Neural Network Adaptive Control for Underwater Robotic Systems

Size: px
Start display at page:

Download "Neural Network Adaptive Control for Underwater Robotic Systems"

Transcription

1 Neual Netok Aaptve Contol fo Uneate Robotc Systems V.S. KODOGIANNIS Mechatoncs Goup, Dept of Compute Scence Unvesty of Westmnste Lonon, HA 3P UNIED KINGDOM Abstact: Neual netoks ae cuently fnng pactcal applcatons, angng fom soft egulatoy contol n consume poucts to accuate moellng of non-lnea systems. hs pape escbes the applcaton of neual netoks to the contol of a emotely opeate uneate vehcle, as an example of a system contanng sevee nonlneates. Neual netoks ae been use n a close-loop to appoxmate the nonlnea vehcle ynamcs. No po off-lne tanng phase an no explct knolege of the stuctue of the vehcle ae eque, an the popose scheme explots the avantages of both neual netok contol an aaptve contol. A contol la an a stable on-lne aaptve la ae eve usng the Lyapunov theoy, an the convegence of the tackng eo to zeo an the boune-ness of sgnals ae guaantee. In ths pape, a neual netok achtectue base on aal bass functons has been use to evaluate the pefomance of the aaptve contolle va compute smulaton. Keyos: neual netoks, uneate vehcles, stablty theoy, aaptve contol. Intoucton he Ocean coves ove sxty pecent of the eath s suface, yet humans have haly been able to fully exploe the epths. Unoubtely th the ecent mages captue by the Hubble Space elescope, the Russan M Space Staton an NASA s Galleo atmosphee pobe mankn knos moe about space o the oute sola system than about the Oceans. Hoeve, n the past ecae, Oceanogaphc exploaton has emege as one of the fastest gong aeas of eseach attactng huge gants. he man eason s the vast amount of mneal esouces that satelltes have mappe acoss the Oceans, not fogettng the ol an natual gas eseves. he esgn of contolles fo unmanne uneate vehcles (UUV) s challengng because of ffcultes n accuately moellng the nheently nonlnea ynamcs of UUVs n a hazaous envonment th pesstent unmoelle stubances. In geneal, eal-tme contol of non-lnea systems th unknon stuctue an paamete uncetanty emans an open aea of eseach. Dynamc moels of UUVs ae eque to esgn avance contol systems, an moels of uneate vehcles have been stue n the past []. he nonlnea ynamcs of UUVs esult n paametc an stuctual uncetantes n the ynamc moel, an ths necesstates the nee fo avance obust contol technques. Contol stateges that aess some of moellng chaactestcs have been epote n the lteatue, nclung lnea contol, obust contol, fuzzy contol, neual netoks, slng moe contol, etc. Among vaous contol technques, slng moe contol has been successfully mplemente an teste fo uneate vehcles []. Fossen et al. [3] evelope an aaptve contolle fo uneate vehcles n 6-DOF by assumng that ts ynamcs can be lnealy paametese. he emegence of neual netoks (NNs) as effectve leanng systems fo a e vaety of applcatons has esulte n the use of these netoks as leanng moels fo ynamcal systems. NN contolles have mpotant featues that ovecome the typcal ffcultes n esgnng contol systems fo uneate vehcles. Fo nstance, the ynamcs of the vehcle nee not be completely knon as a po conton fo contolle esgn. hs s vey esable fo uneate vehcle contolle to have snce the ynamc chaactestcs of uneate vehcles change th confguaton an t s mpossble to conse all the effects fom stubances. Also, the ablty of these netoks fo aaptaton an stubance ejecton an the hghly paallel natue of computaton make ths appoach sutable fo eal-tme applcatons. A NN base contol scheme fo UUV s escbe by Venugopal et al. [4] usng ect contol scheme, hee the nput to ynamcs s mplctly use fo both entfcaton an contol smultaneously. A smla ea to the above s use by Yuh [5] n hs stues on the NN-base contol scheme fo an UUV. Fuj et al. [6] popose a self-oganzng neual netok base contol system to the evelopment of the moton contol fo autonomous UUV. Kooganns et al. use seveal ffeent neual netok achtectues to evaluate a long-ange moel pectve contol scheme both fo smulaton an on-lne contol of vehcle epth [7]. An altenatve appoach to soft-computng technques s the mplementaton of appoxmate contolles base on fuzzy logc theoy. A ne fameok n slng moe fuzzy contol as pesente by eb-ollenu et al. fo selectng fee contol paametes of an nput-output lneasng contolle th slng moe contol fo the epth

