Design of Optimal PID, Fuzzy and New Fuzzy-PID Controller for CANSAT Carrier System Thrust Vector
|
|
- Joan Davidson
- 5 years ago
- Views:
Transcription
1 In J Advanced esgn and Manufacung Technology, Vol 8/ No 2/ June esgn of Opmal PI, Fuzzy and New Fuzzy-PI Conolle fo CANSAT Cae Sysem Thus Veco A Kosa * epamen of New Scences and Technologes, Unvesy of Tehan, Ian E-mal: kosa_a@uac *Coespondng auho H Jahanshah & A A Razav epamen of New Scences and Technologes, Unvesy of Tehan, Ian E-mal: had_jahanshah@uac, aazav68@uac Receved: 4 Febuay 2015, Revsed: 7 Mach 2015, Acceped: 20 May 2015 Absac: In hs pape, mul-objecve opmzaon based on Genec Algohm s used o fnd he desgn vaables of PI, fuzzy and new Fuzzy-PI conolles applyng fo a hus veco conol of CANSAT cae sysem Moon veco conol s consdeed accodng o he dynamc govenng equaon of he sysem whch s deved usng Newon s mehod and defned msson n delveng payload no he specfc hegh and flgh pah angle The cos funcons of he sysem ae poson eo fom he se pon and devaon of he veco angle of cae sysem wh cae body, whee hese cos funcons mus be mnmzed smulaneously Resuls demonsae ha hs new Fuzzy-PI conolle s supeo o ohe conolles whch ae exeed n he hus veco conol of a CANSAT cae sysem Ths Fuzzy-PI s capable of dong he msson wh decease n selng me and se me wh espec o he convenen mnmzed objecve funcon values Keywods: Mul-objecve opmzaon, Genec algohm, PI-conolle, Fuzzy conolle, Fuzzy-PI conolle, CANSAT cae sysem Refeence: Kosa, A, Jahanshah, H, and Razav, A A, esgn of Opmal PI, Fuzzy and New Fuzzy-PI Conolle fo CANSAT Cae Sysem Thus Veco, In J of Advanced esgn and Manufacung Technology, Vol 8/No 2, 2015, pp 1-9 Bogaphcal noes: A R Kosa eceved hs Ph n Aeospace Engneeng fom Shaf Unvesy of Technology n 2003 He s cuenly Asssan Pofesso a he epamen of Aeospace and Mechaonc and Sysem Engneeng, Faculy of New Scence and Technologes, Unvesy of Tehan, Tehan, Ian Hs cuen eseach nees ncludes opmal conol and Pah Plannng H Jahanshah s MSc Suden of Aeospace engneeng a he Unvesy of Tehan, Ian He eceved hs BSc n Mechancal engneeng fom Sjan Unvesy of Technology Hs cuen eseach focuses on Fuzzy se and sysems A A Razav s MSc suden of Aeospace engneeng a he Unvesy of Tehan, Ian He eceved hs BSc n Mechancal engneeng fom Fedows Unvesy of Mashhad
2 2 In J Advanced esgn and Manufacung Technology, Vol 8/ No 2/ June INTROUCTION CANSAT s ae geng moe popula each day n aeospace engneeng cuculums because hey enable sudens o have paccal expeence on vual saelle launch opeaons and expeence he whole pocess of desgn, es, launch and ecovey emand fo anng of spacecaf engneeng s nceasng As paccal space engneeng s a elavely vey expensve feld, hee s an ongong seach fo affodable anng appoaches One of hese appoaches s CANSAT Launch concep whch was noduced by an Amecan Pofesso, Robe Twggs [1] He s a pofesso emeus a Sanfod Unvesy, who along wh Jod Pug-Sua of Calfona Polyechnc Sae Unvesy s esponsble fo ceang he CubeSa sandad fo mnauzed saelles and a sandad fo deploymen of he saelles He hough he could be egaded as he fahe of he mnaue saelles due o hs woks wh he ponees of hs dea [2] CANSAT s a desgn-bul-launch oganzaon whch s made by sudens The man goal of he CANSAT s o educae fuue engnees and scenss Ths pogam spead all ove he wold fom he USA and akes s name (CANSAT) fom he combnaon of "can" and "saelle" [3] The key feaues of a CANSAT desgn may be expessed as: Hgh Technology, Affodably and Lgh wegh The name of he saelle s deemned by he sze of he can "CANSAT" s a nanoscale saelle model, weghng 350 o 1050g These saelles ae launched by he ocke and can each a hegh of 150 o 2000m Afe geng sepaaed fom he saelle ockes, begns o pefom s dues n he couse of a fee fall These asks ae adaped o he ecen space mssons lke eafomng and a bag mssons [2] Havng he vaous sensos, ccus and mechancal componens conanng hese saelles, he CANSAT s he smalles sucue ha could be called a mnaue saelle I should be noed ha vehcles each vey low aludes, up o a few housand mees, whch s much lowe han ha he smalles soundng ockes can each [4] Ths small saelle s lef a a few hunded mees above he gound suface hen euns o he eah by he ecovey sysem Ths hegh s suffcen fo he payload opeaonal es and fgung ou ha CANSAT can pefom mssons smla o hose of eal saelles bu n a small lmed scale The CANSAT can handle dffeen knds of msson The mos mpoan known mssons exsng fo hs sysem whch ae suggesed fo elevan compeons nclude: Amosphee monong Imagng In addon o he pmay mssons of such flyng vehcles, menoned above, ecoveng and landng on a cean locaon o expandng anenna mechansm ae pas of he seconday msson of hs sysem In pevous compeons, CANSAT was usually caed by balloons and hen eleased a a specfc hegh, bu n new ounamens balloon s eplaced by he cayng sysem In hs case cayng sysems ae launched vecally and CANSAT s eleased a he specfc hegh wh specfc pah angle o he eah local hozon, hen a s hghes pon he cayng umbella s opened and lands slowly So, pah conolle desgn of cayng sysem fo delveng CANSAT s payload a he specfed hegh and deemned flgh condon plays an mpoan ole n he sysem desgn of hs msson Some eseaches caed ou n he feld of dffeen cayng pah conolle desgns (excep CANSAT), ae manly based on nonlnea conol mehods In ecen yeas, he developmen of Fuzzy-PI has become one of he majo eseach aeas n dffeen engneeng poblems The mos sgnfcan applcaons and sudes abou fuzzy sysems have concenaed on conol aeas, such as hose n [5], [6] Fuzzy sysems ae knowledge-based o ule-based sysems fomed va human knowledge and heuscs They have been appled o a wde ange of eseachng felds such as conol, communcaon, medcne, managemen, busness, psychology, and so foh The mos sgnfcan applcaons and sudes of he fuzzy sysems have concenaed on he conol aea, such as hose n Refs [7-12] The developmen of fuzzy PI conolles fo vaous engneeng poblems has been a majo eseach acvy n ecen yeas Along he way, he heusc paamees of Fuzzy-PI conolles have o be deemned va an appopae appoach A vey effecve way o choose hese facos s he use of evoluonay algohms, such as he genec algohm (GA) A consaned opmzaon of a smple Fuzzy-PI sysem s desgned fo he onlne mpovemen of PI conol pefomance whle unnng he poducve conol [13] In Ref [14], uan, L and eng poposed an nheen sauaon of he Fuzzy-PI conolle evealed due o he fne fuzzy ules In Ref [15], Oh, Jang, and Pedycz developed a desgn mehodology fo a fuzzy P cascade conolle fo a ball-beam sysem usng pacle swam opmzaon (PSO) In Ref [16], an on-lne unng mehod s poposed fo fuzzy PI conolles va ule weghng Boubeakh, Tadjne, Gloennec, and Labod poposed a new auo-unng fuzzy P and PI conolles usng enfocemen-leanng (QL) algohm fo SISO (sngle-npu sngle-oupu) and TITO (wo npu wooupu) sysems [17] Ne and Tan pesened an mpoved veson of he sable fuzzy adapve conol
