proof of the Chain Rule NAME

3.4 Worksheet: Proof of the Chain Rule NAME Mat 1170 3.4 Workseet: Proof of te Cain Rule NAME Te Cain Rule So far we are able to differentiate all types of functions. For example: polynomials, rational, root, and trigonometric functions. We are

More information

HOMOGENEOUS LEAST SQUARES PROBLEM

HOMOGENEOUS LEAST SQUARES PROBLEM the Photogrammetrc Jornal of nl, Vol. 9, No., 005 HOMOGENEOU LE QURE PROLEM Kejo Inklä Helsnk Unversty of echnology Laboratory of Photogrammetry Remote ensng P.O.ox 00, IN-005 KK kejo.nkla@tkk.f RC he

More information

On a direct solver for linear least squares problems

On a direct solver for linear least squares problems ISSN 2066-6594 Ann. Acad. Rom. Sc. Ser. Math. Appl. Vol. 8, No. 2/2016 On a drect solver for lnear least squares problems Constantn Popa Abstract The Null Space (NS) algorthm s a drect solver for lnear

More information

Delhi School of Economics Course 001: Microeconomic Theory Solutions to Problem Set 2.

Delhi School of Economics Course 001: Microeconomic Theory Solutions to Problem Set 2. Delh School of Economcs Corse 00: Mcroeconomc Theor Soltons to Problem Set.. Propertes of % extend to and. (a) Assme x x x. Ths mples: x % x % x ) x % x. Now sppose x % x. Combned wth x % x and transtvt

More information

Stability analysis for class of switched nonlinear systems

Stability analysis for class of switched nonlinear systems Stablty analyss for class of swtched nonlnear systems The MIT Faculty has made ths artcle openly avalable. Please share how ths access benefts you. Your story matters. Ctaton As Publshed Publsher Shaker,

More information

Polynomial Interpolation

Polynomial Interpolation Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximatinga function fx, wose values at a set of distinct points x, x, x,, x n are known, by a polynomial P x suc

More information

PubH 7405: REGRESSION ANALYSIS. SLR: INFERENCES, Part II

PubH 7405: REGRESSION ANALYSIS. SLR: INFERENCES, Part II PubH 7405: REGRESSION ANALSIS SLR: INFERENCES, Part II We cover te topc of nference n two sessons; te frst sesson focused on nferences concernng te slope and te ntercept; ts s a contnuaton on estmatng

More information

(a) At what number x = a does f have a removable discontinuity? What value f(a) should be assigned to f at x = a in order to make f continuous at a?

(a) At what number x = a does f have a removable discontinuity? What value f(a) should be assigned to f at x = a in order to make f continuous at a? Solutions to Test 1 Fall 016 1pt 1. Te grap of a function f(x) is sown at rigt below. Part I. State te value of eac limit. If a limit is infinite, state weter it is or. If a limit does not exist (but is

More information

Math Spring 2013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, (1/z) 2 (1/z 1) 2 = lim

Math Spring 2013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, (1/z) 2 (1/z 1) 2 = lim Mat 311 - Spring 013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, 013 Question 1. [p 56, #10 (a)] 4z Use te teorem of Sec. 17 to sow tat z (z 1) = 4. We ave z 4z (z 1) = z 0 4 (1/z) (1/z

More information

CENTROID (AĞIRLIK MERKEZİ )

CENTROID (AĞIRLIK MERKEZİ ) CENTOD (ĞLK MEKEZİ ) centrod s a geometrcal concept arsng from parallel forces. Tus, onl parallel forces possess a centrod. Centrod s tougt of as te pont were te wole wegt of a pscal od or sstem of partcles

More information

Section 8.3 Polar Form of Complex Numbers

Section 8.3 Polar Form of Complex Numbers 80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the

More information

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could

More information

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT LIMITS AND DERIVATIVES Te limit of a function is defined as te value of y tat te curve approaces, as x approaces a particular value. Te limit of f (x) as x approaces a is written as f (x) approaces, as

More information

LECTURE 5: FIBRATIONS AND HOMOTOPY FIBERS

LECTURE 5: FIBRATIONS AND HOMOTOPY FIBERS LECTURE 5: FIBRATIONS AND HOMOTOPY FIBERS In ts lecture we wll ntroduce two mortant classes of mas of saces, namely te Hurewcz fbratons and te more general Serre fbratons, wc are bot obtaned by mosng certan

More information

Fracture analysis of FRP composites using a meshless finite point collocation method

Fracture analysis of FRP composites using a meshless finite point collocation method Forth Internatonal Conference on FRP Compostes n Cvl Engneerng (CICE008) -4Jly 008, Zrch, Swtzerland Fractre analyss of FRP compostes sng a meshless fnte pont collocaton method M. Shahverd & S. Mohammad

More information

Order of Accuracy. ũ h u Ch p, (1)