2 contol of a emotely opeate uneate vehcle (ROV) [8]. In the appoach, the concept of multobjectve fuzzy genetc algothm optmsaton as aopte an a ne membeshp eghtng stategy as suggeste. In ths pape, the evelopment of a ect aaptve neual netok contolle fo uneate vehcles s popose, th a paallel nvestgaton of the pefomance an obustness ssues of the aopte contolle. Raal bass functons netoks (RBF) ae use to appoxmate the nonlnea ynamcs of uneate vehcles thout explct knolege of the plant s ynamc stuctue. he onlne eght aaptaton la of the neual netok s eve n the context of Lyapunov stablty concept. Boune-ness of all sgnals as ell as the convegence of the tackng eos to zeo ae guaantee. he contbuton of ths pape s to combne aaptve contol th neual netok achtectues to appoxmate the nonlnea an tme-vayng uneate vehcle ynamcs. ackng pefomances an obustness of the popose contolle s emonstate though compute smulaton. Vehcle Moellng he ynamc equatons of moton of uneate vehcles have been analytcally pesente n the lteatue [9]. In ths pape a nonlnea sx-egee-offeeom moel base on Fossen et al. [0] has been consee. he g boy uneate vehcle moel n the boy-fxe efeence fame can be epesente as M ν + C( ν ) ν + D( ν ) ν + g( = τ () = J ( ν () hee ν = [ u, υ, ω, p, q, ], = [ X, Y, Z, φ, θ, ψ ].In ths notaton, í enotes the lnea an angula velocty vecto th coonates n the boy-fxe efeence fame, ç enotes the poston an atttue vecto th coonates n the eath-fxe efeence fame, an ô s use to escbe the contol nput foces an moments actng on the vehcle n the boy-fxe efeence fame. he boy-fxe velocty vecto can be tansfome nto the eath-fxe efeence fame though the Eule angle tansfomaton enote by J (. M s the neta matx nclung ae mass M A, C(ν ) s the matx of Cools an centfugal tems, D (ν ) s the ampng matx, an g( ) s the vecto of gavtatonal foces an moments. he equaton of moton of uneate vehcle can be epesente n the eath-fxe efeence fame n tems of poston an atttue though the knematc tansfomatons (assumng that J ( ) s non-sngula) = J ( ν ν = J ( (3) ( ν ( ν ν ( [ = J + J = J J ( J ( ] (4) to elmnate ν an ν fom Eq.. Defnng M ( = J ( MJ ( (5) C ( ν, = J ( [ C( ν ) MJ ( J ( ] J ( (6) D ( ν, = J ( DJ g ( (7) ( = J ( g( (8) τ ( = J ( τ (9) yels the eath-fxe vecto epesentaton M ( ) + C ( ν, + D ( ν, + g ( = τ (0) he neta matx M ( ), nclung hyoynamc ae neta, s symmetc an postve efnte. he Cools an centfugal matx, also nclung ae neta effect, C ( ν,, satsfes the ske symmetc elatonshp x [ M ( C ( ν, ] x = 0. he ampng matx D ( ν, s postve efnte. A moe etale scusson on mathematcal moels of uneate vehcles can be foun n [3]. 3 Neual Netok Contolle Desgn Due to the ffculty obtanng the exact values of hyoynamc coeffcents, but also ue to the fact the coeffcents change th the confguaton of uneate vehcles, the obustness an aaptveness ae mpotant equements fo the uneate vehcle contolles. he stubances fom cuents an aves ae also vey ffcult to moel. Fossen et al. [0] eve an aaptve contol la fo uneate vehcles n 6 DOF assumng that M, C (ν ), D (ν ), an g ( ) ae lnea n the paametes an that the ynamcs can be lnealy paametese, hch s a common assumpton n the aaptve contol. he lnea paametesaton n the aaptve contol s usually val an can conse the changes an uncetantes n paametes. Hoeve, t shoul be note that ths assumpton conses the change only n paametes; the unstuctue o un-moelle ynamcs such as stubances fom cuents an aves cannot be lnealy paametese. In ths pape, an aaptve contol la s eve that oes not eque off-lne tanng. An RBF netok s use n the appoxmaton of a nonlnea functon, assumng that the nonlnea moel of the uneate vehcles s unknon. 3. Contolle Specfcatons A cetan measue of eo s efne as s = + λ () hee ë s any postve constant an =. he ese poston an atttue of the vehcle enote by, an the tme evatve, can be obtane fom a tajectoy planne. he efeence moel s

3 chosen conseng the vehcle knematcs as n [3]. he ese paametes ν an ae compute fom ν + Λν + J ( ) Ω = J ( ) Ω () = J ( ν ) (3) hee s a constant (o sloly vayng) commane nput. he esgn paametes n the efeence moel ae the matces Ë > 0 an Ù = Ù > 0 escbng the pefee ampng an stffness of the system. Ë an Ù ae usually chosen as agonal matces th postve entes on the agonal. Fo notatonal smplcty, t s convenent to ete Eq. n tems of the vtual efeence tajectoy efne as s = = λ (4) he efeence tajectoy n the boy-fxe fame can be eve = J ( ν (5) ν J ( [ J = ( J ( ] (6) No, the Eq. 0 escbng the nonlnea equaton of moton of an uneate vehcle n 6 DOF n the eath-fxe efeence coonate s consee. akng the evatve of s th espect to tme, the vehcle ynamcs can be tten n tems of s as M s = M M = ( D + C ) s + J [ τ ( Mν + C( ν ) ν + D( ν ) ν + g( )] (7) Çee, the elatonshp M + C + D + g = (8) J ( Mν + Cν + Dν + g) s use. Denotng the ynamcs of vehcle n the boyfxe efeence coonate as M ν + C( ν ) ν + D( ν ) ν + g( = f ( ν, ν, ν, (9) an takng a contol nput as τ = fˆ ( ν, ν, ν, J K s, the close-loop system becomes M s = ( D + K ) s C s + J [ fˆ( ν, ν, ν, ε] (0) + hee f ˆ( ν, ν, ν, s the estmate of the vehcle ynamcs f ( ν, ν, ν,, K s a symmetc postve egulato gan matx of appopate menson an å s use to enote the appoxmaton eo. Eq. 0 s an eo ynamcs hee the fltee tackng eo s ven by the functonal estmaton eo. Follong the appoach n [], the tackng poblem can thus be solve by fnng a aaptaton la fo ajustng f ˆ( ν, ν, ν, that ensues the boune-ness of the paamete estmates an that s ( t) 0 as t. 3. Lnea Paametesaton Conseng the Eq. (8), Eq. (9) can be paametese as M ν + C ν ) ν + D( ν ) ν + g( = Φ( ν, ν, ν, θ () ( assumng that M, C (ν ), D (ν ), an g ( ) ae lnea n the paametes. Hee, è s an unknon paamete vecto an Φ( ν, ν, ν, s a knon matx functon of measue sgnals usually efee to as egesso matx. Conse a Lyapunov functon as V = s M s + θ Γ θ () hee Γ s a postve efnte eghtng matx of appopate menson an θ = θ ˆ θ s the paamete estmaton eo. Dffeentatng V th espect to tme yels V = ( s M s + s M s + s M s) + θ Γ θ (3) Usng the symmety of neta matx s M s = s M s an the ske-symmetc popety s ( M C ( ν, ) s = 0, Eq. (3) becomes V = s ( M s + C s) + θ Γ θ (4) Conseng Eq. (7), Eq. (4) becomes V = s D s + [ J ( s] [ τ Φ( ν, ν, ν, θ ] + θ Γ (5) Let the contol nput be chosen as τ = Φ( ν, ν, ν, θˆ J ( K s (6) ) hee θˆ s the estmate paamete vecto an K s a symmetc postve egulato gan matx of appopate menson. Hence, V = s ( K + D ) s + θ [ Φ ( ν, ν, ν, J ( s + Γ θ ] (7) hen the paamete upate la th the assumpton of constant paametes ( θ = 0) θ = ΓΦ ( ν, ν, ν, J ( ) s (8) cancels out the last tem n the expesson fo V an yels V = s ( K + D ) s 0 (9) hen, the convegence of s to zeo an the bouneness of the paametes can be shon by applyng Babalat s lemma [] as follos. Snce V s negatve o zeo an V s postve efnte, V tens to a constant as t. Conseng that the neta matx M s postve efnte an s s boune, the estmaton eos θ can be shon to be boune, consequently θˆ s boune. hs makes s s boune shong that s s unfomly contnuous. heefoe, applyng Babalat s lemma [], t can be shon that V 0 an s 0 as t. he convegence of s to zeo mples the convegence of the tackng eo an to zeo snce the tackng eo s ven by s though a stable ynamcs as shon n Eq. (). θ

