Unknown Input Based Observer Synthesis for a Polynomial T-S Fuzzy Model System with Uncertainties
|
|
- Denis Bailey
- 5 years ago
- Views:
Transcription
1 Unknown Input Based Obseve Synthess fo a Polynomal -S Fuzzy Model System wth Uncetantes Van-Phong Vu Wen-June Wang Fellow IEEE Hsang-heh hen Jacek M Zuada Lfe Fellow IEEE Abstact hs pape poposes a new appoach based on the unknown nput method to synthesze the obseve fo polynomal akag-sugeno (-S) fuzzy system wth uncetantes In ths pape the uppe bounds of uncetantes ae not gven the effect of uncetantes s elmnated wthout desgnng an exta contolle Wth the ads of the non-common Lyapunov theoy Matlab s tools of the Sum-of-Squae (SOS) a new obseve s syntheszed n whch the obseve fom s completely dffeent fom the tadtonal obseve foms epoted n pevous papes he condtons fo the obseve synthess ae much elaxed the complexty of the desgn pocess s educed Fnally two llustatve examples ae pesented to demonstate the effectveness of the poposed method Index ems Uncetan polynomal -S fuzzy systems obseve synthess unknown nputs Sum of Squae (SOS) I INRODUION agak-sugeno (-S) fuzzy model []-[4] has eceved a geat deal of attenton n contol system eseach aea hs model has povded anothe way to solve the poblems of nonlnea contol systems heefoe many theoes contol desgn methods fo lnea contol systems can be appled n the -S fuzzy system In addton a new appoach fo desgnng an optmal coodnaton contolle based on the adaptve fuzzy dynamc pogammng game theoy fo solvng the consensus poblem of mult-agent dffeental games was studed n [5] hee was a book [6] to study the ype- fuzzy logc n detal a elated study to desgn an adaptve slde mode contolle fo the nteval ype- fuzzy systems was epoted n [7] In 9 a moe geneal fom of the -S fuzzy model called the polynomal -S fuzzy model has been ntoduced n [8] an nteval ype polynomal fuzzy model was nvestgated n [9] hs model allows the system Manuscpt eceved Octobe 9 6; evsed Febuay 9 7; accepted June 7 7 (oespondng autho: Wen-June Wang) V P Vu W J Wang ae wth the Depatment of Electcal Engneeng Natonal ental Unvesty Jhong-L 3 awan RO (e-mal: phongvv@hcmuteeduvn ;wjwang@eencuedutw) H hen s wth the Depatment of Electcal Engneeng Natonal Unted Unvesty Maol 3663 awan RO(e-mal: chc@nuuedutw) J M Zuada s wth the Depatment of Electcal ompute Engneeng Unvesty of Lousvlle Lousvlle KY49 USA (e-mal: jacekzuada@lousvlleedu) matces contanng polynomal foms n ts entes nstead of only constant foms Wth the suppotng Sum-Of-Squae (SOS) ools n Matlab [] the polynomal -S fuzzy system can be consdeed as an effectve tool fo modelng nonlnea contol systems Recently a lage numbe of studes focused on the polynomal -S fuzzy systems such as contolle desgn obseve desgn stablty analyss [8]-[4] Fo example the stablty analyses fo the polynomal -S fuzzy systems by employng the multple Lyapunov functon swtchng Lyapunov functon wee nvestgated n [3] [4] espectvely Besdes the contolle desgn obseve-based contolle desgn fo the polynomal -S fuzzy system wee studed n many papes such as [8] [] -[] A non-pd contol desgn fo a polynomal -S fuzzy system by usng contol Lyapunov functon Songtag s fomula was poposed n [8] he obseve-based contolles fo the polynomal -S fuzzy system wth mmeasuable pemse vaables wee syntheszed n [] [3] In [] the authos poposed a new appoach fo stablty analyss contolle desgn fo a geneal polynomal -S fuzzy system n whch the polynomal Lyapunov functon cdate does not need to satsfy any constant Addtonally the contolle synthess fo dscete tme polynomal -S fuzzy systems wthout wth delay tme was developed n [9] [] espectvely Fom the above evew t becomes obvous that the polynomal -S fuzzy system has been pad attenton nceasngly t extends the study scope lage than the conventonal -S fuzzy system does fo nonlnea contol systems In a wde ange of eal-lfe pactcal systems all o some of state vaables ae mmeasuable o dffcult to obtan by usng the measuement devces due to both techncal economc ssues hese states howeve ae eally necessay fo system supevson contolle desgn heefoe the obseve desgn was taken notce nceasngly Regadng the obseve synthess fo the polynomal -S fuzzy systems vaous methods have been pesented n the past few yeas [5] -[8] In [5] a synthess of both contolle obseve fo polynomal -S fuzzy system was poposed to guaantee the system stablty the state estmaton smultaneously In addton the method fo desgnng obseve contolle smultaneously fo both contnuous dscete tme polynomal -S fuzzy systems wee pesented n [7] [8] espectvely
2 In pactce thee ae a lage numbe of systems affected by many knds of uncetantes he pesence of uncetantes n the system makes the desgn of the obseve contolle fo the system much moe dffcult In ou lteatue suvey a vaety of studes dealng wth uncetan poblems of -S fuzzy system wee found n [9]-[33] howeve thee ae only few papes concenng the polynomal -S fuzzy system wth uncetantes Recently the obust contolle synthess fo the polynomal -S fuzzy system wth uncetantes was nvestgated n [] [34] n whch the uncetantes n these papes must satsfy the nom-bounded constants Regadng the obseve desgn fo uncetan polynomal -S fuzzy system moe ecently the papes [8] [35] poposed the method to synthesze the contolle obseve smultaneously hese papes not only elmnated the nfluence of uncetantes but also guaanteed the state estmaton eos appoachng to zeo asymptotcally It should be noted that the uncetantes n the above papes must be unde some bounds If the uppe bound of uncetantes s unknown o only obseve wthout contolle s desgned the methods n [8] [35] wll not wok o addess ths shotcomng we popose n ths pape a new appoach based on the unknown nput method to synthesze the obseve fo the uncetan polynomal -S fuzzy system whee the bounded constants of uncetantes ae not gven the contolle s not needed to be desgned smultaneously to elmnate the nfluence of uncetantes Recently thee have been seveal papes poposed the method to desgn obseve based on the unknown nput method [36]-[38] fo -S fuzzy system unknown nput polynomal -S fuzzy system n [39] [4] Unfotunately the esults n [39] [4] have two lmtatons he fst s t s dffcult to fnd the feasble soluton fo the paamete matces to desgn the obseve he detals wll be explaned n Secton II he othe s the poposed method usng the common Lyapunov functon cdate that often leads to a much consevatve esult In ode to ovecome the above dsadvantages ths pape poposes a new fom of obseve uses a non-common Lyapunov functon [4]-[4] to deve the condtons fo the obseve synthess he pape s oganzed as follows In Secton II we descbe the consdeed polynomal fuzzy system model wth uncetantes pont out the man poblems to be esolved n ths study In Secton III the man theoems obseve synthess pocedues ae poposed In Secton IV two examples ae pesented to llustate the effectveness of the syntheszed obseve Fnally a concluson s pesented n Secton V Notatons: A denote the postve defnte matx A ; A denotes the tanspose of matx A ; A denotes the nvese of A ; A denotes the Mooe-Penose pseudo-nvese of A ( nm A A A) A he symbol denotes the set of n m matces; I denotes the dentty matx; the astesk (*) denotes the tansposed elements of the symmetc matx II SYSEM MODEL AND PROBLEM DESRIPION A System model Let us consde the nonlnea system pesented as follows x f ( x u ) (a) y x (b) whee f s the nonlnea functon ncludng possbly uncetantes x s the state vecto s the vecto of possbly tme-vayng paamete he equaton (b) s a lnea output equaton wth constant matx s the output vecto On the bass of the secto nonlneaty method [43] suppose the nonlnea system () can be epesented as the class I polynomal -S fuzzy system as follows [7]: Rule IF () t : s Q s () t s x ( A ( ) A ( )) x Q s ( B ( ) B ( )) u y HEN (a) y x (b) whee s s the vecto of measuable pemse vaables j= s) s the fuzzy set s the numbe of pemse vaables Q j ( = ; s the numbe of ules s () t n Suppose xt () s m the unavalable state vecto ut () s the nput vecto p yt () s the output It s noted that s the measuable vaable that could be a functon of extenal vaable output nn /o tme he polynomal matces A( ) yt () B( ) nm () t ae known polynomal matces of the states nputs espectvely Moeove A( ) B( ) ae the uncetantes of A ( ) B ( ) espectvely he oveall uncetan polynomal -S fuzzy system nfeed fom the plant ules of () s descbed below: x ( ) ( A ( ) A ( )) x ( B( ) B( )) u y x whee s w ( ) Q ( ) j j n (3) w( ) w ( ) w ( ) ( ) ( ) w( )