Order of Accuracy. ũ h u Ch p, (1) Order of Accuracy 1 Terminology We consider a numerical approximation of an exact value u. Te approximation depends on a small parameter, wic can be for instance te grid size or time step in a numerical

More information

Which Separator? Spring 1

Which Separator? Spring 1 Whch Separator? 6.034 - Sprng 1 Whch Separator? Mamze the margn to closest ponts 6.034 - Sprng Whch Separator? Mamze the margn to closest ponts 6.034 - Sprng 3 Margn of a pont " # y (w $ + b) proportonal

More information

CENTROID (AĞIRLIK MERKEZİ )

CENTROID (AĞIRLIK MERKEZİ ) CENTOD (ĞLK MEKEZİ ) centrod s a geometrcal concept arsng from parallel forces. Tus, onl parallel forces possess a centrod. Centrod s tougt of as te pont were te wole wegt of a pscal od or sstem of partcles

More information

On the Multicriteria Integer Network Flow Problem

On the Multicriteria Integer Network Flow Problem BULGARIAN ACADEMY OF SCIENCES CYBERNETICS AND INFORMATION TECHNOLOGIES Volume 5, No 2 Sofa 2005 On the Multcrtera Integer Network Flow Problem Vassl Vasslev, Marana Nkolova, Maryana Vassleva Insttute of

More information

The Prncpal Component Transform The Prncpal Component Transform s also called Karhunen-Loeve Transform (KLT, Hotellng Transform, oregenvector Transfor

The Prncpal Component Transform The Prncpal Component Transform s also called Karhunen-Loeve Transform (KLT, Hotellng Transform, oregenvector Transfor Prncpal Component Transform Multvarate Random Sgnals A real tme sgnal x(t can be consdered as a random process and ts samples x m (m =0; ;N, 1 a random vector: The mean vector of X s X =[x0; ;x N,1] T

More information

EQUATION CHAPTER 1 SECTION 1STRAIN IN A CONTINUOUS MEDIUM

EQUATION CHAPTER 1 SECTION 1STRAIN IN A CONTINUOUS MEDIUM EQUTION HPTER SETION STRIN IN ONTINUOUS MEIUM ontent Introdcton One dmensonal stran Two-dmensonal stran Three-dmensonal stran ondtons for homogenety n two-dmensons n eample of deformaton of a lne Infntesmal

More information

Computer Graphics. Curves and Surfaces. Hermite/Bezier Curves, (B-)Splines, and NURBS. By Ulf Assarsson

Computer Graphics. Curves and Surfaces. Hermite/Bezier Curves, (B-)Splines, and NURBS. By Ulf Assarsson Compter Graphcs Crves and Srfaces Hermte/Bezer Crves, (B-)Splnes, and NURBS By Ulf Assarsson Most of the materal s orgnally made by Edward Angel and s adapted to ths corse by Ulf Assarsson. Some materal

More information

Control of Uncertain Bilinear Systems using Linear Controllers: Stability Region Estimation and Controller Design

Control of Uncertain Bilinear Systems using Linear Controllers: Stability Region Estimation and Controller Design Control of Uncertan Blnear Systems usng Lnear Controllers: Stablty Regon Estmaton Controller Desgn Shoudong Huang Department of Engneerng Australan Natonal Unversty Canberra, ACT 2, Australa shoudong.huang@anu.edu.au

More information

ORDINARY DIFFERENTIAL EQUATIONS EULER S METHOD

ORDINARY DIFFERENTIAL EQUATIONS EULER S METHOD Numercal Analss or Engneers German Jordanan Unverst ORDINARY DIFFERENTIAL EQUATIONS We wll eplore several metods o solvng rst order ordnar derental equatons (ODEs and we wll sow ow tese metods can be appled

More information

1 Derivation of Point-to-Plane Minimization

1 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 information

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator. Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative

More information

EMISSION MEASUREMENTS IN DUAL FUELED INTERNAL COMBUSTION ENGINE TESTS

EMISSION MEASUREMENTS IN DUAL FUELED INTERNAL COMBUSTION ENGINE TESTS XVIII IEKO WORLD NGRESS etrology for a Sstanable Development September, 17, 006, Ro de Janero, Brazl EISSION EASUREENTS IN DUAL FUELED INTERNAL BUSTION ENGINE TESTS A.F.Orlando 1, E.Santos, L.G.do Val

More information

Numerical Differentiation

Numerical Differentiation Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function

More information

bounds, but Mao [{4] only dscussed te mean square (te case of p = ) almost sure exponental stablty. Due to te new tecnques developed n ts paper, te re

bounds, but Mao [{4] only dscussed te mean square (te case of p = ) almost sure exponental stablty. Due to te new tecnques developed n ts paper, te re Asymptotc Propertes of Neutral Stocastc Derental Delay Equatons Xuerong Mao Department of Statstcs Modellng Scence Unversty of Stratclyde Glasgow G XH, Scotl, U.K. Abstract: Ts paper dscusses asymptotc