4 4 Neual Netok Moellng he evaton of the contol la an the aaptaton la of the eghts of the RBF netok ae consee n ths secton. hs neual netok shon n Fg. conssts of one laye of sees of neuons multple by output eghts. Such system s employe snce t s knon that a lnea supeposton of aal bass functons s the optmal soluton to a class of functon n appoxmatons gven a fnte set of ata n R [3]. Also, the elatvely smple netok stuctue enables the easy evaton of an aaptve netok upate la. he mathematcal epesentaton of the neual netok s N f ( x) = γ ) =,...,n (30) hee j= j j j γ j = exp[ x j / σ j s the nonlnea functon at noe j, taken as a Gaussan functon of the nne pouct of ts aguments. he coeffcents Fg. : Stuctue of RBF netok j epesent the cente of aal Gaussan, σ j s a measue of ts th at noe j, an j epesents the output eght fo that noe. he numbe of egee-of-feeom s enote by n, an N s the numbe of employe neuons. It s assume that thee exsts a cetan combnaton of optmal eghts of the netok that poves the satsfactoy appoxmaton of the nonlnea mappng applyng enough numbe of neuons. he Lyapunov functon canate s chosen as { V = s M s + t Γ (3) hee Γ s a postve efnte eghtng matx of appopate menson, an = ˆ s the estmaton eo of the netok output eghts. Hee, ŵ s the output eght estmate an s the optmal eght. Dffeentatng V th espect to tme yels V ( s M s s M s s M s) t{ = Γ (3) Usng the facts that s M s = s M s, the ske symmety of s ( M C ) s = 0, an the close loop system Eq. (0), Eq. (3) can be etten as V = s = s ( M s + C s) + t{ Γ D s + ( J s) [ τ f ( ν, ν, ν, ] + t{ Γ (33) he aal bass neual netok s use as an appoxmaton of the ynamcs of the plant as f ( ν, ν, ν, = ˆ γ ) + ε ( x) (34) hee ε (x) enotes the appoxmaton eo an t s assume to be boune as ε( x ) ε 0 fo x Ω hee s the oman of appoxmaton. he boun ε 0 on the appoxmaton eo can be mae smalle by selectng a lage numbe of neuons n the hen laye, an t s assume that t can be neglecte as long as enough numbe of neuons s aopte. Choosng the contol nput as τ = ˆ γ ) J ( K s (35) an assumng that the output of aal bass neual netok appoxmates the functon th suffcent pecson as long as th oman of appoxmaton s completely covee, Eq. (33) becomes ( ) ( ) [ (, )] { V = s D + K s + J s γ x + t Γ s ( D + K ) s + t{ [ γ )( J s) + Γ (36) Also, choosng the aaptve la of the netok eght as ˆ = Γγ )( J s) (37) the Eq.(33) can be shon to be negatve sem-efnte, hch mples the convegence of s to zeo an the boune-ness of applyng Babalat s lemma []. In summay, the contol la s gven by Eq. (35) an the aaptaton la s gven by Eq. (37). It shoul be note that the appoxmaton of the nonlnea functon Eq. (34) can also be expesse as the pouct of egesso matx an unknon paametes une the assumpton that the nonlnea functon s lnea n the paametes an the ynamc stuctue of vehcles s completely knon. he neual netok appoxmaton oes not eque such assumpton snce no explct knolege of the ynamc stuctue s eque. he achtectue of contolle s shon n Fg.. Fg. : Popose contolle achtectue ]

