A New Nonlinear Excitation Controller for Synchronous Power Generator

Size: px
Start display at page:

Download "A New Nonlinear Excitation Controller for Synchronous Power Generator"

Transcription

1 Proc. of he 5h WSEAS/IASME In. Conf. on Elecrc Power Sysems, Hgh Volages, Elecrc Machnes, Tenerfe, Span, December 16-18, 2005 (pp98-103) A New Nonlnear Excaon Conroller for Synchronous Power Generaor M. OUASSAID*, A. NEJEMI**, M. CHERKAOUI* * Deparmen of Elecrcal Engneerng, Ecole Mohammaa ngéneur, Mohamme V Unersy, B.P. 765, Agal, Raba, Morocco **Faculé es scences e echnques Benmellal, Ka Ayya unersy, Marrakech, Morocco Absrac: - Ths paper presens a new an smple conroller for ransen sablzaon wh olage regulaon of a synchronous power generaor connece o an nfne bus. The oerall sably of he sysem s shown usng Lyapuno echnque. The esgn of he propose conroller akes no accoun he mporan non lneares of he power sysem moel an s nepenen of he equlbrum pon. Smulaon resuls hae been shown o emonsrae he effeceness of he propose conroller for he enhancemen of he ransen sably an olage regulaon of he power sysem uner a large suen faul an a we range of operang conons. Key-Wors: - Excaon conrol, Lyapuno echnque, non lnear conrol, synchronous generaor, ransen sably, olage regulaon 1 Inroucon The hgh complexy an nonlneary of power sysems, ogeher wh her almos connuously me aryng naure, hae eal of challenge of power sysem conrol engneers for ecaes. A parcular ssue encounere a he generang plan leel s o manan sably uner arous operang conons. In orer o oban hgh qualy for synchronous generaor conrollers, many researches has been esablshe an numerous paper are publshe. Conenonal excaon conrollers such as he auomac olage regulaor (AVR) an power sysem sablzer (PSS) are manly esgne by usng lnear conrol heory [1], [2]. These excaon conrollers can be use effecely o amp oscllaon an nsure asympoc sably of he equlbrum followng small perurbaon. In case of a large faul, he operang pon of he sysem may ary conserably; non lneares begn o hae hen sgnfcan effecs an a lnear conrollers may no be able o manan asympoc sably [3]. Recenly, aance nonlnear conroller echnque, whch are nepenen of he equlbrum pon an ake no accoun he mporan non-lneares of he power sysem moel hae been use n he excaon conrol of power sysems [4], [5], [6]. Mos of hese conrollers are base on feeback lnearzaon echnque [3], [7], [8]. I was shown n he leraures ha he ynamcs of he power sysem coul be exacly lnearze by employng nonlnear sae feeback. The essence of hs echnque s o frs ransform a nonlnear sysem no a lnear on by a nonlnear feeback, an hen uses he well-known lnear esgn echnques o complee he conroller esgn. Consequenly one can use conenonal lnear conrol o ge accepable performance [9], [10] an [11]. Neerheless n many cases he feeback lnearzaon meho requres precse parameers plan an ofen cancels some useful non-lneares. I s well known ha power sysems conan some paramerc unceranes n pracce. In hs case, s ffcul o exacly lnearze he sysem wh nomnal parameers. Aape ersons of he feeback lnearzng conrols are hen eelope n [12], [13]. Feeback lnearzaon s recenly enhance by usng robus conrol esgns such as H conrol an L2 surbance aenuaon [14], [15]. Lyapuno heory has for a long me been an mporan ool n lnear as well as nonlnear conrol [16]. Howeer, s use whn nonlnear conrol has been hampere by he ffcules o fn a Lyapuno funcon for a gen sysem. If one can be foun, he sysem s known o be sable, bu he ask of fnng such a funcon has ofen been lef o he magnaon an experence of he esgner.the am of hs paper s he esgn of a conrol law for a nonlnear excaon conroller o enhance he ransen sably an o ensure goo pos-faul olage regulaon for synchronous generaor connece o an nfne bus hrough a ransmsson lne, as shown n Fg. 1. The moel of he synchronous machne use s a 7 h orer moel, 5 for he elecrcal ynamcs an 2 for he mechancal ynamcs, whch akes no accoun he saor ynamcs as well as he amper wnng effecs an praccal lmaon on conrol. The feeback sysem s globally asympocally sable n he sense of he Lyapuno sably heory. The res of hs paper s organze as follows. In secon 2, we escrbe he sngle-machne-nfne-bus power sysem moel n a sae space form suable for