3 3 Remak : As pesented n [7] the polynomal -S fuzzy system s classfed nto thee types (class I class II class III) In ths pape we only consde the class I polynomal -S fuzzy system whch has the polynomal system matces depend on the measuable tme-vayng vaable () t Remak : If () t s a constant the system matces A( ) B ( ) become constant matces A B the polynomal -S fuzzy system () becomes the conventonal -S fuzzy system Remak 3: he uncetantes on () t A( ) B( ) depend t means that the uncetantes ae moe pactcal compaed to the uncetantes n [] [8] [34] whch ae only dependent on tme In addton the bound condtons of these uncetantes ae not gven Remak 4: A nonlnea system can be tansfomed to a polynomal -S fuzzy system of lass I by usng the secto nonlneaty method f the system matx nput matx of the polynomal -S fuzzy system contan only the measuable vaables that could be a functon of extenal vaable output /o tme If some un-avalable state B vaables ae nsde /o then these systems ae consdeed as a polynomal -S fuzzy system of lass II III lass II III ae moe complcated to be studed whch ae not consdeed n ths pape he polynomal -S fuzzy of class I whch s an extenson of the geneal -S fuzzy system can sgnfcantly educe the numbe of fuzzy ules fo pesentng the ognal nonlnea because the pemse vaable has been put nsde the system matces [7] A Poposton []: If p( x( t )) s a SOS then p( x( t )) can be ewtten as polynomal n yt () B n ql x t whee ql ( x) l p( x) ( ( )) xt () the SOS t mples that p( x) B Poblem descpton A s a heefoe when p( x( t )) s detemned as Suppose that when all o some state vaables xt () of the polynomal -S fuzzy system (3) ae unavalable t s necessay to synthesze an obseve to estmate these unavalable state vaables Hence ths pape ams to desgn an obseve fo the system (3) to guaantee the estmated state vaables appoachng to eal states As dscussed befoe [8] [35] dealt wth the poblem of obseve desgn fo uncetan polynomal -S fuzzy systems Howeve n ode to elmnate the nfluences of uncetantes estmate state vaables smultaneously the methods n [8] [35] desgned an obseve-based contolle to acheve ths objectve In addton the uppe bounds of uncetantes have to be gven n advance; othewse t s nfeasble to desgn the obseve In ode to ovecome these dawbacks n ths pape we popose the new appoach based on the unknown nput method to synthesze an obseve fo the uncetan polynomal -S fuzzy system (3) If the unknown nput obseve fom (obseve (7) n [4]) s consdeed z ( ) N ( ) z G ( ) u L ( ) y xˆ z Ey (4) It s noted that the matx E n (4) s a constant matx t s had to satsfy the condton ( P S) R (() n heoem of [4]) whee S=PE snce P S ae constant matces whle the matx s the polynomal matces R Due to the above analyses ths study tes to popose a new appoach to synthesze a specfc fom of the obseve fo the uncetan polynomal -S fuzzy system Befoe the man devaton the followng two assumptons ae needed Assumpton : Assume the matchng condtons A ( ) D( ) A ( ) B ( ) D( ) B ( ) ae satsfed whee D( ) nq s a full nomal column qn ank matx (see [45]-[47]) A( ) qm B( ) ae tme-vayng uncetan matces whch depend on () t Assumpton : he matces D( ) ae full ow nomal column anks espectvely the nomal ank of ( D( )) s equal to the nomal ank of D( ) Remak 5: he Assumpton s necessay to tansfom the uncetantes to unknown nputs the Assumpton s needed to guaantee the exstence of geneal solutons of matx equaton whch wll appea n the poof of heoem III OBSERVER SYNHESIS Fstly on the bass of the Assumpton the uncetan polynomal -S fuzzy system s tansfomed to the unknown nput polynomal -S fuzzy system as follows Based on the Assumpton let us defne A ( ) x B ( ) u whee q q () t () t ae consdeed the unknown nputs heefoe the system (3) can be ewtten as follows: x ( ) A ( ) x B ( ) u D( ) D( ) y x Let be substtuted nto (5) we obtan (5)
4 4 x ( ) A ( ) x B ( ) u D( ) y x (6) Now the uncetan polynomal -S fuzzy system (3) has been tansfomed to unknown nput polynomal -S fuzzy system (6) heefoe the obseve wll be syntheszed to estmate unavalable states of the system (6) athe than of the system (3) Re-consde the fom of obseve (4) but wth a polynomal matx E( ) as follows z ( )[ N ( ) x G ( ) u L ( ) y](7a) xˆ z E( ) y (7b) he s the estmaton of the state vaable s xt ˆ( ) the state vecto of the obseve Let us defne the estmaton eo xt () zt () e x xˆ (8) substtutng (7b) nto (8) yelds e x z E( ) y ( I E( ) ) x z M ( ) x z whee M( ) I E( ) omputng the devatve of estmaton eo M( ) e x M ( ) x z () t et () (9) n (9) yelds () M( ) Fom () t s clealy seen that the tem x s () t vey complcated because of the tems of dffeentaton heefoe ths pape poposes a new obseve fom as follows xˆ ( ( )) ( ( )) ˆ t N t x G ( ) u L ( ) y F( ) y () nn nm n p whee N ( ) G( ) L( ) n p F( ) ae polynomal matces to be detemned late xt ˆ( ) s the estmaton of the eal state vaable xt () Fom (6) we have y x ( )[ A ( ) x B ( ) u D( ) ] Fom (8) we have () e x xˆ (3) Substtutng (6) () nto (3) yelds e ( ) A ( ) x B ( ) u D( ) ( ) N ( ) xˆ G ( ) u (4) L ( ) y F( ) y ombnng () (4) the obtaned esult s e ( ) A ( ) x B ( ) u D( ) N ( ) xˆ G ( ) u L ( ) y F( )[ A ( ) x B ( ) u D( ) ] ( ) A ( ) x F( ) A ( ) x L ( ) x N ( ) xˆ B ( ) u F( ) B ( ) u G ( ) u D( ) F( ) D( ) ( ) ( A ( ) F( ) A ( ) L ( ) N ( )) x N ( ) e ( B ( ) F( ) B ( ) G ( )) u ( D( ) F( ) D( )) (5) In the followng poof of the heoem an assumpton s needed Assumpton 3 [4]: Assume that ( ) k whee s a constant k heoem : Unde Assumptons 3 the estmaton eo (8) wth the obseve () conveges to zeo asymptotcally f thee exst polynomal matces F( ) N ( ) L( ) G ( ) symmetc matx condtons hold wth = P k such that the followng A ( ) F( ) A ( ) L ( ) N ( ) (6) B ( ) F( ) B ( ) G ( ) (7) D( ) F( ) D( ) (8) v ( P I) v s SOS (9) k k j j k v ( P N ( ) P P N ( ) ( ) I) v s SOS whee v v () ae vectos wth appopate dmensons that do not depend on () t ( ) at Poof: If the condtons (6)-(8) of heoem hold then (5) becomes k
5 5 e ( ){ N ( ) e} () Select the non- common Lyapunov functon as follows V ( ) e Pe () It s noted that f the condton (9) holds t means that the symmetc akng the devatve of Lyapunov functon esults n P k k k V ( ) e P e ( )[ e Pe e Pe] (3) Substtutng () nto (3) on the bass of the Assumpton 3 poduces Lemma : Let A S P R be matces wth pope szes he followng two nequaltes ae equvalent: ) R A P PA A S SA R P S A S P S SA S S ) S : Poof of Lemma : *) ) mplcaton ): We pe-multply post-multply () wth I A I A I A espectvely whch yelds A S SA R P S A S I R A P PA P S SA S S A *) ) mplcaton ): Fom ) we have k k j k j V e P e ( ){ e N ( ) P e j k k k j e P N ( ) e} e P e ( ) e { N ( ) P P N ( )} e j j j j k k j k ( ) e { N ( ) P P N ( ) P } e (4) It can be seen fom (4) that f the condton () holds then Vt ( ) t means that the estmaton eo (8) appoaches zeo asymptotcally he poof s completed Remak 5: he tem postve ( ) ae used n heoem to guaantee k P s postve defne matx k Pk N ( ) Pj Pj N ( ) s negatve defne matx nstead of sem-postve sem-negatve defne In ode to synthesze the obseve () all condtons (6)-() must be solved to detemne the paametes N ( ) G ( ) L ( ) F( ) of the obseve () Howeve the condton () s a polynomal BMI (Blnea Matx Inequalty) whch cannot be solved by usng SOS OOL n Matlab theefoe we need to tansfom t nto the polynomal Lnea Matx Inequaltes (LMIs) he followng heoem wll be wth polynomal LMI mn Lemma [44]: hee ae two matces A wth m n kn B suppose that BA A B hen any matx of the fom X BA Y( I AA ) s a soluton of XA B whee km Y s an abtay matx A s defned as ( A A A) A whch s the Mooe-Penose pseudo-nvese of A ( R A P PA) ( A S A S ) ( SA SA) ( A S A A S A) ( A SA A SA) A S SA R PA SA A S A A P A S A SA A S A A SA We can ewte (*) n the fom of matx as follows I A A S SA R P S A S I P S SA S S A hat leads to A S SA R P S A S P S SA S S heefoe ) ) ae equvalent he poof s completed heoem : Unde Assumptons 3 the estmaton eo (8) wth the obseve () conveges to zeo asymptotcally f thee exst polynomal matces F( ) N ( ) L( ) G P ( ) K( ) X( ) Q( ) symmetc matx such that the followng condtons hold fo = v ( P I) v s SOS (5) () (*) k v () ( ) I v s SOS j X ( ) X ( ) (6) (*)