5 5 ROV Case Stuy he computatonal stuy n ths pape as base on the moel stuctue of the Noegan Expemental Remotely Opeate Vehcle (NEROV) [4]. he vehcle s contolle n all 6 DOF by sx c-moto ven thustes. he flu velocty as chosen to be zeo n all computatons. he ese veloctes an postons ee geneate by a efeence tajectoy geneato. he smulaton, usng the evelope contolle, ee pefome at 5Hz, hch mples all the measuements an the contol acton occue at a tme step of 0. secons. he tackng pefomance of the X an Y postons, the epth an the heang angle as consee n ths stuy. he cente of gavty as assume to be locate at the ogn of the vehcle coonate system. he neta matx as assume to be agonal: M ag{ m X I y q, I z, m Y, m Z = u υ ω M he mass s N, I x K p, (38) m = 85 Kg. he moments of neta aoun the x-, y- an z-axes ae I y = 50 kgm an I x = 50 kgm I x = 5 kgm,. he hyoynamc ae netas ae X u = 30 kg, Y υ = 80 kg, Z = 80 kg, ω K p = 5 kgm, M q = 30 kgm, N = 30 kgm. he C matx s assume to be as 0 m mq 0 Zω Yυ m 0 mp Zω 0 Xu u mq mp 0 Y = υ Xu u 0 C (39) 0 Zω Yυ 0 ( Iz N ) ( Iy Mq ) q Zω 0 Xu u ( Iz N ) 0 ( Ix Kp ) p Y υ Xu u 0 ( Iy Mq ) q ( Ix Kp ) p 0 he ag matx s assume to be agonal D( ν ) = ag{ u, υ, (40) ω, p, q, buoyancy. One RBF netok as use to appoxmate the nonlnea ynamcs of NEROV. In ths patcula case, the centes of Gaussan functons γ ) ee unfomly space n the state space. he th of the Gaussan functon γ ) as set to 30, an the oveall eghts of a neual netok ee ntally set to zeo. Only a sngle MIMO neual netok as employe th 4 nput an 6 output unts. he aaptve gan matx as set to 0.3I, hee I as the entty matx of appopate menson. he choce of the th of the Gaussan functon γ ) as the most ctcal facto fo oveall stablty of the system an elate to the choce of the numbe of Gaussan functons ove the state space. In othe os, the optmal th of the Gaussan functon shoul be foun conseng the th of an aea n the nput space to each neuon espons. he value of γ ) shoul be lage enough that neuons espon to enough ovelappng egons of the nput space. he tackng pefomance of the X an Y postons of the vehcle follong the specfe poston s shon n Fg. 3. It can be seen that the popose neual-netok contolle gves faly goo tackng pefomance. In ths smulaton stuy, only the neual netok contolle as use to etemne the feasblty of usng the popose neual netok achtectue. Of couse, mpove an moe obust tackng pefomance coul be acheve hen the PD an the aaptve contol nputs ae combne togethe. Bette pefomance may be obtane by futhe tunng the upate gan an nceasng the numbe of RBF centes. Hghe upate gan gave bette tackng pefomance, but hen the gan as too hgh, oscllatoy behavou as obseve. By combnng th the PD pat of the contolle, the unante oscllatoy moton coul be emove at the pce of slght ncease n the contol effot. Contol nputs ae shon n Fg. 4. Fg. 3: X an Y tajectoy (sol: ese; ashe: popose contolle) he cente of buoyancy as assume to be locate at ( x B, y B, z B ), hee x B =y B =0 an z B =0.0m s the x-, y- an z-coonates n the vehcle coonate system. he system as assume to be neutally buoyant g=(0,0,0, z B Bcèsö, z B Bsè,0), hee B=800N s the Fg. 4: Contol nputs to thustes Robustness of the popose contolle to the unmoelle stubance s shon n the Fg. 5. A snusoal stubance s ae n the ya channel. he pefomance of aaptve neual netok contolle

6 th aal bass neual netok s compae to the aaptve contolle th lnea paametesaton. A obust tackng pefomance has been acheve usng aaptve neual netok, heeas the aaptve contolle th lnea paametesaton gves egaaton n the pefomance. Fg. 5: Robustness test to the unmoelle stubances n the ya channel (sol: ese, ashe: popose, ashot: lnealy paametese) 6 Conclusons An aaptve neual netok contolle has been evelope fo an uneate vehcle n 6 DOF. One RBF netok as use to appoxmate the nonlnea ynamcs of uneate vehcle. Wthout explct po knolege of the vehcle ynamcs, the popose contol technque coul acheve mpove tackng pefomance. Results have shoe that the ynamcs of the vehcle nee not be knon explctly fo the esgn of the contolle an no lneasaton s eque to eal th nonlnea vehcle ynamcs. he popose contolle achtectue s obust an aaptve, hle t oes not nee any po tanng phase an can be apple on-lne. he next stage of ths stuy s to apply the popose aaptve contolle n the une evelopment UUV fune fom the FREESUB 5 th fameok EU poject. Refeences [] Yoege D.R. Slotne J., Robust tajectoy contol of uneate vehcles, IEEE Jounal of Oceanc Engneeng, Vol., No. 4, 985, pp [] Song F. Smth S., Desgn of slng moe fuzzy contolles fo an autonomous uneate vehcle thout system moel, Oceans 000 IEEE Conf., Vol., 000, pp [3] Fossen.I, Guance an contol of ocean vehcles, John Wley an Sons, 994. [4] Venugopal K.P., R. Suhaka R. Panya A.S., On-lne leanng contol of autonomous uneate vehcles usng feefoa neual netoks. IEEE J. of Oceanc Engneeng, Vol. 7, No. 4, 99, pp [5] J. Yuh J., Leanng contol fo uneate obotc vehcles, IEEE Contol Systems Magazne, Vol. 5, No., 994, pp [6] Fuj,., Ish K. Ua., Neual netok system fo on-lne contolle aaptaton an ts applcaton to uneate obot, Poc. 998 IEEE Conf. on obotcs an automaton, Belgum 998, pp [7] Kooganns V.S., Lsboa P.J.G., Lucas J., Neual netok moelng an contol fo uneate vehcles, Atfcal Intellgence n Engneeng, Vol., 996, pp.03-. [8] eb-ollennu A. Whte B.A, Multobjectve fuzzy genetc algothm optmsaton appoach to monto contol system esgn, IEE Poc. Contol heoy Appl., Vol. 44, No, 997, pp [9] Fossen.I., Sagatun S.I., Søensen A., Ientfcaton of ynamcally postone shps, IFAC Wokshop on Contol Applcatons n Mane Systems (CAMS 95), Noay, 995, pp [0] Fossen.I., Sagatun S.I., Aaptve contol of nonlnea systems: A case stuy of uneate obotc systems. Jounal of Robotc Systems, Vol. 8, No. 3, 99, pp [] Sanne R.M. Slotne J.J., Gaussan netoks fo ect aaptve contol, IEEE ansactons on Neual Netoks, Vol. 3, No.6, 99, pp [] Slotne J.J. L W., Apple Nonlnea Contol, Pentce Hall, 99 [3] Chen, S., Chang, E.S., Alkahm, K., Regulaze Othogonal Least Squaes Algothm fo Constuctng Raal Bass Functon Netoks, Int. J. Contol, Vol.64, No. 5, 996, pp [4] Spangelo I Egelan O, ajectoy plannng an collson avoance fo uneate vehcles usng optmal contol, IEEE Jounal of Oceanc Engneeng, Vol. 9, No. 4, 994, 50-5.