3 In J Advanced esgn and Manufacung Technology, Vol 8/ No 2/ June sucue, whch compses an appoxmaon of he deal conolle and a supevsoy conolle [18] In hs pape a PI conolle, hen a fuzzy conolle and fnally a new Fuzzy-PI conolle s exeed on he hus veco of he CANSAT cae sysem In all of hese conolles, genec algohm s appled o fnd he bes conolle gans 2 CANSAT CARRYING SYSTEM YNAMIC MOELLING The fs sep n desgn of pah conol s denfcaon and exacon of dynamc govenng equaons of he sysem In mechancal sysems (such as aeospace sysems), hee ae vaous mehods such as Newon, Lagange, Keen and so foh fo modellng of sysem dynamcs The bes known of hese mehods s Newon's mehod whch s used n hs pape Fgue 1 shows a smplfed model of a cae sysem as θ s he cae longudnal veco angle wh decon of vecal o he eah and Φ s he cae hus veco angle wh decon of cae body Snce n he CANSAT sepaaon nsance fom s cae, he CANSAT velocy veco mage magnude on he hozon plane needs o be zeo, and also n he CANSAT opeaonal me, hs saelle s conneced wh gound saon hough ado waves, o educe he sgnal o nose ao (fuhe dsance equal o sgnal aenuaon and nose ncease), he conol pupose of hs poblem s eseng he angle of θ on zeo Theefoe, usng Newon's laws, govenng dynamc equaons of he sysem can ealze as follows: M CM I Whee M CM, I and α ae he momenum aound cene of mass, oaonal nea, and cae s angula acceleaon aound he axs pependcula o he plane, especvely Fg 1 Cae sysem scheme Fnally govenng dynamc equaon of he sysem s made as follows: 1 lm( a g) an( ) 2I Whee b s calculaed fom he followng equaon: 1 b lm( a g) 2I If we ake an( ) as u, equaon (1) becomes as follows: bu whee a s he acceleaon along pependcula axs, m s he mass of cae, g s he gavy acceleaon, and l s he lengh of cae The sae vaables ae he sysem obsevable sae veco whch s descbed as follows: x [ x1, x2, x3] [,, ] 3 OPTIMIZATION APPROACH Thee ae seveal mehods fo engneeng poblems opmzaon Ou seleced echnque s usng he genec algohm One advanage of genec algohm mehod s dealng wh funcon quany So, fo choosng he funcon, hee s no need o know s exac equaon and seems enough o fnd a way o calculae funcon value by eneng poblem vaables, unlke ohe opmzaon mehods ha eque havng he objecve funcon equaon exacly Eg f we could fnd he funcon value fo a specal case wh dffeen knd of vaables hough gaphcal mehods, hee s no need o know he elaon beween funcon and vaables, because he genec algohm mehod gves us he opmum value wh good accuacy Also, f we had a sofwae fo analyzng engneeng poblem whch could ge he vaables and gave he answe, we could oban he opmum value wh genec algohm only by knowng he value of funcon fo npu vaables wh no equemen of awaeness of soluon pocesses Ths s he unque advanage whch could be aely found n ohe opmzaon mehods In each opmzaon poblem we deal wh some goals whch ae menoned as objecve funcons These funcons ae hose vaables ha need o be mnmzed o maxmzed If we have only one objecve funcon, we encoune sngle-objecve opmzaon poblem, bu f we have moe han one objecve funcons we nvolve n mul-objecve o MOGA poblem, whee genec algohm es o opmze he desed values smulaneously MOGA s he abbevaon fom of
4 4 In J Advanced esgn and Manufacung Technology, Vol 8/ No 2/ June 2015 mul objecve based on genec algohm The objecve funcons n hs opmzaon ae poson eo fom he se poson, and devaon of veco angle of cae sysem wh cae body, descbed as follows: O F1 d O F2 d 4 PI CONTROLLER Sysem sae veco s x 1, x2, x3 whch ae negal of cae longudnal veco angle wh decon of vecal o he gound, cae longudnal veco angle wh decon of vecal o he gound and devaon of cae longudnal veco angle wh decon of vecal o he gound, especvely In PI conolle, advanced conolle can be ceaed consdeng paamees such as se pon changes wh espec o he cuen value of he pocess wh facos lke nensy and amoun of changes wh espec o me In PI conolles, popoonal-devave-negal algohm s used As comes fom s name, he lee P goes fo popoonal, I means negal and means evave Popoonal conolle deceases selng me and eo bu nceases oveshoo evave conolle deceases amoun of oveshoo and selng me and has less nfluence on se me and seady sae eo Inegal conolle deceases se me bu nceases oveshoo and selng me and emoves seady sae eo So a fs, he esponse of open loop and he values whch should be mpoved ae deemned We use Popoonal conolle fo se me mpovemen, devave conolle fo oveshoo mpovemen and negal conolle fo seady sae eo The gans of popoonal, devave and negal exeed n hs conolle accodng o he defned objecve funcons ae calculaed by usng genec algohm 5 FUZZY CONTROLLER Conolles wh fuzzy logc bass ae consdeed a subse of nellgen conol sysems Acually, nellgen conol sysems ae combnaon of conol engneeng and afcal nellgence (pogammng, easonng and leanng), whee fuzzy conolles ae no excluded fom hs law In ohe wods, fuzzy conolles ae song combnaon of nonlnea conols (conol engneeng) and fuzzy logc (nfeence) Thee ae some nfeence mehods n fuzzy logc One of hese mehods s Mamdan fuzzy nfeence sysem A Mamdan fuzzy nfeence sysem s made up of some lmed f-hen ules Fuzzy logc The fac ha cae hus foce mus be n a decon so ha could apply a oque n oppose of cae s head angle decon unl cae angle o he vecal lne become zeo, s he smples lngusc ule comes o he mnd Ths smple ule leads o a peodc sysem f he sysem nea s ovelooked ue o he Newon s laws, an objec keep movng a s unfom speed when hee s no foce on Theefoe, due o he nea law, sysem keeps movng a he same speed and cosses he zeo pon unl hus apples an oppose oque o he cae To solve hs poblem, cae angle velocy s eneed n he poblem n appled ules of makng decson So, he man ules of cae pah conol ae ewen as follows: 1- If he cae