6 6 () k k k k P ( A ( ) U ( ) A ( )) X ( ) ( V ( ) A ( )) K ( ) Q ( ) X ( )( A ( ) U ( ) A ( )) K( )( V ( ) A ( )) Q ( ) (7) () P X ( ) X ( )( A ( ) U( ) A ( )) j j K( )( V ( ) A( )) Q( ) (8) whee ae vectos wth appopate dmensons that v v do not depend on () t ( ( t)) at ( ( ( ))) (( ( ( ))) D t D t ( D( ))) ( D( )) U( ) D( )( D( )) (9) V( ) ( I ( D( ))( D( )) ) (3) K( ) X ( ) Y( ) (3) Q ( ) X( ) L ( ) (3) Moeove the paametes of obseve () ae computed as follows F( ) U( ) Y( ) V( ) (33) G ( ) B ( ) F( ) B ( ) (34) ( ( )) ( ( ))Q ( ( )) L t X t t (35) N ( ) A ( ) F( ) A ( ) L ( ) (36) Poof: Fom the condton () of heoem t can be nfeed that k Pk N ( ) Pj Pj N ( ) (37) k Employng the Lemma fo (37) wth slack vaable X( ) one obtans () (*) k () j X ( ) X ( ) whee () k k k k (38) P N ( ) X ( ) X ( ) N ( ) (39) P X ( ) X ( ) N ( ) (4) () j j Fom (8) we have F( ) D( ) D( ) (4) On the bass of the Lemma the geneal soluton of (4) s F( ) D( )( D( )) whee Y ( )( I ( D( ))( D( )) ) ( ( ( ))) (( ( ( ))) D t D t ( D( ))) ( D( )) (4) It s noted that the exstence of the geneal soluton (4) s guaanteed f only f the matces satsfy the Assumpton Let s denote D( (t)) U( ) D( )( D( )) (43) V( ) ( I ( D( ))( D( )) ) (44) Substtutng (43) (44) nto (4) yelds F( ) U( ) Y( ) V( ) (45) Fom (6) (45) one obtans N ( ) A ( ) ( U( ) Y( ) V ( )) A ( ) L ( ) A ( ) ( U( ) A ( )) ( Y( ) V ( ) A ( )) L ( ) Substtutng (46) nto (39) the obtaned esult s () k k k k P ( A ( ) ( U ( ) A ( )) ( Y ( ) V ( ) A ( )) L ( ) ) X ( ) X ( )( A ( ) ( U ( ) A ( )) ( Y ( ) V ( ) A ( )) L ( ) ) k P ( A ( ) U ( ) A ( )) X ( ) k k (46) ( V ( ) A ( )) Y ( ) X ( ) L ( ) X ( ) X ( )( A ( ) U ( ) A ( )) X ( ) Y ( )( V ( ) A ( )) X ( ) L ( ) Substtutng (46) nto (4) we have P X ( ) X ( )( A ( ) ( U( ) A ( )) () j j ( Y( ) V ( ) A ( )) L ( ) ) P X ( ) X ( )( A ( ) U( ) A ( )) j X ( ) Y( )( V ( ) A ( )) X ( ) L ( ) Let us defne (47) (48) K( ) X ( ) Y( ) (49) Q ( ) X( ) L ( ) (5) Substtutng (49) (5) nto (47) (48) we obtan
7 7 () k k k k P ( A ( ) U ( ) A ( )) X ( ) ( V ( ) A ( )) K ( Q ( ) X ( )( A ( ) U ( ) A ( )) K( )( V ( ) A ( )) Q ( ) (5) () P X ( ) X ( )( A ( ) U( ) A ( )) j j K( )( V ( ) A ( )) Q ( ) (5) Fom (5) (5) t s seen that (38) becomes () (*) k () j X ( ) X ( ) whee () k () j (53) ae expessed as (5) (5) espectvely It s seen that (53) s equvalent to (6) of heoem t s a polynomal LMI It means that the polynomal BMI () has been successfully tansfomed nto polynomal LMI n heoem he poof s completed It s noted that the polynomal LMI n heoem can be solved easly by usng SOS OOL of Matlab [46] he bef pocedue fo the obseve () synthess s pesented below: Step : heck the matces D( ) satsfy the Assumpton o not If yes we go to the next step If not ths method does not wok fo ths case Step : Fom (9) (3) U( ) V( ) ae obtaned Step 3: Resolve (5) (6) to obtan Q( ) then fom (3) we obtan Y( ) P j K( ) X( ) Step 4: he matces F( ) G( ) L( ) N ( ) ae obtaned fom (33)-(36) espectvely Step 5: he obseve () s syntheszed IV ILLUSRAIVE EXAMPLES In ths secton two examples ae llustated to pove the effectveness of the poposed method Example s a numecal example Example s an applcaton fo Inveted Pendulum A Example onsde a nonlnea system as follows Let the system (54) be tansfomed nto a polynomal -S fuzzy system whee of polynomal -S fuzzy system s the output y(t) hen () t x ( )[ A x B u] (55) y x 3 A y A y y B B cos( x) cos( x) ( ) ; ( ) We can see that sn( x) sn( x) ( ) x ( ) x then we assume 4 Suppose the system (55) s nfluenced by the uncetantes the bounded constants of these uncetantes ae unknown he system (55) s expessed n the followng fom x ( )[( A A ) x ( B B ) u] y x (56) whee cos / y sn( y ) / y A 5cos 5sn sn / y 4cos / y A 5sn 6cos cos( y ) / y sn( y ) / y B B 55cos( y ) 5sn( y ) ansfomng system (56) nto the unknown nput system yelds x ( )[ A x B u D ] (57) y x whee 3 x cos( x ) x x u x x x x y x (54) / y Dy ( ) 5 Step : We can see that D( y) ae full ow column anks nomal ank( D( (t))) nomal ank( D( ) thus the Assumpton s satsfed
8 8 Step : Fom (9) (3) U y /4 V ; Step 3: Resolve the constant (5) (6) of heoem usng the SOS OOL of Matlab We can obtan the values below P P K Y X y 6543 y35 Q y 59 y y y377 Q y 3987 y 34 Step 4 Step 5: he matx F( ) s obtaned fom (33) We obtan N ( ) fom (36) L( ) fom (35) G ( ) fom (34) y 463 y N( y) N( y) L y y y y / y 436 y y/ 4 57 y y y y y y y L G 4 y /4 ( G y) 4 y / 4 F y / y 435 y y y Hee we used Smulnk tools to cay out the smulaton he ntal states of the system x() -5 3 the estmated states ae xˆ() -5 5 he nput used fo smulaton s u sn Fg Real state x () t estmated state xˆ () t Fg Real state x () t estmated state xˆ () t Estmaton eo e () t Estmaton eo e () t Fg 3 Estmaton eos e () t e () t
9 9 Fgues -3 show the smulaton esults of the numecal example n whch the system (56) s petubed by the uncetantes A ( y) A ( y) B ( y) B ( y) Fgues depct the states the estmated sgnals he estmaton eo s llustated n Fg 3 It can be seen fom these fgues that the estmated states can appoach eal states asymptotcally Hence the poposed method s successful n syntheszng obseve fo polynomal -S fuzzy system wth uncetantes x x Remak 6: It s noted that f we use geneal -S fuzzy system to epesent the nonlnea system (54) both must cos( x ) be lneazed the local bound ange of must be gven hen thee wll be fou fuzzy ules n the -S fuzzy system Howeve f let a polynomal -S fuzzy system be pesent the ognal nonlnea system x wll be putted n the system matces theefoe the bound ange of does not need to know the numbe of fuzzy ules wll be educed to two It means that the polynomal -S fuzzy system wll epesent the system (54) be moe exactly ove global egon x x x Mc 8kg L m ae the mass of Pendulum at the length of the pendulum espectvely; a / ( m M ) p c ut () the contol nput foce mposed on the cat 7 7 x () t 8 8 In ode to educe computatonal buden the tem sn( x ) s x tan( x ) tx Applyng nonlnea secto to lneaze ths system the nonlnea system (58) s epesented as the followng polynomal -S fuzzy system It s noted that ( ) x y x t x x theefoe the esult of the nonlnea system can be expessed n the fom of (3) wth beng the output y(t) s 8578 t 5534 x ( x ) A x B u y x() t s () t (59) B Example In ths example we consde a pactcal dynamc model of an Inveted Pendulum on a cat [] he system s depcted n the followng fgue whee A a A a B f mn a B fmaxa fmn 5 fmax 7647 a f ( gt am Ly s ) a f ( gt am Ly s ) mn p he pemse vaables max p Fg 4 Inveted Pendulum on a cat he nonlnea equaton of the Inveted Pendulum on a cat s expessed as follows x x g sn( x ) am Lx sn( x )cos( x ) p () 4 L / 3 ampl cos ( x ) x t a cos( x ) u 4 L / 3 ampl cos ( x ) whee (58) x x x s a vecto of states s the angle (n adans) s the angula velocty m kg p ( x ) f ( x ) f max f mn f max cos( x ) f ( x ) 4 L / 3 am Lcos ( x ) p ( x ) ( x ) ; Suppose the (59) ae affect by the followng uncetantes then x ( x ) ( A A ) x ( B B ) u y x() t (6) y sn(y ) y cos A 55sn 6cos y cos y sn A 55cos sn
10 y cos( y ) B 5cos( y ) y sn( y ) B 5sn( y ) G (7767 y ) / 5 ansfom (6) nto unknown nput system wth y 7 7 Dy ( ) Wth x () t n ths pape we assume 5 Step : It s seen that the matces ae full ow column anks espectvely nomal ank( D( (t))) nomal ank( D( ) theefoe the Assumpton s satsfed Step : he matces ae calculated: U V D( y) y 8 y5537 L 3 6 y y y y357 L 3 63 y 4865 y Afte obtanng all paametes the obseve () s constucted he smulaton esults of the fuzzy obseve fo the system n Example wth nput u sn ntal values of the states x() 7*p/8 estmated states xˆ() -35*p/8 ae llustated as follows y /5 U V Step 3: he matces X ( y) P Q ( y) ae obtaned as follows K( y) Y( y) P P 8 Y K X( y) y 3 y 53 Q y 469 y y 985 y 53 Q 4 7 y 88 y 3 4 Fg 5 Real state x () t estmated state xˆ () t Step 4 Step 5: he paametes N ( y ) L ( y) ae computed G F he matces N N ( ) y ae expessed n (6) (6) espectvely y /5 (6 y ) / 5 F G Fg 6 Real state x () t estmated state xˆ () t he smulaton esults of the obseve synthess fo the pactcal dynamc system of Inveted Pendulum on a at whch s affected by uncetantes ae llustated n Fgs 5-7 Obvously Fg 5 Fg 6 show that estmaton states ˆx N 4 ( y ((447 y ) 79496)) / 5 893y 8 y y 9397 y 999 (6) N 8 ( y ((53 y ) 68645)) / y 4559 y y 48 y 9999 (6)