ADAPTIVE SLIDING MODE CONROL WITH RADIAL BASIS FUNCTION NEURAL NETWORK FOR TIME DEPENDENT DISTURBANCES AND UNCERTAINTIES

ADAPTIVE SLIDING MODE CONROL WITH RADIAL BASIS FUNCTION NEURAL NETWORK FOR TIME DEPENDENT DISTURBANCES AND UNCERTAINTIES VOL., NO. 6, MARCH 6 ISSN 89-668 ARPN Jounal of Engneeng an Apple Scences 6-6 Asan Reseach Publshng Netwok (ARPN). All ghts eseve. ADAPIVE SLIDING MODE CONROL WIH RADIAL BASIS FUNCION NEURAL NEWORK FOR

More information

Part V: Velocity and Acceleration Analysis of Mechanisms

Part 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 information

Scalars and Vectors Scalar

Scalars 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 information

Modeling and Adaptive Control of a Coordinate Measuring Machine

Modeling 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 information

A NOTE ON ELASTICITY ESTIMATION OF CENSORED DEMAND

A 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 information

CS649 Sensor Networks IP Track Lecture 3: Target/Source Localization in Sensor Networks

CS649 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 information

Sliding Mode Control of Surface-Mount Permanent-Magnet Synchronous Motor Based on Error Model with Unknown Load

Sliding Mode Control of Surface-Mount Permanent-Magnet Synchronous Motor Based on Error Model with Unknown Load JOURNAL OF SOFTWARE VOL. 6 NO. 5 MAY 0 89 Slng Moe Contol o SuaceMount PemanentMagnet Synchonous Moto Base on Eo Moel th Unknon Loa Baojun Wang Insttute o Inomaton Technology /Zhejang Insttute o Communcatons

More information

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model 6. ntoucton to anssto mples: oncepts an Small-Sgnal Moel Lectue notes: Sec. 5 Sea & Smth 6 th E: Sec. 5.4, 5.6 & 6.3-6.4 Sea & Smth 5 th E: Sec. 4.4, 4.6 & 5.3-5.4 EE 65, Wnte203, F. Najmaba Founaton o

More information

Density Functional Theory I

Density Functional Theory I Densty Functonal Theoy I cholas M. Hason Depatment of Chemsty Impeal College Lonon & Computatonal Mateals Scence Daesbuy Laboatoy ncholas.hason@c.ac.uk Densty Functonal Theoy I The Many Electon Schönge

More information

8 Baire Category Theorem and Uniform Boundedness

8 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 information

P 365. r r r )...(1 365

P 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 information

A Brief Guide to Recognizing and Coping With Failures of the Classical Regression Assumptions

A 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 information

Exact Simplification of Support Vector Solutions

Exact 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 information

Set of square-integrable function 2 L : function space F

Set 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 information

Multistage Median Ranked Set Sampling for Estimating the Population Median

Multistage 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 information

A. Thicknesses and Densities

A. 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 information

PHYS 705: Classical Mechanics. Derivation of Lagrange Equations from D Alembert s Principle

PHYS 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 information

Khintchine-Type Inequalities and Their Applications in Optimization

Khintchine-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 information

On Maneuvering Target Tracking with Online Observed Colored Glint Noise Parameter Estimation

On 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 information

Machine Learning. Spectral Clustering. Lecture 23, April 14, Reading: Eric Xing 1

Machine 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 information

3. A Review of Some Existing AW (BT, CT) Algorithms

3. 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 information

Rigid Bodies: Equivalent Systems of Forces

Rigid 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 information

Adaptive Fuzzy Dynamic Surface Control for a Class of Perturbed Nonlinear Time-varying Delay Systems with Unknown Dead-zone

Adaptive 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 information

Observer Design for Takagi-Sugeno Descriptor System with Lipschitz Constraints

Observer 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 information

An Approach to Inverse Fuzzy Arithmetic

An 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 information

4 Recursive Linear Predictor

4 Recursive Linear Predictor 4 Recusve Lnea Pedcto The man objectve of ths chapte s to desgn a lnea pedcto wthout havng a po knowledge about the coelaton popetes of the nput sgnal. In the conventonal lnea pedcto the known coelaton

More information

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Physics 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 information

19 The Born-Oppenheimer Approximation

19 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 information

Experimental study on parameter choices in norm-r support vector regression machines with noisy input

Experimental 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 information

M. T. Franklin. Tests of Composite Null Hypotheses. Applied to Multivariate Measurements

M. T. Franklin. Tests of Composite Null Hypotheses. Applied to Multivariate Measurements TESTING AGREEMENT OF ISOTOPIC ABUNDANCE MEASUREMENTS WILE TAKING ACCOUNT OF ACCEPTABLE BIAS M T Fankln Tests of Composte Null ypotheses Apple to Multvaate Measuements EUR 476 EN 9 The msson of the Insttute

More information

Support Vector Machines

Support Vector Machines Hstoy Suppot Vecto Machnes Moe om Po. Ane W. Mooe s Lectue otes.cs.cmu.eu/~am SVM s a classe eve om statstcal leanng theoy y Vapn an Chevonens SVMs ntouce y Bose, Guyon, Vapn n COLT-9 o an mpotant an actve