2 Proc. of he 5h WSEAS/IASME In. Conf. on Elecrc Power Sysems, Hgh Volages, Elecrc Machnes, Tenerfe, Span, December 16-18, 2005 (pp98-103) Lyapuno-base conrol esgn. In secon 3, he nonlnear excaon conroller s ere. The sably of hs conroller s proen. Some llusrae smulaon resuls are presene an compare o he performance of a sanar regulaor olage AVR an PSS n secon 4 o alae he propose conroller an some conclung remarks are menone n he fnal secon. 2 Mahemacal moel of power sysem The generaor o be conrolle, sue n hs work, s shown n Fg. 1. I consss of synchronous generaor connece o an nfne bus a a ransmsson lne (SMIB). The synchronous machne equaons n erms of Park s -q axs are expresse as follows [17], [18]: Armaure wnngs where Fel wnng Damper wnngs Rs ωλq λ = + (1) q Rsq ωλ λq = + + (2) λ = L + L ( + ) (3) m k λ q = L q q + Lmq kq (4) = R L + L + L (5) s m m k 0 = Rkk Lm + Lm + Lk k 0 = Rkqkq Lmq + Lkq kq (6) (7) where, q are rec an quaraure axs saor ermnal olage componens, respecely; s he excaon conrol npu;, q rec an quaraure axs saor curren componens, respecely; he fel wnng curren; k, kq rec an quaraure axs amper wnng curren componens, respecely; λ,λ q rec an quaraure axs flux lnkages, respecely; R s he saor ressance; R he fel ressance; R k, R kq he amper wnng ressances; L, L q he rec an quaraure self nucances, respecely; L he roor self nucance; L k, L kq rec an quaraure amper wnng self nucances, respecely an L m, L mq rec an quaraure magnezng nucances, respecely. Mechancal equaon δ = ω 1 2 ω m e H = T T Dω (8) (9) where ω s he angular spee of he generaor; δ he roor angle of he generaor; T m he mechancal orque; T e he elecromagnec orque; D he ampng consan an H he nera consan. Generaor G Lne (R e, L e) Fg. 1. Sngle machne nfne bus. Infne Bus The equaon for ransmsson nework wh exernal ressance Re an nucance Le, n he Park ransforme coornaes are = R + L ωl + V cos( δ a) e e e q = R + L + ωl V sn( δ a) q e q e q e I.B (10) (11) where V s he nfne bus olage an a s s phase angle. By combnng equaons (1) o (11), he resulan generaor sysem moel, n per un, has he followng form = a + a + a ω + a + a ω q 14 k 15 kq + a cos( ) + b 16 1 = a + a + a ω + a + a ω q 24 k 25 kq + a cos( ) + b 26 2 (12) (13) q = a31ω+ a32ω+ a33q + a34kω+ a35kq (14) + a sn( ) 36 = a + a + a ω + a + a ω k q 44 k 45 kq + a cos( ) + b 46 3 = a ω+ a ω+ a + a ω+ a kq q 54 k 55 kq + a sn( ) 56 ω = a + a + a + a 61 q 62 q 63 q k 64 kq + a ω + a T m (15) (16) (17) δ = ω ( 1 R ω ) (18) where ω R s he elecrcal frequency; a j an b are consans whch epen on he generaor an on he loa parameers [3]. 3 Desgn of a nonlnear excaon conroller Lyapuno s secon or rec meho s a ery powerful ool of assessng sably of a nonlnear sysem [16], [19]. In hs paper, he concep of Lyapuno s sably creron s use o selec he conrol sraegy of he Sngle Machne Infne Bus (SMIB), n orer o ensure