11 Estmaton eo e () t Estmaton eo e () t Estmaton eo e () t ˆx appoach asymptotcally to eal states x x espectvely In Fg 7 t s clealy seen that the estmaton eos convege to zeo asymptotcally e e Remak 7: ( ) k n Assumpton 3 s k k used n the above two examples Howeve n ths study the bound ange of some o all state vaables ae not known the bound of the uncetantes s not known ethe; hence the uppe bounds ae dffcult to estmate heefoe n ths study the values of n Example ae selected by tal eo If the chosen make the obseve synthess be feasble the smulaton s successful then the syntheszed obseve s effectve If the chosen ethe make the obseve synthess be not feasble o the smulaton s not successful we need to choose anothe couple Based on ou expeence f the feasble obseve s /o not obtaned we may decease to desgn t agan; howeve f the obseve synthess s feasble but the smulaton s not successful we may ncease We have to admt that tal eo method s not elable fo the obseve synthess t should be esolved n the futue wok /o Remak 8: It s woth notng that we assume that the uppe bounds of the uncetantes n Example Example ae unavalable theefoe the method n [] [8] wll fal to desgn obseve fo the system (56) (6) By usng the poposed method wth a new fom of the obseve () the obseve has been syntheszed successfully fo the uncetan polynomal -S fuzzy system n whch the bounded constants ae unknown the contolle dd not need to be desgned togethe wth an obseve fo the pupose of elmnatng the effects of uncetantes V ONLUSION hs pape has poposed a new appoach based on the unknown nput method to synthesze the obseve fo the uncetan polynomal -S fuzzy system On the bass of non-common Lyanpunov functon SOS technque two man theoems whch contan the condtons fo obseve Fg 7 Estmaton eos e () t e () t synthess have been deved hese condtons ae solved easly by usng SOS OOL of Matlab Fnally two examples have demonstated to pesent the effectveness of the poposed method he man chaactestcs of ths pape ae as follows () hee ae no uppe bound lmts fo uncetantes () he obseve synthess can be completed ndependently wthout desgnng contolle togethe () he obseve fom s new s notably completely dffeent fom othe exstng tadtonal fom of obseves AKNOWLEDGMEN hs wok was suppoted by the Gant MOS4--E-8-54-MY3 fom the Mnsty of Scence echnology of awan the coespondng autho D W J Wang completed ths wok when he was the vstng schola n the Unvesty of Lousvlle KY wth the Gant MOS 5-98-I-8-7 REFERENES [] akag M Sugeno Fuzzy dentfcaton of systems ts applcaton to modelng contol IEEE ans Syst Man yben vol 5 no pp [] K anaka M Sugeno Stablty analyss desgn of fuzzy contol systems Fuzzy Sets Syst vol 45 no pp Jan 99 [3] H G Zhang Y B Quan Modelng dentfcaton contol of a class of nonlnea systems IEEE ans Fuzzy Syst vol 9 no pp [4] H G Zhang D R Lu Fuzzy modellng fuzzy contol Bkhause Boston 6 [5] H G Zhang J L Zhang G H Yang Y H Luo Leade-based optmal coodnaton contol fo the consensus poblem of multagent dffeental games va fuzzy adaptve dynamc pogammng IEEE ans Fuzzy Syst vol 3 no pp [6] O astllo P Meln ype- fuzzy logc: theoy applcatons vol 3 Spnge-Velag Beln Hedelbeg 8 [7] H Y L J H Wang H K Lam Q Zhou H P Du Adaptve sldng mode contol fo nteval type- fuzzy systems IEEE ans Syst Man ybe:syst vol 46 no pp [8] K anaka H Yoshda H Ohtake Hua O Wang A sum-of-squaes appoach to modelng contol of nonlnea dynamcal systems wth polynomal fuzzy systems IEEE ans Fuzzy Syst vol 7 no 4 pp [9] B Xao HK Lam H Y L Stablzaton of nteval type- polynomal-fuzzy-model-based contol systems IEEE ans Fuzzy Syst vol 5 no pp [] A Papachstodoulou J Andeson G Valmobda S Pajna P Sele P A Palo SOSOOLS: Sum of Squaes Optmzaton oolbox fo MALAB Veson 3 6
12 [] K anaka H Ohtake H O Wang Guaanteed cost contol of polynomal fuzzy systems va a sum of squaes appoach IEEE ans Syst Man yben B yben vol 39 no pp [] M Naman H K Lam SOS-based stablty analyss of polynomal fuzzy-model-based contol systems va polynomal membeshp functons IEEE ans Fuzzy Syst vol 8 no 5 pp Oct [3] H K Lam M Naman H Y L H H Lu Stablty analyss of polynomal-fuzzy-model-based contol systems usng swtchng polynomal Lyapunov functon IEEE ans Fuzzy Syst vol no 5 pp [4] K Guelton N Manamann Duong D L Koumba-Emanwe Sum-of-squaes stablty analyss of akag-sugeno systems based on multple polynomal Lyapunov functons Intenatonal Jounal of Fuzzy Systems vol 5 no pp -8 Mach 3 [5] G R Yu L W Huang Y heng he SOS-based extended desgn of polynomal fuzzy contol the IEEE Intenatonal onfeence on Systems Man ybenetcs Octobe Seoul Koea pp [6] H K Lam S H sa Stablty analyss of polynomal-fuzzy-model-based contol systems wth msmatched pemse membeshp functons IEEE ans Fuzzy Syst vol no pp [7] J L Ptach A Sala V Ano losed-fom estmates of the doman of attacton fo nonlnea systems va fuzzy-polynomal models IEEE ans Fuzzy Syst vol 44 no 4 pp [8] R Fuqon Y J hen M anaka K anaka H O Wang An SOS-based contol Lyapunov functon desgn fo polynomal fuzzy contol of nonlnea systems IEEE ans Fuzzy Syst vol 3 no 9 pp -3 4 [9] Y J hen M anaka K anaka H Ohtake H O Wang Dscete polynomal fuzzy systems contol IE ontol heoy Appl vol 8 no 4 pp [] Y Y Wang H G Zhang Y Wang J Y Zhang Stablty analyss contolle desgn of dscete-tme polynomal fuzzy tme-vayng delay systems Jounal of the Fankln Insttute vol 35 pp [] Lu H K Lam Desgn of polynomal fuzzy obseve-contolle wth sampled-output measuements fo nonlnea systems consdeng unmeasuable pemse vaables IEEE ans Fuzzy Systvol 3 no 6 pp [] H K Lam L G Wu J Lam wo-step stablty analyss fo geneal polynomal-fuzzy-model-based contol systems IEEE ans Fuzzy Syst vol 3 no 3 pp [3] Lu H K Lam X J Ban X D Zhao Desgn of polynomal fuzzy obseve-contolle wth membeshp functon usng unmeasuable pemse vaables fo nonlnea systems Infomaton Scences vol pp [4] H G Han J Y hen H R Kam State dstubance obseves-based polynomal fuzzy contolle Infomaton Scences vol pp [5] K anaka H Ohtake Seo H O Wang An SOS-based obseve desgn fo polynomal fuzzy systems the Amecan ontol onfeence on O'Faell Steet San Fancsco A USA June 9 - July pp [6] K anaka H Ohtake M Wada H O Wang Y J hen Polynomal fuzzy obseve desgn: a sum of squaes appoach the Jont 48th IEEE onfeence on Decson ontol 8th hnese ontol onfeence Shangha PR hna Dec 9 pp [7] K anaka H Ohtake Seo M anaka HO Wang Polynomal fuzzy obseve desgns: a sum-of-squaes appoach IEEE ans Syst Man yben Pat B: yben vol 4 no 5 pp Oct [8] Y Y Wang H G Zhang J Y Zhang Y Wang An SOS-based obseve desgn fo dscete-tme polynomal fuzzy systems Int J Fuzzy Syst vol7 no pp [9] V Dang W J Wang L Luoh et al Adaptve obseve desgn fo the uncetan akag Sugeno fuzzy system wth output dstubance IE ontol heoy Appl vol 6 no pp [3] W J Wang V P Vu W hang H Sun S J Yeh A synthess of obseve-based contolle fo stablzng uncetan -S fuzzy systems J Intell Fuzzy Syst vol3 pp [3] H H ho LMI-based nonlnea fuzzy obseve-contolle desgn fo uncetan MIMO nonlnea system IEEE ans Fuzzy Syst vol 5 no7 pp [3] A Golab M Behesht M H Aseman H obust fuzzy dynamc obseve-based contolle fo uncetan akag Sugeno fuzzy systems IE ontol heoy Appl vol 6 no pp [33] V Dang W J Wang H Huang et al Obseve synthess fo the S fuzzy system wth uncetanty output dstubance J Intell Fuzzy Syst vol no 6 pp [34] H S Km J B Pak Y H Joo Robust stablzaton condton fo a polynomal fuzzy system wth paametc uncetantes the th Intenatonal onfeence on ontol Automaton Systems Jeju Isl Koea Oct pp 7- [35] K anaka M anaka Y J hen H O Wang A new sum-of-squaes desgn famewok fo obust contol of polynomal fuzzy systems wth uncetantes IEEE ans Fuzzy Syst vol 4 no pp 94-6 [36] V P Vu W J Wang Obseve synthess fo uncetan akag Sugeno fuzzy systems wth multple output matces IE ontol heoy Appl vol no pp [37] S J Yeh W hang WJ Wang Unknown nput based obseve synthess fo uncetan S fuzzy systems IE ontol heoy Appl vol 9 no7 pp [38] V P Vu W J Wang "Obseve desgn fo a dscete-tme -S fuzzy system wth uncetantes" the 5 IEEE Intenatonal onfeence on Automaton Scence Engneeng (ASE) Gothenbug Sweden Aug 5 pp 6-67 [39] A hban M hadl M M Belhaouane N B Baek Polynomal obseve desgn fo unknown nputs polynomal fuzzy systems: A Sum of Squaes appoach the 53d IEEE onfeence on Decson ontol Los Angeles alfona USA Dec 4 pp [4] A hban M hadl N B Baek A sum of squaes appoach fo polynomal fuzzy obseve desgn fo polynomal fuzzy systems wth unknown nputs Intenatonal Jounal of ontol Automaton Systems vol 4 no pp [4] K anaka Ho H O Wang A multple Lyapunov functon appoach to stablzaton of fuzzy contol systems IEEE ans Fuzzy Syst vol no 4 pp [4] S H Km P G Pak Obseve-based elaxed H contol fo fuzzy systems usng a multple Lyapunov functon IEEE ans Fuzzy Syst vol 7 no pp [43] K anaka H O Wang Fuzzy ontol Systems Desgn Analyss: A Lnea Matx Inequalty Appoach Hoboken NJ:Wley [44] A J Laub Matx Analyss fo Scentsts Engnees Sam 5 [45] P J Antsakls A N Mchel Lnea Systems chapte 7 Bkhause Boston 6 [46] Polynomal oolbox 3 Manual fo Matlab PolyX Ltd Septembe 9 [47] WS Levne he contol h book vol Jaco Publshng House 999 Van-Phong Vu eceved the BS degee n electcal engneeng fom Ha No Unvesty of Scences echnology Vetnam n 7 the MS degee n electcal engneeng fom Southen awan Unvesty of Scences echnology awan n Snce he has been a lectue at Ho h Mnh cty Unvesty of Educaton echnology Vetnam He s cuently pusung the PhD degee n electcal engneeng at Natonal ental Unvesty Hs eseach nteests ae fuzzy systems ntellgent contol obseve contolle desgn fo uncetan system