angle s negave and cae angle velocy s negave, hen hus veco s posve bg 2- If he cae angle s negave and cae angle velocy s nea o zeo (whou consdeng posve and negave), hen hus veco s posve small 3- If he cae angle s zeo (whou consdeng posve and negave) and cae angle velocy s negave hen hus veco s posve small 4- If he cae angle s zeo (whou consdeng posve and negave) and cae angle velocy s zeo (whou consdeng posve and negave) hen hus veco s posve zeo 5- If he cae angle s zeo (whou consdeng posve and negave) and cae angle velocy s posve hen hus veco s negave small 6- If he cae angle s posve and cae angle velocy s nea o zeo (whou consdeng posve and negave), hen hus veco s negave small 7- If he cae angle s posve and cae angle velocy s posve, hen hus veco s negave bg Fuzzfcaon Snce govenng equaon of cae dynamc sysem s connuous and dffeenable, s bee o use Gaussan funcons n fuzzfcaon The pupose of desgn s o make cae angle o he vecal lne zeo, so s necessay o have less ceon devaon n Gaussan funcon n he saemen of f cae angle s zeo han he ohe lngusc saemens The fuzzfcaon membeshp funcons of cae angle o he vecal axs ae shown n Fg 2
5 In J Advanced esgn and Manufacung Technology, Vol 8/ No 2/ June efuzzfcaon As menoned n above pa, govenng equaon of cae dynamc sysem s connuous and dffeenable So, s bee o use Gaussan funcons (whch ae dffeenable) n defuzzfcaon Moeove, usng Gaussan funcons esul n smooh pefomance of oupu ahe han usng ohe funcons such as angula o apezodal funcons ue o symmec popey of he sysem, Gaussan funcons ae consdeed homogeneous and symmec The defuzzfcaon membeshp funcons of hus angle ae shown n Fg 3 Fg 2 Fuzzfcaon of cae angle o he vecal axs Fg 3 efuzzfcaon of hus angle Takng Laplace ansfom fom Eq 4, and selecng conol paamee U as follows: U( s) ( w 0 w s)( ( s)) Closed loop ansfe funcon of he sysem becomes: ( s) U( s) s 2 0 bw s bw 0 bw s bw Fuzzy gan used n hs conolle accodng o he defned objecve funcons, poson eo fom he se pon, and devaon of he veco angle of cae sysem wh cae body s calculaed by genec algohm 6 FUZZY-PI CONTROLLER In he poposed new Fuzzy-PI conolle, wo fuzzy nfeence moos ae ulzed The fs s he Sngle Inpu Fuzzy Infeence Moo (SIFIM) ha has only one npu Snce all of he desed values n he sablzaon conol ae zeos, he vaables ae evesely npued no he Nom block Fo each nomalzed vaable (Nom block oupu), a SIFIM s defned The second s he Pefee Fuzzy Infeence Moo (PFIM) ha epesens he conol poy ode of each Nom block oupu j j j m : j 1 SIFIM { R : f x A henu C } SIFIM- menon he sngle npu nfeence moo whch accep he h j npu among npus and R s he j h ule of he sngle npu nfeence moo j A and C j ae he membeshp funcons Each npu em usually has a dffeen ole n mplemenaon of conol To expess he dffeen effecs of each npu em n he mplemenaon of sysem, sngle npu fuzzy nfeence moo defnes a dynamc mpoance degee ( w each npu em w ) fo w B w Whee w, B and w ae conol paamees whch ae descbed by fuzzy ules SIFIM- block calculae f as follows: VB f1 PO f2 ZB f f VB PO ZB 3 The membeshp funcons of SIFIMs ae shown n Fg 4 f 1, f 2 and f 3 (fuzzy ules of SIFIMs) noed n he above equaon, ae exploed fom he Table 1 Ohe ype of fuzzy nfeence moos ae PFIMs PFIMs guaanee CANSAT cae conol sysem when s deved fom desed values n one o moe of he coodnae sysem decons PFIM- calculae w as follows: W1 HS W2 HM W3 HB W1 W2 W3 HS HM HB The membeshp funcons of SIFIMs ae shown n Fg 4, and fuzzy ules of PFIMs ae shown n Table 2 Afe calculang f and w, s possble o defne new Fuzzy-PI conolle as he followng: f Kˆ ˆd Kˆ ˆ Kˆ p d dˆ d dˆ Whee f s he conol acon ˆ d, ˆ, ae he fuzzy d foms of d d,,, especvely, and should be d
6 6 In J Advanced esgn and Manufacung Technology, Vol 8/ No 2/ June 2015 obaned by SIFIM In ohe wods, ˆ ˆ ˆ d d f1; f 2; f3 Fuhemoe, n Eq 13, d ˆ Kˆ K p, and Kˆ d ae he fuzzy vaables calculaed by he followng equaons: ˆ b K K KW 1 ˆ b K K KW 2 ˆ b Kd Kd KdW 3 b b b Whee K, K and K d ae he base vaables K, K, and K d ae he egulaon vaables The base and egulaon vaables can be obaned by al and eo pocess Howeve, he bes soluon o have an opmal conol, s he use of opmzaon appoaches such as evoluonay algohms, especally genec algohm Fg 4 Membeshp funcons of SIFIM f Table 1 Fuzzy ules of SIFIMs Then VB f 1 1 PO f 2 0 ZB f SIMULATION AN RESULT Fo PI, fuzzy and Fuzzy-PI conolle, gan values and objecve funcon values elaed o hese gans ae shown n Tables 3, 4, 5, 6, 7 and 8, especvely The me esponses of cae poson o he vecal decon, cae angula velocy and cae hus veco angle wh cae body decon fo PI, fuzzy and Fuzzy-PI conolles ae shown n Fgues 6, 7, 8, 9, 10, 11, 13, 14 and 15 especvely Also, Smulaon of fuzzy conolle fo cae sysem n MATLAB, s shown n Fg 12 The sysem paamees used fo smulaon ae, m 100 kg, g 10 m s 2, l 1m, 100 m 2 a 2, I 1000kgm and he nom block faco s s 1 ad The nal values ae x [ x1, x2, x3] [0,02,0] and he algohm confguaon of he genec algohm (exs n he envonmen of MATLABR2012a) s as follows The cossove facon = 08, populaon sze = 200, selecon funcon = ounamen, muaon funcon =consan dependen, cossove funcon= nemedae, cossove ao= 1, mgaon decon= fowad, mgaon facon=02, mgaon neval= 20, dsance measue funcon=dsance cowdng, Paeo fon populaon funcon=035, and soppng cea s defned as funcon oleance = 10-4 Table 3 esgn vaables of opmum pon fo PI conolle esgn vaable value K p K d K Table 4 Objecve funcons of opmum pon fo PI conolle objecve funcon O F1 d O F2 d Fg 5 Membeshp funcons of PFIM Table 2 Fuzzy ules of PFIMs f Then HS W 1 1 HM W HB W 3 1 Table 5 esgn vaables of opmum pon fo fuzzy conolle esgn vaable w w Table 6 Objecve funcons of opmum pon fo fuzzy conolle objecve funcon O F1 d O F2 d 01961
7 In J Advanced esgn and Manufacung Technology, Vol 8/ No 2/ June Fg 6 Tme esponse of angula poson of PI conolle fo opmum pon Fg 10 Tme esponse of angula velocy of fuzzy conolle fo opmum pon Fg 7 Tme esponse of angula velocy of PI conolle fo opmum pon Fg 11 Tme esponse of hus veco angle of fuzzy conolle fo opmum pon Fg 8 Tme esponse of hus veco angle of PI conolle fo opmum pon Fg 12 Smulaon of fuzzy conolle fo cae sysem n MATLAB/SIMULINK Fg 9 Tme esponse of angula poson of fuzzy conolle fo opmum pon Table 7 esgn vaables of opmum pon fo Fuzzy-PI conolle esgn vaable b K b K b Kd K K Kd 09018