More information

A Discrete Approach to Continuous Second-Order Boundary Value Problems via Monotone Iterative Techniques

A Discrete Approach to Continuous Second-Order Boundary Value Problems via Monotone Iterative Techniques Internatonal Journal of Dfference Equatons ISSN 0973-6069, Volume 12, Number 1, pp. 145 160 2017) ttp://campus.mst.edu/jde A Dscrete Approac to Contnuous Second-Order Boundary Value Problems va Monotone

More information

Solutions to exam in SF1811 Optimization, Jan 14, 2015

Solutions to exam in SF1811 Optimization, Jan 14, 2015 Solutons to exam n SF8 Optmzaton, Jan 4, 25 3 3 O------O -4 \ / \ / The network: \/ where all lnks go from left to rght. /\ / \ / \ 6 O------O -5 2 4.(a) Let x = ( x 3, x 4, x 23, x 24 ) T, where the varable

More information

Feature Selection: Part 1

Feature Selection: Part 1 CSE 546: Machne Learnng Lecture 5 Feature Selecton: Part 1 Instructor: Sham Kakade 1 Regresson n the hgh dmensonal settng How do we learn when the number of features d s greater than the sample sze n?

More information

How to Find the Derivative of a Function: Calculus 1

How to Find the Derivative of a Function: Calculus 1 Introduction How to Find te Derivative of a Function: Calculus 1 Calculus is not an easy matematics course Te fact tat you ave enrolled in suc a difficult subject indicates tat you are interested in te

More information

ECE559VV Project Report

ECE559VV Project Report ECE559VV Project Report (Supplementary Notes Loc Xuan Bu I. MAX SUM-RATE SCHEDULING: THE UPLINK CASE We have seen (n the presentaton that, for downlnk (broadcast channels, the strategy maxmzng the sum-rate

More information

CME 302: NUMERICAL LINEAR ALGEBRA FALL 2005/06 LECTURE 13

CME 302: NUMERICAL LINEAR ALGEBRA FALL 2005/06 LECTURE 13 CME 30: NUMERICAL LINEAR ALGEBRA FALL 005/06 LECTURE 13 GENE H GOLUB 1 Iteratve Methods Very large problems (naturally sparse, from applcatons): teratve methods Structured matrces (even sometmes dense,

More information

4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these.

4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these. Mat 11. Test Form N Fall 016 Name. Instructions. Te first eleven problems are wort points eac. Te last six problems are wort 5 points eac. For te last six problems, you must use relevant metods of algebra

More information

Math 1210 Midterm 1 January 31st, 2014

Math 1210 Midterm 1 January 31st, 2014 Mat 110 Midterm 1 January 1st, 01 Tis exam consists of sections, A and B. Section A is conceptual, wereas section B is more computational. Te value of every question is indicated at te beginning of it.

More information

Design and Optimization of Fuzzy Controller for Inverse Pendulum System Using Genetic Algorithm

Design and Optimization of Fuzzy Controller for Inverse Pendulum System Using Genetic Algorithm Desgn and Optmzaton of Fuzzy Controller for Inverse Pendulum System Usng Genetc Algorthm H. Mehraban A. Ashoor Unversty of Tehran Unversty of Tehran h.mehraban@ece.ut.ac.r a.ashoor@ece.ut.ac.r Abstract:

More information

The equation of motion of a dynamical system is given by a set of differential equations. That is (1)

The equation of motion of a dynamical system is given by a set of differential equations. That is (1) Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence

More information

The finite element method explicit scheme for a solution of one problem of surface and ground water combined movement

The finite element method explicit scheme for a solution of one problem of surface and ground water combined movement IOP Conference Seres: Materals Scence and Engneerng PAPER OPEN ACCESS e fnte element metod explct sceme for a soluton of one problem of surface and ground water combned movement o cte ts artcle: L L Glazyrna

More information

Using T.O.M to Estimate Parameter of distributions that have not Single Exponential Family

Using T.O.M to Estimate Parameter of distributions that have not Single Exponential Family IOSR Journal of Mathematcs IOSR-JM) ISSN: 2278-5728. Volume 3, Issue 3 Sep-Oct. 202), PP 44-48 www.osrjournals.org Usng T.O.M to Estmate Parameter of dstrbutons that have not Sngle Exponental Famly Jubran

More information

Module 9. Lecture 6. Duality in Assignment Problems

Module 9. Lecture 6. Duality in Assignment Problems Module 9 1 Lecture 6 Dualty n Assgnment Problems In ths lecture we attempt to answer few other mportant questons posed n earler lecture for (AP) and see how some of them can be explaned through the concept

More information

Polynomial Interpolation

Polynomial Interpolation Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximating a function f(x, wose values at a set of distinct points x, x, x 2,,x n are known, by a polynomial P (x

More information

Linear Feature Engineering 11

Linear 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 information

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,

More information

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t). . Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd, periodic function tat as been sifted upwards, so we will use

More information