13 3 Wen-June Wang eceved the BS degee n the Depatment of ontol Engneeng fom Natonal hao-ung Unvesty Hsn-hu awan n 98; MS degee n the Depatment of Electcal Engneeng fom atung Unvesty ape awan n 984 Moeove he eceved the PhD degee n the Insttute of Electoncs fom Natonal hao-ung Unvesty of awan n 987 Pof Wang s pesently a ha Pofesso of Depatment of Electcal Engneeng He was the Dean of ollege of Electcal Engneeng ompute Scence Natonal ental Unvesty hung-l ty awan He was also a ha Pofesso the Dean of the Reseach Development Offce of Natonal ape Unvesty of echnology ape awan n 7~9 In 5~7 he was the Dean of ollege of Scence echnology Natonal h-nan Unvesty Pul Nanou awan Moeove Pof Wang obtaned the hono of IEEE Fellow n 8 IFSA Fellow n 7 Pof Wang has authoed o coauthoed ove 6 efeeed jounal papes 6 confeence papes n the aeas of fuzzy systems theoems obust nonlnea contol n lage scale systems neual netwoks etc Hs most sgnfcant contbutons ae the desgn of fuzzy systems the development of obotcs Hs othe eseach nteests nclude the aeas of obot contol neual netwoks patten ecognton etc echnology Intellgent omputng the edto of Spnge s Natual omputng Book Sees He was elected as the Pesdent of the IEEE omputatonal Intellgence Socety n 4-5 He now chas the IEEE AB Peodcals ommttee (- ) the IEEE AB Peodcals Revew ommttee (-3) a Lfe Fellow of the IEEE Hsang-heh hen eceved hs BS degee n engneeng scence fom the Natonal heng Kung Unvesty awan n hs MS PhD degees n electcal engneeng fom the Natonal ental Unvesty aoyuan awan n 5 9 Snce Aug 6 he joned the faculty of the Depatment of Electcal Engneeng Natonal Unted Unvesty Maol awan whee he s cuently an assstant pofesso Hs eseach nteests nclude mage pocessng compute vson atfcal ntellgence obotcs Jacek M Zuada eceved the MS PhD degees n electcal engneeng fom the echncal Unvesty of Gdansk Pol n espectvely He has publshed ove 4 joual confeence papes n vaous aeas Fom 998 to 3 he was the edto-n-chef of the IEEE ansactons on Neual Netwoks He was an assocate edto of the IEEE ansactons on cuts Systems Pat I Pat II seved on the edtoal boad of the Poceedngs of IEEE He s an assocate edto of Neual Netwoks Neuocomputng Schedae Infomatcae the Intenatonal Jounal of Appled Mathematcs ompute Scence the advsoy edto of the Intenatonal Jounal of Infomaton
FUZZY CONTROL VIA IMPERFECT PREMISE MATCHING APPROACH FOR DISCRETE TAKAGI-SUGENO FUZZY SYSTEMS WITH MULTIPLICATIVE NOISES
Jounal of Mane Scence echnology Vol. 4 No.5 pp. 949-957 (6) 949 DOI:.69/JMS-6-54- FUZZY CONROL VIA IMPERFEC PREMISE MACHING APPROACH FOR DISCREE AKAGI-SUGENO FUZZY SYSEMS WIH MULIPLICAIVE NOISES Wen-Je
More informationObserver Design for Takagi-Sugeno Descriptor System with Lipschitz Constraints
Intenatonal Jounal of Instumentaton and Contol Systems (IJICS) Vol., No., Apl Obseve Desgn fo akag-sugeno Descpto System wth Lpschtz Constants Klan Ilhem,Jab Dalel, Bel Hadj Al Saloua and Abdelkm Mohamed
More informationNew Condition of Stabilization of Uncertain Continuous Takagi-Sugeno Fuzzy System based on Fuzzy Lyapunov Function
I.J. Intellgent Systems and Applcatons 4 9-5 Publshed Onlne Apl n MCS (http://www.mecs-pess.og/) DOI:.585/sa..4. New Condton of Stablzaton of Uncetan Contnuous aag-sugeno Fuzzy System based on Fuzzy Lyapunov
More informationIf there are k binding constraints at x then re-label these constraints so that they are the first k constraints.
Mathematcal Foundatons -1- Constaned Optmzaton Constaned Optmzaton Ma{ f ( ) X} whee X {, h ( ), 1,, m} Necessay condtons fo to be a soluton to ths mamzaton poblem Mathematcally, f ag Ma{ f ( ) X}, then
More informationState Feedback Controller Design via Takagi- Sugeno Fuzzy Model : LMI Approach
State Feedback Contolle Desgn va akag- Sugeno Fuzzy Model : LMI Appoach F. Khabe, K. Zeha, and A. Hamzaou Abstact In ths pape, we ntoduce a obust state feedback contolle desgn usng Lnea Matx Inequaltes
More informationMultistage Median Ranked Set Sampling for Estimating the Population Median
Jounal of Mathematcs and Statstcs 3 (: 58-64 007 ISSN 549-3644 007 Scence Publcatons Multstage Medan Ranked Set Samplng fo Estmatng the Populaton Medan Abdul Azz Jeman Ame Al-Oma and Kamaulzaman Ibahm
More informationSet of square-integrable function 2 L : function space F
Set of squae-ntegable functon L : functon space F Motvaton: In ou pevous dscussons we have seen that fo fee patcles wave equatons (Helmholt o Schödnge) can be expessed n tems of egenvalue equatons. H E,
More informationDistinct 8-QAM+ Perfect Arrays Fanxin Zeng 1, a, Zhenyu Zhang 2,1, b, Linjie Qian 1, c
nd Intenatonal Confeence on Electcal Compute Engneeng and Electoncs (ICECEE 15) Dstnct 8-QAM+ Pefect Aays Fanxn Zeng 1 a Zhenyu Zhang 1 b Lnje Qan 1 c 1 Chongqng Key Laboatoy of Emegency Communcaton Chongqng
More informationAdvanced Robust PDC Fuzzy Control of Nonlinear Systems
Advanced obust PDC Fuzzy Contol of Nonlnea Systems M Polanský Abstact hs pape ntoduces a new method called APDC (Advanced obust Paallel Dstbuted Compensaton) fo automatc contol of nonlnea systems hs method
More informationStable Model Predictive Control Based on TS Fuzzy Model with Application to Boiler-turbine Coordinated System
5th IEEE Confeence on Decson and Contol and Euopean Contol Confeence (CDC-ECC) Olando, FL, USA, Decembe -5, Stable Model Pedctve Contol Based on S Fuy Model wth Applcaton to Bole-tubne Coodnated System
More informationFuzzy Controller Design for Markovian Jump Nonlinear Systems
72 Intenatonal Jounal of Juxang Contol Dong Automaton and Guang-Hong and Systems Yang vol. 5 no. 6 pp. 72-77 Decembe 27 Fuzzy Contolle Desgn fo Maovan Jump Nonlnea Systems Juxang Dong and Guang-Hong Yang*
More informationON THE FRESNEL SINE INTEGRAL AND THE CONVOLUTION
IJMMS 3:37, 37 333 PII. S16117131151 http://jmms.hndaw.com Hndaw Publshng Cop. ON THE FRESNEL SINE INTEGRAL AND THE CONVOLUTION ADEM KILIÇMAN Receved 19 Novembe and n evsed fom 7 Mach 3 The Fesnel sne
More informationKhintchine-Type Inequalities and Their Applications in Optimization
Khntchne-Type Inequaltes and The Applcatons n Optmzaton Anthony Man-Cho So Depatment of Systems Engneeng & Engneeng Management The Chnese Unvesty of Hong Kong ISDS-Kolloquum Unvestaet Wen 29 June 2009
More information3. A Review of Some Existing AW (BT, CT) Algorithms
3. A Revew of Some Exstng AW (BT, CT) Algothms In ths secton, some typcal ant-wndp algothms wll be descbed. As the soltons fo bmpless and condtoned tansfe ae smla to those fo ant-wndp, the pesented algothms
More information8 Baire Category Theorem and Uniform Boundedness
8 Bae Categoy Theoem and Unfom Boundedness Pncple 8.1 Bae s Categoy Theoem Valdty of many esults n analyss depends on the completeness popety. Ths popety addesses the nadequacy of the system of atonal
More informationP 365. r r r )...(1 365
SCIENCE WORLD JOURNAL VOL (NO4) 008 www.scecncewoldounal.og ISSN 597-64 SHORT COMMUNICATION ANALYSING THE APPROXIMATION MODEL TO BIRTHDAY PROBLEM *CHOJI, D.N. & DEME, A.C. Depatment of Mathematcs Unvesty
More informationAn Approach to Inverse Fuzzy Arithmetic
An Appoach to Invese Fuzzy Athmetc Mchael Hanss Insttute A of Mechancs, Unvesty of Stuttgat Stuttgat, Gemany mhanss@mechaun-stuttgatde Abstact A novel appoach of nvese fuzzy athmetc s ntoduced to successfully
More informationAdaptive Fuzzy Dynamic Surface Control for a Class of Perturbed Nonlinear Time-varying Delay Systems with Unknown Dead-zone
Intenatonal Jounal of Automaton and Computng 95, Octobe 0, 545-554 DOI: 0.007/s633-0-0678-5 Adaptve Fuzzy Dynamc Suface Contol fo a Class of Petubed Nonlnea Tme-vayng Delay Systems wth Unknown Dead-zone