8 8 In J Advanced esgn and Manufacung Technology, Vol 8/ No 2/ June 2015 Table 8 Objecve funcons of opmum pon fo Fuzzy- PI conolle objecve funcon O F1 d O F2 d Fg 13 Tme esponse of angula poson of Fuzzy-PI conolle fo opmum pon mehod The objecve funcons fo hs sysem ae poson eo fom se pon and devaon of veco angle of cae sysem o cae body An negal em s augmened o he sae vaables due o seady sae eo elmnaon and se me decease In PI and fuzzy and Fuzzy-PI conolle, desgn vaables ae calculaed by usng genec algohm wh espec o defned objecve funcons Mamdan nfeence sysem wh some defned f-hen ules and Gaussan membeshp funcons fo fuzzfcaon and defuzzfcaon pas ae used n fuzzy conolle The new Fuzzy-PI conolle ulzes wo aveage nfeence engnes called SIFIM and PFIM whee he fs engne ge one npu fom each Nom block and gve f as oupus, and he second one guaanee CANSAT cae conol sysem n lage devaon fom desed values n one o moe of coodnae sysem decons and gve he W as oupus The epoed esuls demonsaed ha he poposed mehodology fo Fuzzy-PI conolle can conol CANSAT cae sysem effecvely ahe han appled PI and fuzzy conolles I s ecommended o denfy accuae dynamc of sysem and choose convenen fuzzy ules o mpove pefomance of conolles REFERENCES Fg 14 Tme esponse of angula velocy of Fuzzy-PI conolle fo opmum pon Fg 15 Tme esponse of hus veco angle of Fuzzy-PI conolle fo opmum pon 8 CONCLUSION In hs wok, he mul-objecve opmzaon was successfully used fo an opmum desgn of PI, fuzzy and new Fuzzy-PI conolles fo he CANSAT cae sysem whee he dynamc s deved by usng Newon s [1] Aydem, M E, usun, R C, and Pehlevan, M, Gound Saon esgn Pocedues fo CANSAT, he 6h Inenaonal Confeence on Recen Advanced n Space Technologes (RAST), Isanbul, Tukey, June 2013, pp [2] Soye, S, Small Space Can: CANSAT, n 5h Inenaonal Confeence on Recen Advanced n Space Technologes (RAST), Isanbul, Tukey, June 2011, pp [3] Çabuloğlu, C, Aykş, H, Yapacak, R, Çalşkan, E, Ağbuş, Ö, Abu, Ş, Soye, S, Tükmen, H, Ay, S, Kaaaş, Y, Aydem, M E, and Ҫeleb, M, Msson Analyss and Plannng of a CANSAT, The 5h Inenaonal Confeence on Recen Advanced n Space Technologes (RAST), Isanbul, Tukey, June 2011, pp [4] Oknnsk, A, Macnak, B, Bakowak, B, Kanewsk,, Mayszewsk, J, Kndack, J, and Wolansk, P, evelopmen of he Polsh Small Soundng Rocke Pogam, Aca Asonauca, Vol 108, 2015, pp [5] Zadeh, L A, Fuzzy algohms, Infomaon and Conol, Vol 12, 1968, pp [6] Zadeh, L A, Oulne of a new appoach o he analyss of complex sysems and decson pocesses, IEEE Tansacons on Sysems, Man and Cybenecs, Vol 3, 1973, pp [7] Nasse, H, Kefe-Kamal, E H, Hu, H, Belouea, S, and Bakanov, E, Acve vbaon dampng of
9 In J Advanced esgn and Manufacung Technology, Vol 8/ No 2/ June compose sucues usng a nonlnea fuzzy conolle, Compose Sucues, Vol 94, 2012, pp [8] LI, P, JIN, F J, Adapve Fuzzy Conol fo Unknown Nonlnea Sysems wh Peubed eadzone Inpus, Aca Auomaca Snca, Vol 36, 2010, pp [9] Lygouas, J N, Bosas, P N, Vouvoulaks, J, and Kodoganns, V, Fuzzy logc conolle mplemenaon fo a sola a-condonng sysem, Appled Enegy, Vol 84, 2007, pp [10] Jee, S, Koen, Y, Adapve fuzzy logc conolle fo feed dves of a CNC machne ool, Mechaoncs, Vol 14, 2004, pp [11] Snha, A S C, Lyshevsk, S, Fuzzy conol wh andom delays usng nvaan cones and s applcaon o conol of enegy pocesses n mcoelecomechancal moon devces, Enegy Conveson and Managemen, Vol 46, 2005, pp [12] Zupel, U, Cus, F, and Mlfelne, M, Fuzzy conol saegy fo an adapve foce conol n endmllng, Jounal of Maeals Pocessng Technology, Vol , 2005, pp [13] Mansou, S E, Kembe, G C, ubay, R, and Robeson, B, Onlne opmzaon of fuzzy-pi conol of a hemal pocess, ISA Tansacons, Vol 44, 2005, pp [14] uan, X G, L, H X, and eng, H, Robusness of fuzzy PI conolle due o s nheen sauaon, Jounal of Pocess Conol, Vol 22, 2012, pp [15] Oh, S K, Jang, H J, and Pedycz, W, Opmzed fuzzy P cascade conolle: A compaave analyss and desgn, Smulaon Modellng Pacce and Theoy, Vol 19, 2011, pp [16] Kaasakal, O, Guzelkaya, M, Eksn, I, Yesl, E, and Kumbasa, T, Onlne unng of fuzzy PI conolles va ule weghng based on nomalzed acceleaon, Engneeng Applcaons of Afcal Inellgence, Vol 26, 2013, pp [17] Boubeakh, H, Tadjne, M, Gloennec, P Y, and Labod, S, Tunng fuzzy P and PI conolles usng enfocemen leanng, ISA Tansacons, Vol 49, 2010, pp [18] Ne, M, Tan, W W, Sable adapve fuzzy P plus PI conolle fo nonlnea uncean sysems, Fuzzy Ses and Sysems, Vol 179, 2011, pp 1-19
5-1. We apply Newton s second law (specifically, Eq. 5-2). F = ma = ma sin 20.0 = 1.0 kg 2.00 m/s sin 20.0 = 0.684N. ( ) ( )
5-1. We apply Newon s second law (specfcally, Eq. 5-). (a) We fnd he componen of he foce s ( ) ( ) F = ma = ma cos 0.0 = 1.00kg.00m/s cos 0.0 = 1.88N. (b) The y componen of he foce s ( ) ( ) F = ma = ma
More informationName of the Student:
Engneeng Mahemacs 05 SUBJEC NAME : Pobably & Random Pocess SUBJEC CODE : MA645 MAERIAL NAME : Fomula Maeal MAERIAL CODE : JM08AM007 REGULAION : R03 UPDAED ON : Febuay 05 (Scan he above QR code fo he dec
More informationCHAPTER 10: LINEAR DISCRIMINATION
HAPER : LINEAR DISRIMINAION Dscmnan-based lassfcaon 3 In classfcaon h K classes ( k ) We defned dsmnan funcon g () = K hen gven an es eample e chose (pedced) s class label as f g () as he mamum among g
More informations = rθ Chapter 10: Rotation 10.1: What is physics?
Chape : oaon Angula poson, velocy, acceleaon Consan angula acceleaon Angula and lnea quanes oaonal knec enegy oaonal nea Toque Newon s nd law o oaon Wok and oaonal knec enegy.: Wha s physcs? In pevous
More informationHandling Fuzzy Constraints in Flow Shop Problem
Handlng Fuzzy Consans n Flow Shop Poblem Xueyan Song and Sanja Peovc School of Compue Scence & IT, Unvesy of Nongham, UK E-mal: {s sp}@cs.no.ac.uk Absac In hs pape, we pesen an appoach o deal wh fuzzy
More informationChapter 3: Vectors and Two-Dimensional Motion
Chape 3: Vecos and Two-Dmensonal Moon Vecos: magnude and decon Negae o a eco: eese s decon Mulplng o ddng a eco b a scala Vecos n he same decon (eaed lke numbes) Geneal Veco Addon: Tangle mehod o addon
More informationModern Energy Functional for Nuclei and Nuclear Matter. By: Alberto Hinojosa, Texas A&M University REU Cyclotron 2008 Mentor: Dr.