More information

Machine Learning 4771

Machine 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 information

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

If 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 information

Chapter Fifiteen. Surfaces Revisited

Chapter 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 information

CHAPTER 2 DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE. 2.1 Derivation of Machine Equations

CHAPTER 2 DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE. 2.1 Derivation of Machine Equations 1 CHAPTER DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE 1 Deivation of Machine Equations A moel of a phase PM machine is shown in Figue 1 Both the abc an the q axes ae shown

More information

Determining solar characteristics using planetary data

Determining solar characteristics using planetary data Detemining sola chaacteistics using planetay data Intoduction The Sun is a G-type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this investigation

More information

C e f paamete adaptation f (' x) ' ' d _ d ; ; e _e K p K v u ^M() RBF NN ^h( ) _ obot s _ s n W ' f x x xm xm f x xm d Figue : Block diagam of comput

C e f paamete adaptation f (' x) ' ' d _ d ; ; e _e K p K v u ^M() RBF NN ^h( ) _ obot s _ s n W ' f x x xm xm f x xm d Figue : Block diagam of comput A Neual-Netwok Compensato with Fuzzy Robustication Tems fo Impoved Design of Adaptive Contol of Robot Manipulatos Y.H. FUNG and S.K. TSO Cente fo Intelligent Design, Automation and Manufactuing City Univesity

More information

New Condition of Stabilization of Uncertain Continuous Takagi-Sugeno Fuzzy System based on Fuzzy Lyapunov Function

New 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 information

Energy in Closed Systems

Energy 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 information

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3.

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3. 3 Eath s Rotaton 3.1 Rotatng Famewok Othe eadng: Valls 2.1, 2.2; Mashall and Plumb Ch. 6; Holton Ch. 2; Schubet Ch. 3 Consde the poston vecto (the same as C n the fgue above) otatng at angula velocty.

More information

1.050 Engineering Mechanics I. Summary of variables/concepts. Lecture 27-37

1.050 Engineering Mechanics I. Summary of variables/concepts. Lecture 27-37 .5 Engneeng Mechancs I Summa of vaabes/concepts Lectue 7-37 Vaabe Defnton Notes & ments f secant f tangent f a b a f b f a Convet of a functon a b W v W F v R Etena wok N N δ δ N Fee eneg an pementa fee

More information

9/12/2013. Microelectronics Circuit Analysis and Design. Modes of Operation. Cross Section of Integrated Circuit npn Transistor

9/12/2013. 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 information

Vibration Input Identification using Dynamic Strain Measurement

Vibration 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 information

Stable Model Predictive Control Based on TS Fuzzy Model with Application to Boiler-turbine Coordinated System

Stable 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 information

1. A body will remain in a state of rest, or of uniform motion in a straight line unless it

1. A body will remain in a state of rest, or of uniform motion in a straight line unless it Pncples of Dnamcs: Newton's Laws of moton. : Foce Analss 1. A bod wll eman n a state of est, o of unfom moton n a staght lne unless t s acted b etenal foces to change ts state.. The ate of change of momentum

More information

4 SingularValue Decomposition (SVD)

4 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 information

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Physics 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 information

time [s] time [s]

time [s] time [s] ROBUST ATTITUDE STABILIZATION OF AN UNDERACTUATED AUV K. Y. Pettesen and O. Egeland Depatment of Engineeing Cybenetics Nowegian Univesity of Science and Technology N- Tondheim, Noway Fax: + 9 99 E-mail:

More information

LASER ABLATION ICP-MS: DATA REDUCTION

LASER ABLATION ICP-MS: DATA REDUCTION Lee, C-T A Lase Ablaton Data educton 2006 LASE ABLATON CP-MS: DATA EDUCTON Cn-Ty A. Lee 24 Septembe 2006 Analyss and calculaton of concentatons Lase ablaton analyses ae done n tme-esolved mode. A ~30 s

More information

Summer Workshop on the Reaction Theory Exercise sheet 8. Classwork

Summer Workshop on the Reaction Theory Exercise sheet 8. Classwork Joned Physcs Analyss Cente Summe Wokshop on the Reacton Theoy Execse sheet 8 Vncent Matheu Contact: http://www.ndana.edu/~sst/ndex.html June June To be dscussed on Tuesday of Week-II. Classwok. Deve all

More information

Optimization Methods: Linear Programming- Revised Simplex Method. Module 3 Lecture Notes 5. Revised Simplex Method, Duality and Sensitivity analysis

Optimization 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 information

Learning the structure of Bayesian belief networks

Learning the structure of Bayesian belief networks Lectue 17 Leanng the stuctue of Bayesan belef netwoks Mlos Hauskecht mlos@cs.ptt.edu 5329 Sennott Squae Leanng of BBN Leanng. Leanng of paametes of condtonal pobabltes Leanng of the netwok stuctue Vaables:

More information

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS

COMPLEMENTARY 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 information

Amplifier Constant Gain and Noise

Amplifier Constant Gain and Noise Amplfe Constant Gan and ose by Manfed Thumm and Wene Wesbeck Foschungszentum Kalsuhe n de Helmholtz - Gemenschaft Unvestät Kalsuhe (TH) Reseach Unvesty founded 85 Ccles of Constant Gan (I) If s taken to

More information

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution

The 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 information

ENGI9496 Lecture Notes Multiport Models in Mechanics

ENGI9496 Lecture Notes Multiport Models in Mechanics ENGI9496 Moellng an Smulaton of Dynamc Systems Mechancs an Mechansms ENGI9496 Lecture Notes Multport Moels n Mechancs (New text Secton 4..3; Secton 9.1 generalzes to 3D moton) Defntons Generalze coornates