More informationGenerating Functions, Weighted and Non-Weighted Sums for Powers of Second-Order Recurrence Sequences
Geneatng Functons, Weghted and Non-Weghted Sums fo Powes of Second-Ode Recuence Sequences Pantelmon Stăncă Aubun Unvesty Montgomey, Depatment of Mathematcs Montgomey, AL 3614-403, USA e-mal: stanca@studel.aum.edu
More informationExact Simplification of Support Vector Solutions
Jounal of Machne Leanng Reseach 2 (200) 293-297 Submtted 3/0; Publshed 2/0 Exact Smplfcaton of Suppot Vecto Solutons Tom Downs TD@ITEE.UQ.EDU.AU School of Infomaton Technology and Electcal Engneeng Unvesty
More informationExperimental study on parameter choices in norm-r support vector regression machines with noisy input
Soft Comput 006) 0: 9 3 DOI 0.007/s00500-005-0474-z ORIGINAL PAPER S. Wang J. Zhu F. L. Chung Hu Dewen Expemental study on paamete choces n nom- suppot vecto egesson machnes wth nosy nput Publshed onlne:
More informationChapter Fifiteen. Surfaces Revisited
Chapte Ffteen ufaces Revsted 15.1 Vecto Descpton of ufaces We look now at the vey specal case of functons : D R 3, whee D R s a nce subset of the plane. We suppose s a nce functon. As the pont ( s, t)
More informationAPPLICATIONS OF SEMIGENERALIZED -CLOSED SETS
Intenatonal Jounal of Mathematcal Engneeng Scence ISSN : 22776982 Volume Issue 4 (Apl 202) http://www.mes.com/ https://stes.google.com/ste/mesounal/ APPLICATIONS OF SEMIGENERALIZED CLOSED SETS G.SHANMUGAM,
More informationMachine Learning 4771
Machne Leanng 4771 Instucto: Tony Jebaa Topc 6 Revew: Suppot Vecto Machnes Pmal & Dual Soluton Non-sepaable SVMs Kenels SVM Demo Revew: SVM Suppot vecto machnes ae (n the smplest case) lnea classfes that
More informationPhysics 2A Chapter 11 - Universal Gravitation Fall 2017
Physcs A Chapte - Unvesal Gavtaton Fall 07 hese notes ae ve pages. A quck summay: he text boxes n the notes contan the esults that wll compse the toolbox o Chapte. hee ae thee sectons: the law o gavtaton,
More informationOn Maneuvering Target Tracking with Online Observed Colored Glint Noise Parameter Estimation
Wold Academy of Scence, Engneeng and Technology 6 7 On Maneuveng Taget Tacng wth Onlne Obseved Coloed Glnt Nose Paamete Estmaton M. A. Masnad-Sha, and S. A. Banan Abstact In ths pape a compehensve algothm
More informationOptimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time
Intenatonal Jounal of ompute Applcatons (5 ) Volume 44 No, Apl Optmal System fo Wam Standby omponents n the esence of Standby Swtchng Falues, Two Types of Falues and Geneal Repa Tme Mohamed Salah EL-Shebeny
More informationUNIT10 PLANE OF REGRESSION
UIT0 PLAE OF REGRESSIO Plane of Regesson Stuctue 0. Intoducton Ojectves 0. Yule s otaton 0. Plane of Regesson fo thee Vaales 0.4 Popetes of Resduals 0.5 Vaance of the Resduals 0.6 Summay 0.7 Solutons /
More informationIntegral Vector Operations and Related Theorems Applications in Mechanics and E&M
Dola Bagayoko (0) Integal Vecto Opeatons and elated Theoems Applcatons n Mechancs and E&M Ι Basc Defnton Please efe to you calculus evewed below. Ι, ΙΙ, andιιι notes and textbooks fo detals on the concepts
More informationPHYS 705: Classical Mechanics. Derivation of Lagrange Equations from D Alembert s Principle
1 PHYS 705: Classcal Mechancs Devaton of Lagange Equatons fom D Alembet s Pncple 2 D Alembet s Pncple Followng a smla agument fo the vtual dsplacement to be consstent wth constants,.e, (no vtual wok fo
More informationOptimization Methods: Linear Programming- Revised Simplex Method. Module 3 Lecture Notes 5. Revised Simplex Method, Duality and Sensitivity analysis
Optmzaton Meods: Lnea Pogammng- Revsed Smple Meod Module Lectue Notes Revsed Smple Meod, Dualty and Senstvty analyss Intoducton In e pevous class, e smple meod was dscussed whee e smple tableau at each
More informationGroupoid and Topological Quotient Group
lobal Jounal of Pue and Appled Mathematcs SSN 0973-768 Volume 3 Numbe 7 07 pp 373-39 Reseach nda Publcatons http://wwwpublcatoncom oupod and Topolocal Quotent oup Mohammad Qasm Manna Depatment of Mathematcs
More informationCOMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS
ultscence - XXX. mcocd Intenatonal ultdscplnay Scentfc Confeence Unvesty of skolc Hungay - pl 06 ISBN 978-963-358-3- COPLEENTRY ENERGY ETHOD FOR CURVED COPOSITE BES Ákos József Lengyel István Ecsed ssstant
More informationRelaxed LMI Based designs for Takagi Sugeno Fuzzy Regulators and Observers Poly-Quadratic Lyapunov Function approach
Poceedngs of the 9 EEE ntenatonal Confeence on Systems, Man, and Cybenetcs San Antono, X, USA - Octobe 9 Relaxed LM Based desgns fo aag Sugeno uzzy Regulatos and Obsees Poly-Quadatc Lyapuno uncton appoach
More informationA Brief Guide to Recognizing and Coping With Failures of the Classical Regression Assumptions
A Bef Gude to Recognzng and Copng Wth Falues of the Classcal Regesson Assumptons Model: Y 1 k X 1 X fxed n epeated samples IID 0, I. Specfcaton Poblems A. Unnecessay explanatoy vaables 1. OLS s no longe
More informationGradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function
Intenational Confeence on Infomation echnology and Management Innovation (ICIMI 05) Gadient-based Neual Netwok fo Online Solution of Lyapunov Matix Equation with Li Activation unction Shiheng Wang, Shidong
More informationSome Approximate Analytical Steady-State Solutions for Cylindrical Fin
Some Appoxmate Analytcal Steady-State Solutons fo Cylndcal Fn ANITA BRUVERE ANDRIS BUIIS Insttute of Mathematcs and Compute Scence Unvesty of Latva Rana ulv 9 Rga LV459 LATVIA Astact: - In ths pape we
More informationModeling and Adaptive Control of a Coordinate Measuring Machine
Modelng and Adaptve Contol of a Coodnate Measung Machne Â. Yudun Obak, Membe, IEEE Abstact Although tadtonal measung nstuments can povde excellent solutons fo the measuement of length, heght, nsde and
More informationEnergy in Closed Systems
Enegy n Closed Systems Anamta Palt palt.anamta@gmal.com Abstact The wtng ndcates a beakdown of the classcal laws. We consde consevaton of enegy wth a many body system n elaton to the nvese squae law and
More informationThermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering
Themodynamcs of solds 4. Statstcal themodynamcs and the 3 d law Kwangheon Pak Kyung Hee Unvesty Depatment of Nuclea Engneeng 4.1. Intoducton to statstcal themodynamcs Classcal themodynamcs Statstcal themodynamcs
More informationV. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. "Flux": = da i. "Force": = -Â g a ik k = X i. Â J i X i (7.
Themodynamcs and Knetcs of Solds 71 V. Pncples of Ievesble Themodynamcs 5. Onsage s Teatment s = S - S 0 = s( a 1, a 2,...) a n = A g - A n (7.6) Equlbum themodynamcs detemnes the paametes of an equlbum
More informationScalars and Vectors Scalar
Scalas and ectos Scala A phscal quantt that s completel chaacteed b a eal numbe (o b ts numecal value) s called a scala. In othe wods a scala possesses onl a magntude. Mass denst volume tempeatue tme eneg
More informationMechanics Physics 151
Mechancs Physcs 151 Lectue 18 Hamltonan Equatons of Moton (Chapte 8) What s Ahead We ae statng Hamltonan fomalsm Hamltonan equaton Today and 11/6 Canoncal tansfomaton 1/3, 1/5, 1/10 Close lnk to non-elatvstc
More informationPhysics 11b Lecture #2. Electric Field Electric Flux Gauss s Law
Physcs 11b Lectue # Electc Feld Electc Flux Gauss s Law What We Dd Last Tme Electc chage = How object esponds to electc foce Comes n postve and negatve flavos Conseved Electc foce Coulomb s Law F Same
More informationRigid Bodies: Equivalent Systems of Forces
Engneeng Statcs, ENGR 2301 Chapte 3 Rgd Bodes: Equvalent Sstems of oces Intoducton Teatment of a bod as a sngle patcle s not alwas possble. In geneal, the se of the bod and the specfc ponts of applcaton
More informationContact, information, consultations
ontact, nfomaton, consultatons hemsty A Bldg; oom 07 phone: 058-347-769 cellula: 664 66 97 E-mal: wojtek_c@pg.gda.pl Offce hous: Fday, 9-0 a.m. A quote of the week (o camel of the week): hee s no expedence
More informationPart V: Velocity and Acceleration Analysis of Mechanisms
Pat V: Velocty an Acceleaton Analyss of Mechansms Ths secton wll evew the most common an cuently pactce methos fo completng the knematcs analyss of mechansms; escbng moton though velocty an acceleaton.