Moden Enegy Funconal fo Nucle and Nuclea Mae By: lbeo noosa Teas &M Unvesy REU Cycloon 008 Meno: D. Shalom Shlomo Oulne. Inoducon.. The many-body poblem and he aee-fock mehod. 3. Skyme neacon. 4. aee-fock
More information1 Constant Real Rate C 1
Consan Real Rae. Real Rae of Inees Suppose you ae equally happy wh uns of he consumpon good oday o 5 uns of he consumpon good n peod s me. C 5 Tha means you ll be pepaed o gve up uns oday n eun fo 5 uns
More informationField due to a collection of N discrete point charges: r is in the direction from
Physcs 46 Fomula Shee Exam Coulomb s Law qq Felec = k ˆ (Fo example, f F s he elecc foce ha q exes on q, hen ˆ s a un veco n he decon fom q o q.) Elecc Feld elaed o he elecc foce by: Felec = qe (elecc
More informationCptS 570 Machine Learning School of EECS Washington State University. CptS Machine Learning 1
ps 57 Machne Leann School of EES Washnon Sae Unves ps 57 - Machne Leann Assume nsances of classes ae lneal sepaable Esmae paamees of lnea dscmnan If ( - -) > hen + Else - ps 57 - Machne Leann lassfcaon
More informationReal-coded Quantum Evolutionary Algorithm for Global Numerical Optimization with Continuous Variables
Chnese Jounal of Eleconcs Vol.20, No.3, July 2011 Real-coded Quanum Evoluonay Algohm fo Global Numecal Opmzaon wh Connuous Vaables GAO Hu 1 and ZHANG Ru 2 (1.School of Taffc and Tanspoaon, Souhwes Jaoong
More informationDelay-Dependent Control for Time-Delayed T-S Fuzzy Systems Using Descriptor Representation
82 Inenaonal Jounal of Conol Auomaon and Sysems Vol 2 No 2 June 2004 Delay-Dependen Conol fo me-delayed -S Fuzzy Sysems Usng Descpo Repesenaon Eun ae Jeung Do Chang Oh and Hong Bae ak Absac: hs pape pesens
More informationJournal of Engineering Science and Technology Review 7 (1) (2014) Research Article
Jes Jounal o Engneeng Scence and echnology Revew 7 5 5 Reseach Acle JOURNAL OF Engneeng Scence and echnology Revew www.jes.og Sudy on Pedcve Conol o ajecoy ackng o Roboc Manpulao Yang Zhao Dep. o Eleconc
More informationNew Stability Condition of T-S Fuzzy Systems and Design of Robust Flight Control Principle
96 JOURNAL O ELECRONIC SCIENCE AND ECHNOLOGY, VOL., NO., MARCH 3 New Sably Conon of -S uzzy Sysems an Desgn of Robus lgh Conol Pncple Chun-Nng Yang, Ya-Zhou Yue, an Hu L Absac Unlke he pevous eseach woks
More informationHierarchical Production Planning in Make to Order System Based on Work Load Control Method
Unvesal Jounal of Indusal and Busness Managemen 3(): -20, 205 DOI: 0.389/ujbm.205.0300 hp://www.hpub.og Heachcal Poducon Plannng n Make o Ode Sysem Based on Wok Load Conol Mehod Ehsan Faah,*, Maha Khodadad
More informationSCIENCE CHINA Technological Sciences
SIENE HINA Technologcal Scences Acle Apl 4 Vol.57 No.4: 84 8 do:.7/s43-3-5448- The andom walkng mehod fo he seady lnea convecondffuson equaon wh axsymmec dsc bounday HEN Ka, SONG MengXuan & ZHANG Xng *
More informationLecture 5. Plane Wave Reflection and Transmission
Lecue 5 Plane Wave Reflecon and Tansmsson Incden wave: 1z E ( z) xˆ E (0) e 1 H ( z) yˆ E (0) e 1 Nomal Incdence (Revew) z 1 (,, ) E H S y (,, ) 1 1 1 Refleced wave: 1z E ( z) xˆ E E (0) e S H 1 1z H (
More informationInteger Programming Models for Decision Making of. Order Entry Stage in Make to Order Companies 1. INTRODUCTION
Inege Pogammng Models fo Decson Makng of Ode Eny Sage n Make o Ode Companes Mahendawah ER, Rully Soelaman and Rzal Safan Depamen of Infomaon Sysems Depamen of Infomacs Engneeng Insu eknolog Sepuluh Nopembe,
More informationFast Calibration for Robot Welding System with Laser Vision
Fas Calbaon fo Robo Weldng Ssem h Lase Vson Lu Su Mechancal & Eleccal Engneeng Nanchang Unves Nanchang, Chna Wang Guoong Mechancal Engneeng Souh Chna Unves of echnolog Guanghou, Chna Absac Camea calbaon
More informationCHAPTER 3 DETECTION TECHNIQUES FOR MIMO SYSTEMS
4 CAPTER 3 DETECTION TECNIQUES FOR MIMO SYSTEMS 3. INTRODUCTION The man challenge n he paccal ealzaon of MIMO weless sysems les n he effcen mplemenaon of he deeco whch needs o sepaae he spaally mulplexed
More informationI-POLYA PROCESS AND APPLICATIONS Leda D. Minkova
The XIII Inenaonal Confeence Appled Sochasc Models and Daa Analyss (ASMDA-009) Jne 30-Jly 3, 009, Vlns, LITHUANIA ISBN 978-9955-8-463-5 L Sakalaskas, C Skadas and E K Zavadskas (Eds): ASMDA-009 Seleced
More informationScienceDirect. Behavior of Integral Curves of the Quasilinear Second Order Differential Equations. Alma Omerspahic *
Avalable onlne a wwwscencedeccom ScenceDec oceda Engneeng 69 4 85 86 4h DAAAM Inenaonal Smposum on Inellgen Manufacung and Auomaon Behavo of Inegal Cuves of he uaslnea Second Ode Dffeenal Equaons Alma
More informationOptimized Braking Force Distribution during a Braking-in- Turn Maneuver for Articulated Vehicles
56 Opmzed Bakng Foce Dsbuon dung a Bakng-n- Tun Maneuve o Aculaed Vehcles E. Esmalzadeh, A. Goodaz and M. Behmad 3 Downloaded om www.us.ac. a 3:04 IRST on Fday Novembe 3d 08,* Faculy o Engneeng and Appled
More informationp E p E d ( ) , we have: [ ] [ ] [ ] Using the law of iterated expectations, we have:
Poblem Se #3 Soluons Couse 4.454 Maco IV TA: Todd Gomley, gomley@m.edu sbued: Novembe 23, 2004 Ths poblem se does no need o be uned n Queson #: Sock Pces, vdends and Bubbles Assume you ae n an economy
More informationL4:4. motion from the accelerometer. to recover the simple flutter. Later, we will work out how. readings L4:3
elave moon L4:1 To appl Newon's laws we need measuemens made fom a 'fed,' neal efeence fame (unacceleaed, non-oang) n man applcaons, measuemens ae made moe smpl fom movng efeence fames We hen need a wa
More informationUniversity of California, Davis Date: June xx, PRELIMINARY EXAMINATION FOR THE Ph.D. DEGREE ANSWER KEY
Unvesy of Calfona, Davs Dae: June xx, 009 Depamen of Economcs Tme: 5 hous Mcoeconomcs Readng Tme: 0 mnues PRELIMIARY EXAMIATIO FOR THE Ph.D. DEGREE Pa I ASWER KEY Ia) Thee ae goods. Good s lesue, measued
More informationN 1. Time points are determined by the
upplemena Mehods Geneaon of scan sgnals In hs secon we descbe n deal how scan sgnals fo 3D scannng wee geneaed. can geneaon was done n hee seps: Fs, he dve sgnal fo he peo-focusng elemen was geneaed o
More informationA hybrid method to find cumulative distribution function of completion time of GERT networks