More information

Dynamics of Rigid Bodies

Dynamics of Rigid Bodies Dynamcs of Rgd Bodes A gd body s one n whch the dstances between consttuent patcles s constant thoughout the moton of the body,.e. t keeps ts shape. Thee ae two knds of gd body moton: 1. Tanslatonal Rectlnea

More information

2 dependence in the electrostatic force means that it is also

2 dependence in the electrostatic force means that it is also lectc Potental negy an lectc Potental A scala el, nvolvng magntues only, s oten ease to wo wth when compae to a vecto el. Fo electc els not havng to begn wth vecto ssues woul be nce. To aange ths a scala

More information

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Engineering 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 information

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS. GNRAL PHYSICS PH -3A (D. S. Mov) Test (/3/) key STUDNT NAM: STUDNT d #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

Passivity-Based Control of Saturated Induction Motors

Passivity-Based Control of Saturated Induction Motors Passivity-Base Contol of Satuate Inuction otos Levent U. Gökee, embe, IEEE, awan A. Simaan, Fellow, IEEE, an Chales W. Bice, Senio embe, IEEE Depatment of Electical Engineeing Univesity of South Caolina

More information

Impact of donor-acceptor morphology on the charge carrier generation in organic photovoltaic devices

Impact of donor-acceptor morphology on the charge carrier generation in organic photovoltaic devices Jounal of Physcs: Confeence Sees PAPER OPEN ACCESS Impact of ono-accepto mophology on the chage cae geneaton n oganc photovoltac evces To cte ths atcle: M. L. Inche Ibahm 2017 J. Phys.: Conf. Se. 949 012007

More information

NOTE. Some New Bounds for Cover-Free Families

NOTE. Some New Bounds for Cover-Free Families Jounal of Combinatoial Theoy, Seies A 90, 224234 (2000) doi:10.1006jcta.1999.3036, available online at http:.idealibay.com on NOTE Some Ne Bounds fo Cove-Fee Families D. R. Stinson 1 and R. Wei Depatment

More information

Minimising Energy Consumption for Robot Arm Movement

Minimising Energy Consumption for Robot Arm Movement Mnmsng Enegy Consumpton fo obot Am Movement Abdullah Mohammed, Benad Schmdt, Lhu Wang, Lang Gao KH oyal Insttute of echnology, Bnellvägen 8, Stockholm, SE- Sweden, E-Mal: abdullah.mohammed@tm.kth.se, lhu.wang@p.kth.se

More information

Advanced Robust PDC Fuzzy Control of Nonlinear Systems

Advanced 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 information

Supersymmetry in Disorder and Chaos (Random matrices, physics of compound nuclei, mathematics of random processes)

Supersymmetry in Disorder and Chaos (Random matrices, physics of compound nuclei, mathematics of random processes) Supesymmety n Dsoe an Chaos Ranom matces physcs of compoun nucle mathematcs of anom pocesses Lteatue: K.B. Efetov Supesymmety n Dsoe an Chaos Cambge Unvesty Pess 997999 Supesymmety an Tace Fomulae I.V.

More information

Tian Zheng Department of Statistics Columbia University

Tian 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 information

Correspondence Analysis & Related Methods

Correspondence 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 information

The Backpropagation Algorithm

The Backpropagation Algorithm The Backpopagaton Algothm Achtectue of Feedfowad Netwok Sgmodal Thehold Functon Contuctng an Obectve Functon Tanng a one-laye netwok by teepet decent Tanng a two-laye netwok by teepet decent Copyght Robet

More information

( )( )( ) ( ) + ( ) ( ) ( )

( )( )( ) ( ) + ( ) ( ) ( ) 3.7. Moel: The magnetic fiel is that of a moving chage paticle. Please efe to Figue Ex3.7. Solve: Using the iot-savat law, 7 19 7 ( ) + ( ) qvsinθ 1 T m/a 1.6 1 C. 1 m/s sin135 1. 1 m 1. 1 m 15 = = = 1.13

More information

Light Time Delay and Apparent Position

Light Time Delay and Apparent Position Light Time Delay and ppaent Position nalytical Gaphics, Inc. www.agi.com info@agi.com 610.981.8000 800.220.4785 Contents Intoduction... 3 Computing Light Time Delay... 3 Tansmission fom to... 4 Reception

More information

A Crash Course in (2 2) Matrices

A Crash Course in (2 2) Matrices A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula

More information

Chapter 13 - Universal Gravitation

Chapter 13 - Universal Gravitation Chapte 3 - Unesal Gataton In Chapte 5 we studed Newton s thee laws of moton. In addton to these laws, Newton fomulated the law of unesal gataton. Ths law states that two masses ae attacted by a foce gen

More information

J. Electrical Systems 1-3 (2005): Regular paper

J. Electrical Systems 1-3 (2005): Regular paper K. Saii D. Rahem S. Saii A Miaoui Regula pape Coupled Analytical-Finite Element Methods fo Linea Electomagnetic Actuato Analysis JES Jounal of Electical Systems In this pape, a linea electomagnetic actuato

More information

FUZZY CONTROL VIA IMPERFECT PREMISE MATCHING APPROACH FOR DISCRETE TAKAGI-SUGENO FUZZY SYSTEMS WITH MULTIPLICATIVE NOISES

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 information

A Study about One-Dimensional Steady State. Heat Transfer in Cylindrical and. Spherical Coordinates

A 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 information

Distinct 8-QAM+ Perfect Arrays Fanxin Zeng 1, a, Zhenyu Zhang 2,1, b, Linjie Qian 1, c

Distinct 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 information

(8) Gain Stage and Simple Output Stage

(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 information

Department of Electrical Engineering, University of Tiaret, Tiaret BP 078, Tiaret, Algeria