More informationTest 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?
Test 1 phy 0 1. a) What s the pupose of measuement? b) Wte all fou condtons, whch must be satsfed by a scala poduct. (Use dffeent symbols to dstngush opeatons on ectos fom opeatons on numbes.) c) What
More informationA NOTE ON ELASTICITY ESTIMATION OF CENSORED DEMAND
Octobe 003 B 003-09 A NOT ON ASTICITY STIATION OF CNSOD DAND Dansheng Dong an Hay. Kase Conell nvesty Depatment of Apple conomcs an anagement College of Agcultue an fe Scences Conell nvesty Ithaca New
More informationMachine Learning. Spectral Clustering. Lecture 23, April 14, Reading: Eric Xing 1
Machne Leanng -7/5 7/5-78, 78, Spng 8 Spectal Clusteng Ec Xng Lectue 3, pl 4, 8 Readng: Ec Xng Data Clusteng wo dffeent ctea Compactness, e.g., k-means, mxtue models Connectvty, e.g., spectal clusteng
More informationCorrespondence Analysis & Related Methods
Coespondence Analyss & Related Methods Ineta contbutons n weghted PCA PCA s a method of data vsualzaton whch epesents the tue postons of ponts n a map whch comes closest to all the ponts, closest n sense
More informationA Method of Reliability Target Setting for Electric Power Distribution Systems Using Data Envelopment Analysis
27 กก ก 9 2-3 2554 ก ก ก A Method of Relablty aget Settng fo Electc Powe Dstbuton Systems Usng Data Envelopment Analyss ก 2 ก ก ก ก ก 0900 2 ก ก ก ก ก 0900 E-mal: penjan262@hotmal.com Penjan Sng-o Psut
More informationA Study about One-Dimensional Steady State. Heat Transfer in Cylindrical and. Spherical Coordinates
Appled Mathematcal Scences, Vol. 7, 03, no. 5, 67-633 HIKARI Ltd, www.m-hka.com http://dx.do.og/0.988/ams.03.38448 A Study about One-Dmensonal Steady State Heat ansfe n ylndcal and Sphecal oodnates Lesson
More informationSTATE OBSERVATION FOR NONLINEAR SWITCHED SYSTEMS USING NONHOMOGENEOUS HIGH-ORDER SLIDING MODE OBSERVERS
Asan Jounal of Contol Vol. 5 No. pp. 3 Januay 203 Publshed onlne n Wley Onlne Lbay (wleyonlnelbay.com) DOI: 0.002/asc.56 STATE OBSERVATION FOR NONLINEAR SWITCHED SYSTEMS USING NONHOMOGENEOUS HIGH-ORDER
More informationUnconventional double-current circuit accuracy measures and application in twoparameter
th IMEKO TC Wokshop on Techncal Dagnostcs dvanced measuement tools n techncal dagnostcs fo systems elablty and safety June 6-7 Wasaw Poland nconventonal double-cuent ccut accuacy measues and applcaton
More informationSTATE OBSERVATION FOR NONLINEAR SWITCHED SYSTEMS USING NONHOMOGENEOUS HIGH-ORDER SLIDING MODE OBSERVERS
JOBNAME: No Job Name PAGE: SESS: 0 OUTPUT: Tue Feb 0:0: 0 Toppan Best-set Pemeda Lmted Jounal Code: ASJC Poofeade: Mony Atcle No: ASJC Delvey date: Febuay 0 Page Etent: Asan Jounal of Contol Vol. No. pp.
More information19 The Born-Oppenheimer Approximation
9 The Bon-Oppenheme Appoxmaton The full nonelatvstc Hamltonan fo a molecule s gven by (n a.u.) Ĥ = A M A A A, Z A + A + >j j (883) Lets ewte the Hamltonan to emphasze the goal as Ĥ = + A A A, >j j M A
More informationImproved delay-dependent stability criteria for discrete-time stochastic neural networks with time-varying delays
Avalable onlne at www.scencedrect.com Proceda Engneerng 5 ( 4456 446 Improved delay-dependent stablty crtera for dscrete-tme stochastc neural networs wth tme-varyng delays Meng-zhuo Luo a Shou-mng Zhong
More informationSTATE VARIANCE CONSTRAINED FUZZY CONTROL VIA OBSERVER-BASED FUZZY CONTROLLERS
Jounal of Maine Science and echnology, Vol. 4, No., pp. 49-57 (6) 49 SAE VARIANCE CONSRAINED FUZZY CONROL VIA OBSERVER-BASED FUZZY CONROLLERS Wen-Je Chang*, Yi-Lin Yeh**, and Yu-eh Meng*** Key wods: takagi-sugeno
More informationEfficiency of the principal component Liu-type estimator in logistic
Effcency of the pncpal component Lu-type estmato n logstc egesson model Jbo Wu and Yasn Asa 2 School of Mathematcs and Fnance, Chongqng Unvesty of Ats and Scences, Chongqng, Chna 2 Depatment of Mathematcs-Compute
More informationN = N t ; t 0. N is the number of claims paid by the
Iulan MICEA, Ph Mhaela COVIG, Ph Canddate epatment of Mathematcs The Buchaest Academy of Economc Studes an CECHIN-CISTA Uncedt Tac Bank, Lugoj SOME APPOXIMATIONS USE IN THE ISK POCESS OF INSUANCE COMPANY
More informationGENERALIZATION OF AN IDENTITY INVOLVING THE GENERALIZED FIBONACCI NUMBERS AND ITS APPLICATIONS
#A39 INTEGERS 9 (009), 497-513 GENERALIZATION OF AN IDENTITY INVOLVING THE GENERALIZED FIBONACCI NUMBERS AND ITS APPLICATIONS Mohaad Faokh D. G. Depatent of Matheatcs, Fedows Unvesty of Mashhad, Mashhad,
More informationVISUALIZATION OF THE ABSTRACT THEORIES IN DSP COURSE BASED ON CDIO CONCEPT
VISUALIZATION OF THE ABSTRACT THEORIES IN DSP COURSE BASED ON CDIO CONCEPT Wang L-uan, L Jan, Zhen Xao-qong Chengdu Unvesty of Infomaton Technology ABSTRACT The pape analyzes the chaactestcs of many fomulas
More informationCEEP-BIT WORKING PAPER SERIES. Efficiency evaluation of multistage supply chain with data envelopment analysis models
CEEP-BIT WORKING PPER SERIES Effcency evaluaton of multstage supply chan wth data envelopment analyss models Ke Wang Wokng Pape 48 http://ceep.bt.edu.cn/englsh/publcatons/wp/ndex.htm Cente fo Enegy and
More informationDirichlet Mixture Priors: Inference and Adjustment
Dchlet Mxtue Pos: Infeence and Adustment Xugang Ye (Wokng wth Stephen Altschul and Y Kuo Yu) Natonal Cante fo Botechnology Infomaton Motvaton Real-wold obects Independent obsevatons Categocal data () (2)
More informationCS649 Sensor Networks IP Track Lecture 3: Target/Source Localization in Sensor Networks
C649 enso etwoks IP Tack Lectue 3: Taget/ouce Localaton n enso etwoks I-Jeng Wang http://hng.cs.jhu.edu/wsn06/ png 006 C 649 Taget/ouce Localaton n Weless enso etwoks Basc Poblem tatement: Collaboatve
More informationDynamic State Feedback Control of Robotic Formation System
so he 00 EEE/RSJ ntenatonal Confeence on ntellgent Robots and Systems Octobe 8-, 00, ape, awan Dynamc State Feedback Contol of Robotc Fomaton System Chh-Fu Chang, Membe, EEE and L-Chen Fu, Fellow, EEE
More information(8) Gain Stage and Simple Output Stage
EEEB23 Electoncs Analyss & Desgn (8) Gan Stage and Smple Output Stage Leanng Outcome Able to: Analyze an example of a gan stage and output stage of a multstage amplfe. efeence: Neamen, Chapte 11 8.0) ntoducton
More informationEngineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems
Engneeng echancs oce esultants, Toques, Scala oducts, Equvalent oce sstems Tata cgaw-hll Companes, 008 Resultant of Two oces foce: acton of one bod on anothe; chaacteed b ts pont of applcaton, magntude,
More informationControl of Dynamic HIV/AIDS Infection System with Robust H Fuzzy Output Feedback Controller
Intenatonal Jounal of odelng and Optmzaton Vol. 3 No. 3 June 3 Contol of Dynamc IV/AIDS Infecton System wth Robust Fuzzy Output Feedback Contolle Wudhcha Assawnchachote Abstact hs pape consdes the poblem
More informationA. Thicknesses and Densities
10 Lab0 The Eath s Shells A. Thcknesses and Denstes Any theoy of the nteo of the Eath must be consstent wth the fact that ts aggegate densty s 5.5 g/cm (ecall we calculated ths densty last tme). In othe
More informationTian Zheng Department of Statistics Columbia University
Haplotype Tansmsson Assocaton (HTA) An "Impotance" Measue fo Selectng Genetc Makes Tan Zheng Depatment of Statstcs Columba Unvesty Ths s a jont wok wth Pofesso Shaw-Hwa Lo n the Depatment of Statstcs at
More informationHow to Obtain Desirable Transfer Functions in MIMO Systems Under Internal Stability Using Open and Closed Loop Control
How to Obtain Desiable ansfe Functions in MIMO Sstems Unde Intenal Stabilit Using Open and losed Loop ontol echnical Repot of the ISIS Goup at the Univesit of Note Dame ISIS-03-006 June, 03 Panos J. Antsaklis
More informationA Novel Ordinal Regression Method with Minimum Class Variance Support Vector Machine
Intenatonal Confeence on Mateals Engneeng and Infomaton echnology Applcatons (MEIA 05) A ovel Odnal Regesson Method wth Mnmum Class Vaance Suppot Vecto Machne Jnong Hu,, a, Xaomng Wang and Zengx Huang
More information4 SingularValue Decomposition (SVD)
/6/00 Z:\ jeh\self\boo Kannan\Jan-5-00\4 SVD 4 SngulaValue Decomposton (SVD) Chapte 4 Pat SVD he sngula value decomposton of a matx s the factozaton of nto the poduct of thee matces = UDV whee the columns
More informationThe Unique Solution of Stochastic Differential Equations With. Independent Coefficients. Dietrich Ryter.