Jounal of Indusal Engneeng Inenaonal Sepembe 2005, Vol., No., - 9 Islamc Azad Uvesy, Tehan Souh Banch A hybd mehod o fnd cumulave dsbuon funcon of compleon me of GERT newos S. S. Hashemn * Depamen of Indusal
More informationCourse Outline. 1. MATLAB tutorial 2. Motion of systems that can be idealized as particles
Couse Oulne. MATLAB uoal. Moon of syses ha can be dealzed as pacles Descpon of oon, coodnae syses; Newon s laws; Calculang foces equed o nduce pescbed oon; Deng and solng equaons of oon 3. Conseaon laws
More informationThe Unique Solution of Stochastic Differential Equations. Dietrich Ryter. Midartweg 3 CH-4500 Solothurn Switzerland
The Unque Soluon of Sochasc Dffeenal Equaons Dech Rye RyeDM@gawne.ch Mdaweg 3 CH-4500 Solohun Swzeland Phone +4132 621 13 07 Tme evesal n sysems whou an exenal df sngles ou he an-iô negal. Key wods: Sochasc
More informationMolecular dynamics modeling of thermal and mechanical properties
Molecula dynamcs modelng of hemal and mechancal popees Alejando Sachan School of Maeals Engneeng Pudue Unvesy sachan@pudue.edu Maeals a molecula scales Molecula maeals Ceamcs Meals Maeals popees chas Maeals
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More informationA VISCOPLASTIC MODEL OF ASYMMETRICAL COLD ROLLING
SISOM 4, BUCHAEST, - May A VISCOPLASTIC MODEL OF ASYMMETICAL COLD OLLING odca IOAN Spu Hae Unvesy Buchaes, odcaoan7@homal.com Absac: In hs pape s gven a soluon of asymmecal sp ollng poblem usng a Bngham
More informationChapter Finite Difference Method for Ordinary Differential Equations
Chape 8.7 Fne Dffeence Mehod fo Odnay Dffeenal Eqaons Afe eadng hs chape, yo shold be able o. Undesand wha he fne dffeence mehod s and how o se o solve poblems. Wha s he fne dffeence mehod? The fne dffeence
More informationSolution of Non-homogeneous bulk arrival Two-node Tandem Queuing Model using Intervention Poisson distribution
Volume-03 Issue-09 Sepembe-08 ISSN: 455-3085 (Onlne) RESEARCH REVIEW Inenaonal Jounal of Muldscplnay www.jounals.com [UGC Lsed Jounal] Soluon of Non-homogeneous bulk aval Two-node Tandem Queung Model usng
More informationComputer Propagation Analysis Tools
Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion
More informationPhysics 201 Lecture 15
Phscs 0 Lecue 5 l Goals Lecue 5 v Elo consevaon of oenu n D & D v Inouce oenu an Iulse Coens on oenu Consevaon l oe geneal han consevaon of echancal eneg l oenu Consevaon occus n sses wh no ne eenal foces
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationFIRMS IN THE TWO-PERIOD FRAMEWORK (CONTINUED)
FIRMS IN THE TWO-ERIO FRAMEWORK (CONTINUE) OCTOBER 26, 2 Model Sucue BASICS Tmelne of evens Sa of economc plannng hozon End of economc plannng hozon Noaon : capal used fo poducon n peod (decded upon n
More informationRotor profile design in a hypogerotor pump
Jounal of Mechancal Scence and Technology (009 459~470 Jounal of Mechancal Scence and Technology www.spngelnk.com/conen/78-494x DOI 0.007/s06-009-007-y oo pofle desgn n a hypogeoo pump Soon-Man Kwon *,
More informationSuppose we have observed values t 1, t 2, t n of a random variable T.
Sppose we have obseved vales, 2, of a adom vaable T. The dsbo of T s ow o belog o a cea ype (e.g., expoeal, omal, ec.) b he veco θ ( θ, θ2, θp ) of ow paamees assocaed wh s ow (whee p s he mbe of ow paamees).
More informationajanuary't I11 F or,'.
',f,". ; q - c. ^. L.+T,..LJ.\ ; - ~,.,.,.,,,E k }."...,'s Y l.+ : '. " = /.. :4.,Y., _.,,. "-.. - '// ' 7< s k," ;< - " fn 07 265.-.-,... - ma/ \/ e 3 p~~f v-acecu ean d a e.eng nee ng sn ~yoo y namcs
More informationRadial Motion of Two Mutually Attracting Particles
Radal Moon of Two Muually Aacng Pacles Cal E. Mungan, U.S. Naval Academy, Annapols, MD A pa of masses o oppose-sgn chages eleased fom es wll move decly owad each ohe unde he acon of he nvesedsance-squaed
More informationChapters 2 Kinematics. Position, Distance, Displacement
Chapers Knemacs Poson, Dsance, Dsplacemen Mechancs: Knemacs and Dynamcs. Knemacs deals wh moon, bu s no concerned wh he cause o moon. Dynamcs deals wh he relaonshp beween orce and moon. The word dsplacemen
More informationReflection and Refraction
Chape 1 Reflecon and Refacon We ae now neesed n eplong wha happens when a plane wave avelng n one medum encounes an neface (bounday) wh anohe medum. Undesandng hs phenomenon allows us o undesand hngs lke:
More information( ) ( )) ' j, k. These restrictions in turn imply a corresponding set of sample moment conditions:
esng he Random Walk Hypohess If changes n a sees P ae uncoelaed, hen he followng escons hold: va + va ( cov, 0 k 0 whee P P. k hese escons n un mply a coespondng se of sample momen condons: g µ + µ (,,
More information[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5
TPG460 Reservor Smulaon 08 page of 5 DISCRETIZATIO OF THE FOW EQUATIOS As we already have seen, fne dfference appromaons of he paral dervaves appearng n he flow equaons may be obaned from Taylor seres
More informationOutline. GW approximation. Electrons in solids. The Green Function. Total energy---well solved Single particle excitation---under developing
Peenaon fo Theoecal Condened Mae Phyc n TU Beln Geen-Funcon and GW appoxmaon Xnzheng L Theoy Depamen FHI May.8h 2005 Elecon n old Oulne Toal enegy---well olved Sngle pacle excaon---unde developng The Geen
More informationcalculating electromagnetic
Theoeal mehods fo alulang eleomagne felds fom lghnng dshage ajeev Thoapplll oyal Insue of Tehnology KTH Sweden ajeev.thoapplll@ee.kh.se Oulne Despon of he poblem Thee dffeen mehods fo feld alulaons - Dpole
More informationto Assess Climate Change Mitigation International Energy Workshop, Paris, June 2013
Decomposng he Global TIAM-Maco Maco Model o Assess Clmae Change Mgaon Inenaonal Enegy Wokshop Pas June 2013 Socaes Kypeos (PSI) & An Lehla (VTT) 2 Pesenaon Oulne The global ETSAP-TIAM PE model and he Maco
More informationSimulation of Non-normal Autocorrelated Variables
Jounal of Moden Appled Sascal Mehods Volume 5 Issue Acle 5 --005 Smulaon of Non-nomal Auocoelaed Vaables HT Holgesson Jönöpng Inenaonal Busness School Sweden homasholgesson@bshse Follow hs and addonal
More informationCubic Bezier Homotopy Function for Solving Exponential Equations
Penerb Journal of Advanced Research n Compung and Applcaons ISSN (onlne: 46-97 Vol. 4, No.. Pages -8, 6 omoopy Funcon for Solvng Eponenal Equaons S. S. Raml *,,. Mohamad Nor,a, N. S. Saharzan,b and M.