3 Proc. of he 5h WSEAS/IASME In. Conf. on Elecrc Power Sysems, Hgh Volages, Elecrc Machnes, Tenerfe, Span, December 16-18, 2005 (pp98-103) goo seay an ransen sably. To reach hs objece, we efne he ermnal olage error as e= (19) where = 1 s he esre rajecory an V ref Nonlnear Conroller P m Synchronous Generaor V = + q (20) 2 2 Sysem sae arables The expressons of an as a funcon of he sae arables can be expresse as follow = c + c + c ω + c + c ω q 14 k 15 kq + c cos( ) + c q (21) q = c21ω + c22ω+ c23q + c24kω+ c25kq c sn( ) (22) + 26 where c j are consans whch epen on he consans a j an on he loa parameers [3]. A pose efne Lyapuno funcon of he SMIB can be consere as 1 2 V = e (23) 2 The me erae of he V() ecan be wren as V = ee (24) From he erae of he ermnal olage error an by usng (12)-(16) an (20)-(22), we obans he followng expresson 1 e= = + qq (25) q = c17 + bc g1 + c14 g2 + q where g1 = c11+ c12+ c13 ωq+ qω (26) + c sn( ) 15 ωkq + kq ω + c16 an g2 = a41 + a42 + a43qω + a44k + a45k qω a cos( ) (27) + 46 Then he erae of he Lyapuno funcon s compue as V = c e+ bc e+ g e q gc 2 14 e q e (28) Thus, he Lyapuno s sably creron can be sasfe by makng erm on he rgh han se of (28) negae sem efne n orer o guaranee he global asympoc sably of he sysem. The canaes of ha Fg. 2 Bloc agram of he propose nonlnear scheme guaranees he sem negae efneness creron of equaon (28) can be consere as Ke + b3c14 + g1 = c 17 q (29) + c14 g2 + q where K s a pose consan feeback gan. Subsung (29) no (28) he erae of he Lyapuno funcon becomes 2 V = Ke (30) Defne he followng equaon 2 W () = Ke 0 (31) Furhermore, by usng LaSalle Yoshzawa s heorem [16], s can be shown ha W() en o zero as. Therefore, e wll conerge o zero as. 4 Smulaon resuls an scusson In orer o alae he mahemacal analyss an, hence, o esablsh he effeceness of he propose nonlnear conrol scheme, Smulaons works are carre ou for he Sngle Machne Infne Bus Sysem. The sysem confguraon s presene as shown n Fg.2.The performance of he nonlnear conroller was ese on he complee 7 h orer moel of he generaor sysem wh he physcal lm of he excaon olage of he generaor. The parameer alues use n he ensung smulaon are gen n he appenx. The faul consere n hs paper s a symmercal hree-phase shor crcu. The faul locaon s nexe by a consan λ whch s he fracon of he lne o he rgh of he faul. If λ = 1 he faul s a he nfne bus bar. The smulae resuls are gen n Fg. 3. I s shown ermnal olage, roor spee, roor angle an excaon olage, respecely. The operang pon consere s P mo = 0.6 p.u. The faul occurs closer o he nfne bus bar a = 5s an remoe by openng he barkers of he faule lne a = 5.1s. As can be seen he pos faul ermnal olage s regulae o s prefaul alue ery quckly. I s que een ha he propose