The Unque Soluton of Stochastc Dffeental Equatons Wth Independent Coeffcents Detch Ryte RyteDM@gawnet.ch Mdatweg 3 CH-4500 Solothun Swtzeland Phone +4132 621 13 07 SDE s must be solved n the ant-itô sense
More informationChapter 8. Linear Momentum, Impulse, and Collisions
Chapte 8 Lnea oentu, Ipulse, and Collsons 8. Lnea oentu and Ipulse The lnea oentu p of a patcle of ass ovng wth velocty v s defned as: p " v ote that p s a vecto that ponts n the sae decton as the velocty
More informationNeuro-Adaptive Design - I:
Lecture 36 Neuro-Adaptve Desgn - I: A Robustfyng ool for Dynamc Inverson Desgn Dr. Radhakant Padh Asst. Professor Dept. of Aerospace Engneerng Indan Insttute of Scence - Bangalore Motvaton Perfect system
More informationGeneral Variance Covariance Structures in Two-Way Random Effects Models
Appled Mathematcs 3 4 64-63 http://dxdoog/436/am34486 Publshed Onlne Apl 3 (http://wwwscpog/jounal/am) Geneal aance Covaance Stuctues n wo-way Rom Effects Models Calos e Poes Jaya Kshnakuma epatment of
More informationINTRODUCTION. consider the statements : I there exists x X. f x, such that. II there exists y Y. such that g y
INRODUCION hs dssetaton s the eadng of efeences [1], [] and [3]. Faas lemma s one of the theoems of the altenatve. hese theoems chaacteze the optmalt condtons of seveal mnmzaton poblems. It s nown that
More informationCSJM University Class: B.Sc.-II Sub:Physics Paper-II Title: Electromagnetics Unit-1: Electrostatics Lecture: 1 to 4
CSJM Unvesty Class: B.Sc.-II Sub:Physcs Pape-II Ttle: Electomagnetcs Unt-: Electostatcs Lectue: to 4 Electostatcs: It deals the study of behavo of statc o statonay Chages. Electc Chage: It s popety by
More informationVibration Input Identification using Dynamic Strain Measurement
Vbaton Input Identfcaton usng Dynamc Stan Measuement Takum ITOFUJI 1 ;TakuyaYOSHIMURA ; 1, Tokyo Metopoltan Unvesty, Japan ABSTRACT Tansfe Path Analyss (TPA) has been conducted n ode to mpove the nose
More informationResearch Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function
Abstact and Applied Analysis Volume 011, Aticle ID 697547, 7 pages doi:10.1155/011/697547 Reseach Aticle On Alze and Qiu s Conjectue fo Complete Elliptic Integal and Invese Hypebolic Tangent Function Yu-Ming
More information9/12/2013. Microelectronics Circuit Analysis and Design. Modes of Operation. Cross Section of Integrated Circuit npn Transistor
Mcoelectoncs Ccut Analyss and Desgn Donald A. Neamen Chapte 5 The pola Juncton Tanssto In ths chapte, we wll: Dscuss the physcal stuctue and opeaton of the bpola juncton tanssto. Undestand the dc analyss
More informationScienceDirect. Dynamic model of a mobile robot
Avalable onlne at www.scencedect.com ScenceDect Poceda Engneeng 96 (014 ) 03 08 Modellng of Mechancal and Mechatonc Systems MMaMS 014 Dynamc model of a moble obot Ján Kadoš* Faculty of Electcal Engneeng
More informationBayesian Assessment of Availabilities and Unavailabilities of Multistate Monotone Systems
Dept. of Math. Unvesty of Oslo Statstcal Reseach Repot No 3 ISSN 0806 3842 June 2010 Bayesan Assessment of Avalabltes and Unavalabltes of Multstate Monotone Systems Bent Natvg Jøund Gåsemy Tond Retan June
More informationNew problems in universal algebraic geometry illustrated by boolean equations
New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic
More informationThe Greatest Deviation Correlation Coefficient and its Geometrical Interpretation
By Rudy A. Gdeon The Unvesty of Montana The Geatest Devaton Coelaton Coeffcent and ts Geometcal Intepetaton The Geatest Devaton Coelaton Coeffcent (GDCC) was ntoduced by Gdeon and Hollste (987). The GDCC
More informationA New Approach for Deriving the Instability Potential for Plates Based on Rigid Body and Force Equilibrium Considerations
Avalable onlne at www.scencedect.com Poceda Engneeng 4 (20) 4 22 The Twelfth East Asa-Pacfc Confeence on Stuctual Engneeng and Constucton A New Appoach fo Devng the Instablty Potental fo Plates Based on
More informationModelling of tangential vibrations in cylindrical grinding contact with regenerative chatter
Modellng of tangental vbatons n cylndcal gndng contact wth egeneatve chatte Vel-Matt ävenpää, Lhong Yuan, Hessam Kalbas Shavan and asal Mehmood ampee Unvesty of echnology epatment of Engneeng esgn P.O.Bo
More informationThe Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution
oden Appled Scence The Fomn Theoy and the NC achnn fo The Rotay us wth the Spectal Ede Dstbuton Huan Lu Depatment of echancal Enneen, Zhejan Unvesty of Scence and Technoloy Hanzhou, c.y. chan, 310023,
More informationChapter 23: Electric Potential
Chapte 23: Electc Potental Electc Potental Enegy It tuns out (won t show ths) that the tostatc foce, qq 1 2 F ˆ = k, s consevatve. 2 Recall, fo any consevatve foce, t s always possble to wte the wok done
More informationSOME NEW SELF-DUAL [96, 48, 16] CODES WITH AN AUTOMORPHISM OF ORDER 15. KEYWORDS: automorphisms, construction, self-dual codes
Факултет по математика и информатика, том ХVІ С, 014 SOME NEW SELF-DUAL [96, 48, 16] CODES WITH AN AUTOMORPHISM OF ORDER 15 NIKOLAY I. YANKOV ABSTRACT: A new method fo constuctng bnay self-dual codes wth
More informationSTABILITY ANALYSIS OF NON-LINEAR STOCHASTIC DYNAMIC SYSTEM BASED ON NUMERICAL SIMULATION
Jounal of Theoetcal and Appled Infomaton Technoloy th Febuay 13. Vol. 48 No. 5-13 JATIT & LLS. All hts eseved. ISSN: 199-8645 www.jatt.o E-ISSN: 1817-3195 STABILITY ANALYSIS OF NON-LINEAR STOCHASTIC DYNAMIC
More informationTransport Coefficients For A GaAs Hydro dynamic Model Extracted From Inhomogeneous Monte Carlo Calculations
Tanspot Coeffcents Fo A GaAs Hydo dynamc Model Extacted Fom Inhomogeneous Monte Calo Calculatons MeKe Ieong and Tngwe Tang Depatment of Electcal and Compute Engneeng Unvesty of Massachusetts, Amhest MA
More informationResearch Article Incremental Tensor Principal Component Analysis for Handwritten Digit Recognition
Hndaw Publshng Copoaton athematcal Poblems n Engneeng, Atcle ID 89758, 0 pages http://dx.do.og/0.55/04/89758 Reseach Atcle Incemental enso Pncpal Component Analyss fo Handwtten Dgt Recognton Chang Lu,,
More informationInternational Journal of Pure and Applied Sciences and Technology
Int. J. Pue Appl. Sc. Technol., 9( (, pp. -8 Intenatonal Jounal of Pue and Appled Scences and Technology ISSN 9-67 Avalable onlne at www.jopaasat.n Reseach Pape Soluton of a Pobablstc Inventoy Model wth
More informationOn the Quasi-inverse of a Non-square Matrix: An Infinite Solution
Applied Mathematical Sciences, Vol 11, 2017, no 27, 1337-1351 HIKARI Ltd, wwwm-hikaicom https://doiog/1012988/ams20177273 On the Quasi-invese of a Non-squae Matix: An Infinite Solution Ruben D Codeo J
More informationOn a quantity that is analogous to potential and a theorem that relates to it
Su une quantité analogue au potential et su un théoème y elatif C R Acad Sci 7 (87) 34-39 On a quantity that is analogous to potential and a theoem that elates to it By R CLAUSIUS Tanslated by D H Delphenich
More informationAnalytical and Numerical Solutions for a Rotating Annular Disk of Variable Thickness
Appled Mathematcs 00 43-438 do:0.436/am.00.5057 Publshed Onlne Novembe 00 (http://www.scrp.og/jounal/am) Analytcal and Numecal Solutons fo a Rotatng Annula Ds of Vaable Thcness Abstact Ashaf M. Zenou Daoud
More information