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 information) from i = 0, instead of i = 1, we have =
Chape 3: Adjusmen Coss n he abou Make I Movaonal Quesons and Execses: Execse 3 (p 6): Illusae he devaon of equaon (35) of he exbook Soluon: The neempoal magnal poduc of labou s epesened by (3) = = E λ
More informationReinforcement learning
Lecue 3 Reinfocemen leaning Milos Hauskech milos@cs.pi.edu 539 Senno Squae Reinfocemen leaning We wan o lean he conol policy: : X A We see examples of x (bu oupus a ae no given) Insead of a we ge a feedback
More informationSTABILITY CRITERIA FOR A CLASS OF NEUTRAL SYSTEMS VIA THE LMI APPROACH
Asan Jounal of Conol, Vol. 6, No., pp. 3-9, Mach 00 3 Bef Pape SABILIY CRIERIA FOR A CLASS OF NEURAL SYSEMS VIA HE LMI APPROACH Chang-Hua Len and Jen-De Chen ABSRAC In hs pape, he asypoc sably fo a class
More informationAn axisymmetric incompressible lattice BGK model for simulation of the pulsatile ow in a circular pipe
INTERNATIONAL JOURNAL FOR NUMERICAL METHODS IN FLUIDS In. J. Nume. Meh. Fluds 005; 49:99 116 Publshed onlne 3 June 005 n Wley IneScence www.nescence.wley.com). DOI: 10.100/d.997 An axsymmec ncompessble
More informationTHE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS
THE PREICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS INTROUCTION The wo dmensonal paral dfferenal equaons of second order can be used for he smulaon of compeve envronmen n busness The arcle presens he
More informationMCTDH Approach to Strong Field Dynamics
MCTDH ppoach o Song Feld Dynamcs Suen Sukasyan Thomas Babec and Msha Ivanov Unvesy o Oawa Canada Impeal College ondon UK KITP Sana Babaa. May 8 009 Movaon Song eld dynamcs Role o elecon coelaon Tunnel
More informationSolution in semi infinite diffusion couples (error function analysis)
Soluon n sem nfne dffuson couples (error funcon analyss) Le us consder now he sem nfne dffuson couple of wo blocks wh concenraon of and I means ha, n a A- bnary sysem, s bondng beween wo blocks made of
More information, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t
Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission
More informationNumerical Study of Large-area Anti-Resonant Reflecting Optical Waveguide (ARROW) Vertical-Cavity Semiconductor Optical Amplifiers (VCSOAs)
USOD 005 uecal Sudy of Lage-aea An-Reonan Reflecng Opcal Wavegude (ARROW Vecal-Cavy Seconduco Opcal Aplfe (VCSOA anhu Chen Su Fung Yu School of Eleccal and Eleconc Engneeng Conen Inoducon Vecal Cavy Seconduco
More informationI-Hsuan Hong Hsi-Mei Hsu Yi-Mu Wu Chun-Shao Yeh
Poceedngs of he 8 Wne Smulaon Confeence S. J. ason, R. R. Hll, L. önch, O. Rose, T. Jeffeson, J. W. Fowle eds. PRICING DECISION AND LEAD TIE SETTING IN A DUOPOL SEICONDUCTOR INDUSTR I-Hsuan Hong Hs-e Hsu
More informationA Novel Fast Otsu Digital Image Segmentation Method
The Inenaonal Aab Jounal of Infomaon Technology, Vol. 3, No. 4, July 06 47 A Novel Fas Osu Dgal Image Segmenaon Mehod Duaa AlSaeed,, Ahmed oudane,, and Al El-Zaa 3 Depamen of Compue Scence and Dgal Technologes,
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 information8. HAMILTONIAN MECHANICS
8. HAMILTONIAN MECHANICS In ode o poceed fom he classcal fomulaon of Maxwell's elecodynamcs o he quanum mechancal descpon a new mahemacal language wll be needed. In he pevous secons he elecomagnec feld
More informationWhen to Treat Prostate Cancer Patients Based on their PSA Dynamics
When o Tea Posae Cance Paens Based on he PSA Dynamcs CLARA day on opeaons eseach n cance eamen & opeaons managemen Novembe 7 00 Mael S. Lave PhD Man L. Pueman PhD Sco Tyldesley M.D. Wllam J. Mos M.D CIHR
More informationAccelerated Sequen.al Probability Ra.o Test (SPRT) for Ongoing Reliability Tes.ng (ORT)
cceleaed Sequen.al Pobably Ra.o Tes (SPRT) fo Ongong Relably Tes.ng (ORT) Mlena Kasch Rayheon, IDS Copygh 25 Rayheon Company. ll ghs eseved. Cusome Success Is Ou Msson s a egseed adema of Rayheon Company
More informationHeuristic Unit Commitment of Wind Farms Integrated in Power System Consideration with Demand Response
Avalable onlne a www.scnze.com Scnze Jounal of Engneeng, ol 3, Issue 1, (2017): 40-47 DOI: 10.21634/SJE.3.1.4047 ISSN 2415-105X Heusc Un Commmen of Wnd Fams Inegaed n Powe Sysem Consdeaon wh Demand Response
More informationAnswers to Tutorial Questions
Inoducoy Mahs ouse Answes.doc Answes o Tuoal Quesons Enjoy wokng hough he examples. If hee ae any moe quesons, please don hesae o conac me. Bes of luck fo he exam and beyond, I hope you won need. Tuoal
More informationESS 265 Spring Quarter 2005 Kinetic Simulations
SS 65 Spng Quae 5 Knec Sulaon Lecue une 9 5 An aple of an lecoagnec Pacle Code A an eaple of a knec ulaon we wll ue a one denonal elecoagnec ulaon code called KMPO deeloped b Yohhau Oua and Hoh Mauoo.