Department of Electrical Engineering, University of Tiaret, Tiaret BP 078, Tiaret, Algeria Jounal of Netwok an Innovatve Computng ISSN 6-74 Volume (4) pp. 58-65 MIR abs www.mlabs.net/jnc/nex.html A New Appoach Fuzzy-MRAS Spee Sensoless Slng moe Contol fo Inteo Pemanent-Magnet Machne Dve Khalfallah

More information

Optimization Algorithms for System Integration

Optimization Algorithms for System Integration Optmzaton Algothms fo System Integaton Costas Papadmtou 1, a and Evaggelos totsos 1,b 1 Unvesty of hessaly, Depatment of Mechancal and Industal Engneeng, Volos 38334, Geece a costasp@uth.g, b entotso@uth.g

More information

CSJM University Class: B.Sc.-II Sub:Physics Paper-II Title: Electromagnetics Unit-1: Electrostatics Lecture: 1 to 4

CSJM 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 information

Chapter 8. Linear Momentum, Impulse, and Collisions

Chapter 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 information

is the instantaneous position vector of any grid point or fluid

is the instantaneous position vector of any grid point or fluid Absolute inetial, elative inetial and non-inetial coodinates fo a moving but non-defoming contol volume Tao Xing, Pablo Caica, and Fed Sten bjective Deive and coelate the govening equations of motion in

More information

Remember: When an object falls due to gravity its potential energy decreases.

Remember: When an object falls due to gravity its potential energy decreases. Chapte 5: lectc Potental As mentoned seveal tmes dung the uate Newton s law o gavty and Coulomb s law ae dentcal n the mathematcal om. So, most thngs that ae tue o gavty ae also tue o electostatcs! Hee

More information

Unknown Input Based Observer Synthesis for a Polynomial T-S Fuzzy Model System with Uncertainties

Unknown Input Based Observer Synthesis for a Polynomial T-S Fuzzy Model System with Uncertainties 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

More information

Efficiency of the principal component Liu-type estimator in logistic

Efficiency 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 information

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15,

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15, Event Shape Update A. Eveett A. Savn T. Doyle S. Hanlon I. Skllcon Event Shapes, A. Eveett, U. Wsconsn ZEUS Meetng, Octobe 15, 2003-1 Outlne Pogess of Event Shapes n DIS Smla to publshed pape: Powe Coecton

More information

Generating Functions, Weighted and Non-Weighted Sums for Powers of Second-Order Recurrence Sequences

Generating 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 information

Chapter 3 Vector Integral Calculus

Chapter 3 Vector Integral Calculus hapte Vecto Integal alculus I. Lne ntegals. Defnton A lne ntegal of a vecto functon F ove a cuve s F In tems of components F F F F If,, an ae functon of t, we have F F F F t t t t E.. Fn the value of the

More information

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE LINEAR AND NONLINEAR ANALYSES O A WIND-TUNNEL INTRODUCTION BALANCE R. Kakehabadi and R. D. Rhew NASA LaRC, Hampton, VA The NASA Langley Reseach Cente (LaRC) has been designing stain-gauge balances fo utilization

More information

Chapter 5 Force and Motion

Chapter 5 Force and Motion Chapte 5 Foce and Motion In chaptes 2 and 4 we have studied kinematics i.e. descibed the motion of objects using paametes such as the position vecto, velocity and acceleation without any insights as to

More information

Vector Control. Application to Induction Motor Control. DSP in Motion Control - Seminar

Vector Control. Application to Induction Motor Control. DSP in Motion Control - Seminar Vecto Contol Application to Induction Moto Contol Vecto Contol - Pinciple The Aim of Vecto Contol is to Oient the Flux Poducing Component of the Stato Cuent to some Suitable Flux Vecto unde all Opeating

More information

Large scale magnetic field generation by accelerated particles in galactic medium

Large scale magnetic field generation by accelerated particles in galactic medium Lage scale magnetc feld geneaton by acceleated patcles n galactc medum I.N.Toptygn Sant Petesbug State Polytechncal Unvesty, depatment of Theoetcal Physcs, Sant Petesbug, Russa 2.Reason explonatons The

More information

Basic Electrohydrodynamics (Electrostatics) of the Floating Water Bridge

Basic Electrohydrodynamics (Electrostatics) of the Floating Water Bridge Basc lectohyoynamcs lectostatcs) o the loatng Wate Bge Wate has a emanent electc ole moment ue to ts molecula conguaton To scuss a ole, let us assume two ont chages, one wth chage +q an one wth chage q,

More information

Perturbation to Symmetries and Adiabatic Invariants of Nonholonomic Dynamical System of Relative Motion

Perturbation to Symmetries and Adiabatic Invariants of Nonholonomic Dynamical System of Relative Motion Commun. Theo. Phys. Beijing, China) 43 25) pp. 577 581 c Intenational Academic Publishes Vol. 43, No. 4, Apil 15, 25 Petubation to Symmeties and Adiabatic Invaiants of Nonholonomic Dynamical System of

More information

Capítulo. Three Dimensions

Capítulo. Three Dimensions Capítulo Knematcs of Rgd Bodes n Thee Dmensons Mecánca Contents ntoducton Rgd Bod Angula Momentum n Thee Dmensons Pncple of mpulse and Momentum Knetc Eneg Sample Poblem 8. Sample Poblem 8. Moton of a Rgd

More information

4/18/2005. Statistical Learning Theory

4/18/2005. Statistical Learning Theory Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse

More information

Research Article A Robust Longitudinal Control Strategy for Safer and Comfortable Automotive Driving

Research Article A Robust Longitudinal Control Strategy for Safer and Comfortable Automotive Driving Reseach Jounal of Appled Scences, Engneeng and Technology 7(3): 506-5033, 014 DOI:10.1906/jaset.7.896 ISSN: 040-7459; e-issn: 040-7467 014 Mawell Scentfc Publcaton Cop. Submtted: Febuay 18, 014 Accepted:

More information

V. 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.

V. 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 information

ScienceDirect. Dynamic model of a mobile robot

ScienceDirect. 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 information