More informationAdaptive complex modified hybrid function projective synchronization of different dimensional complex chaos with uncertain complex parameters
Nonlnea Dyn (26) 83:9 2 DOI.7/s7--239-8 ORIGINAL PAPER Adapve complex modfed hybd funcon pojecve synchonzaon of dffeen dmensonal complex chaos wh uncean complex paamees Jan Lu Shuang Lu Julen Clnon Spo
More informationThe balanced budget multiplier and labour intensity in home production
Inenaonal Jounal of Economc Behavo and Oganzaon 205; 3(2-): 23-30 Publshed onlne Febuay 26, 205 (hp://www.scencepublshnggoup.com/j/jebo) do: 0.648/j.jebo.s.20503020.5 ISSN: 2328-7608 (Pn); ISSN: 2328-766
More informationVariants of Pegasos. December 11, 2009
Inroducon Varans of Pegasos SooWoong Ryu bshboy@sanford.edu December, 009 Youngsoo Cho yc344@sanford.edu Developng a new SVM algorhm s ongong research opc. Among many exng SVM algorhms, we wll focus on
More informationWORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done
More informationAn Exact Resource Allocation Model with Hard and Soft Resource Constraints
An Exac Resouce Allocaon Model wh Had and Sof Resouce Consans Sxeenh Annual Confeence of POMS, Chcago, IL, Apl 29 - May 2, 2005. Feenc Kuzslcz (kuzslc@kk.pe.hu) nvesy of Pécs, Depamen of Busness Infomacs,
More informationA multiple-relaxation-time lattice Boltzmann model for simulating. incompressible axisymmetric thermal flows in porous media
A mulple-elaxaon-me lace Bolmann model fo smulang ncompessble axsymmec hemal flows n poous meda Qng Lu a, Ya-Lng He a, Qng L b a Key Laboaoy of Themo-Flud Scence and Engneeng of Mnsy of Educaon, School
More informationDEVELOPMENT OF A PROGRAMMABLE LOAD
DEVELOPMENT OF A POGAMMABLE LOAD Ulch John Mnnaa A dsseaon submed o he Faculy of Engneeng, Unvesy of he Wwaesand, n fulflmen of he equemens fo he degee of Mase of cence n Engneeng. Johannesbug, 2006 DECLAATION
More informationUnsupervised Cross-Domain Transfer in Policy Gradient Reinforcement Learning via Manifold Alignment
Unsupevsed Coss-Doman ansfe n Polcy Gaden Renfocemen Leanng va Manfold Algnmen Haham Bou Amma Unv. of Pennsylvana hahamb@seas.upenn.edu Ec Eaon Unv. of Pennsylvana eeaon@cs.upenn.edu Paul Ruvolo Oln College
More informationMIMO Capacity for UWB Channel in Rectangular Metal Cavity
MMO Capacy o UB Channel n Recangula Meal Cavy Zhen u, Dalwnde ngh Depamen o Eleccal and Compue Engneeng Cene o Manuacung Reseach Tennessee Tech Unvesy zhu@nech.edu, dsngh@nech.edu Robe Qu (Conac Auho)
More informationThe Application of Fuzzy Comprehensive Evaluations in The College Education Informationization Level
IOSR Jounal of Reseach & Mehod n Educaon IOSR-JRME) e- ISSN: 3 7388,p-ISSN: 3 737X Volume 8, Issue 3 Ve IV May June 8), PP -7 wwwosjounalsog The Applcaon of Fuzzy Compehensve Evaluaons n The College Educaon
More informationCombinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions
Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,
More informationMATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH
Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias
More informationMonetary policy and models
Moneay polcy and odels Kes Næss and Kes Haae Moka Noges Bank Moneay Polcy Unvesy of Copenhagen, 8 May 8 Consue pces and oney supply Annual pecenage gowh. -yea ovng aveage Gowh n oney supply Inflaon - 9
More informationEfficient Bayesian Network Learning for System Optimization in Reliability Engineering
Qualy Technology & Quanave Managemen Vol. 9, No., pp. 97-, 202 QTQM ICAQM 202 Effcen Bayesan Newok Leanng fo Sysem Opmzaon n Relably Engneeng A. Gube and I. Ben-Gal Depamen of Indusal Engneeng, Faculy
More informationLecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation
Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion
More information( ) () we define the interaction representation by the unitary transformation () = ()
Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger
More informationAPPROXIMATIONS FOR AND CONVEXITY OF PROBABILISTICALLY CONSTRAINED PROBLEMS WITH RANDOM RIGHT-HAND SIDES
R U C O R R E S E A R C H R E P O R APPROXIMAIONS FOR AND CONVEXIY OF PROBABILISICALLY CONSRAINED PROBLEMS WIH RANDOM RIGH-HAND SIDES M.A. Lejeune a A. PREKOPA b RRR 7-005, JUNE 005 RUCOR Ruges Cene fo
More informationOrdinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s
Ordnary Dfferenal Equaons n Neuroscence wh Malab eamples. Am - Gan undersandng of how o se up and solve ODE s Am Undersand how o se up an solve a smple eample of he Hebb rule n D Our goal a end of class
More informationTecnologia e Inovação, Lisboa, Portugal. ABB Corporate Research Center, Wallstadter Str. 59, Ladenburg, Germany,
A New Connuous-Tme Schedulng Fomulaon fo Connuous Plans unde Vaable Eleccy Cos Pedo M. Caso * Io Hajunkosk and Ignaco E. Gossmann Depaameno de Modelação e Smulação de Pocessos Insuo Naconal de Engenhaa
More information( ) ( ) Weibull Distribution: k ti. u u. Suppose t 1, t 2, t n are times to failure of a group of n mechanisms. The likelihood function is
Webll Dsbo: Des Bce Dep of Mechacal & Idsal Egeeg The Uvesy of Iowa pdf: f () exp Sppose, 2, ae mes o fale of a gop of mechasms. The lelhood fco s L ( ;, ) exp exp MLE: Webll 3//2002 page MLE: Webll 3//2002
More informationDynamic Team Decision Theory. EECS 558 Project Shrutivandana Sharma and David Shuman December 10, 2005
Dynamc Team Decson Theory EECS 558 Proec Shruvandana Sharma and Davd Shuman December 0, 005 Oulne Inroducon o Team Decson Theory Decomposon of he Dynamc Team Decson Problem Equvalence of Sac and Dynamc
More informationLOW-LOSS TUNING CIRCUITS FOR FREQUENCY-TUNABLE SMALL RESONANT ANTENNAS
LOW-LOSS TUNING CIRCUITS FOR FREQUENCY-TUNABLE SMALL RESONANT ANTENNAS Jan Ollkanen 1,, Ou Kvekäs 1,3, and Pe Vankanen 1,4 1 Helsnk Unvesy o Technology, Insue o Dgal Communcaons, Rado Laboaoy, P.O. Box
More informationHEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD
Journal of Appled Mahemacs and Compuaonal Mechancs 3, (), 45-5 HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD Sansław Kukla, Urszula Sedlecka Insue of Mahemacs,
More informationCHAPTER 10: LINEAR DISCRIMINATION
CHAPER : LINEAR DISCRIMINAION Dscrmnan-based Classfcaon 3 In classfcaon h K classes (C,C,, C k ) We defned dscrmnan funcon g j (), j=,,,k hen gven an es eample, e chose (predced) s class label as C f g
More informationGraduate Macroeconomics 2 Problem set 5. - Solutions
Graduae Macroeconomcs 2 Problem se. - Soluons Queson 1 To answer hs queson we need he frms frs order condons and he equaon ha deermnes he number of frms n equlbrum. The frms frs order condons are: F K
More informationAn Open cycle and Closed cycle Gas Turbine Engines. Methods to improve the performance of simple gas turbine plants
An Open cycle and losed cycle Gas ubine Engines Mehods o impove he pefomance of simple gas ubine plans I egeneaive Gas ubine ycle: he empeaue of he exhaus gases in a simple gas ubine is highe han he empeaue
More informationA Methodology for Detecting the Change of Customer Behavior based on Association Rule Mining
A Mehodology fo Deecng he Change of Cusome Behavo based on Assocaon Rule Mnng Hee Seo Song, Soung He Km KAIST Gaduae School of Managemen Jae Kyeong Km KyungHee Unvesy Absac Undesandng and adapng o changes
More informationCircular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.
1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule
More informationRelative and Circular Motion
Relaie and Cicula Moion a) Relaie moion b) Cenipeal acceleaion Mechanics Lecue 3 Slide 1 Mechanics Lecue 3 Slide 2 Time on Video Pelecue Looks like mosly eeyone hee has iewed enie pelecue GOOD! Thank you
More information