4 Proc. of he 5h WSEAS/IASME In. Conf. on Elecrc Power Sysems, Hgh Volages, Elecrc Machnes, Tenerfe, Span, December 16-18, 2005 (pp98-103) Termnal olage (p.u.) Roor spee (p.u.) Tme (s) Tme (s) Excaon olage (p.u.) Roor angle (egree) Tme (s) Tme (s) Fg. 3 Smulae resul of he propose nonlnear excaon conroller. conroller achees goo ransen sably, an ampens ou he power angle oscllaons. In orer o proe he robusness of he propose conroller, he resuls are compare wh hose of he lnear conrollers (conenonal IEEE ype 1 AVR an PSS). Fg. 4 an Fg. 5 show he responses of he ermnal olage uner P mo = 0.9 p.u, λ = 0.01 an P mo = 0.3 p.u, λ = 1, respecely. I s seen how ynamcs of he ermnal olage exhb large oershoos urng pos faul sae before he sele o s seay sae alue wh he sanar lnear scheme han wh he nonlnear conroller. The propose conroller can quckly an accuraely rack he esre ermnal olage espe he fferen faul locaons an operang pons. Anoher smulae ermnal olage responses for a suen ncrease n he mechancal power s shown n Fg.6. The power sysem s sare a mechancal power of P mo = 0.3 p.u. Aroun = 6s, he mechancal power s se a P mo = 0.75 p.u. I s shown ha he ermnal olage of he lnear conroller shows remarkable ransen before o seles o esre alue, whle he ermnal olage of he propose conroller s unaffece by hs araon. From he resuls presene earler, agan he superory of he nonlnear conroller s obsere. 5 Concluson Ths paper has successfully emonsrae he esgn, an sably analyss of Lyapuno echnque approach for he ransen sably an olage regulaon of a SMIB power sysem base on he complee 7 h orer moel of he generaor sysem. Frs, he ynamc moel of a SMIB was nrouce. Then, a nonlnear conrol sysem was esgne n he sense of Lyapuno conrol echnque. The feeback sysem s globally asympocally sable. The esgn of he conroller s nepenen of he operang pon. Smulaon resuls emonsrae ha wh he propose conroller, he generaor excaon conroller can effecely mproe he olage sably amp oscllaon an enhance he ransen sably of power sysem uner a large suen faul. Wh he ere conrol hgh an accuracy sably can be achee compare o he conenonal AVR an PSS conrollers.

5 Proc. of he 5h WSEAS/IASME In. Conf. on Elecrc Power Sysems, Hgh Volages, Elecrc Machnes, Tenerfe, Span, December 16-18, 2005 (pp98-103) Termnal olage (p.u.) Tme (s) Fg. 4 Responses of he ermnal olage uner P mo = 0.9 p.u an λ = 0.01; (sol) propose conroller; (o) lnear conrollers. Termnal olage (p.u.) Tme (s) Fg. 5 Responses of he ermnal olage uner P mo = 0.3 p.u an λ = 1; (sol) propose conroller; (o) lnear conrollers. Termnal olage (p.u.) Tme (s) Fg. 6 Responses of he ermnal olage for a suen ncrease n mechancal power, P mo =0.45 a = 6 s; (sol) propose conroller; (o) lnear conrollers.

6 Proc. of he 5h WSEAS/IASME In. Conf. on Elecrc Power Sysems, Hgh Volages, Elecrc Machnes, Tenerfe, Span, December 16-18, 2005 (pp98-103) Appenx Table 1 Parameers of he Transmsson Lne n p.u. Parameer L e, nucance of he ransmsson lne. R e, ressance of he ransmsson lne. Value Table 2 Parameers of he Power Synchronous Generaor n p.u. Parameer R s, saor ressance. R, fel ressance. R k, rec amper wnng ressance. R kq, quaraure amper wnng ressance. L, rec self-nucance. L q quaraure self-nucances. L, roor self nucance. L k, rec amper wnng self nucance. L kq, quaraure amper wnng self nucance. L m, rec magnezng nucance. L mq, quaraure magnezng nucance. V, nfne bus olage D, ampng consan. H, nera consan. Value s References: [1] M.S. Ghazzaeh, F. M. Hughs, A Generaor Transfer Funcon Regulaor for Improe Excaon Conrol, IEEE Trans on. Power Sysems, Vol. 13, N 2, 1998, pp [2] Al. A Ghanakly, A. M. Farhou, A Paramercally Opmze Self Tunng Regulaor for Power Sysem Ssablzers, IEEE Trans on. Power Sysems, Vol. 7, N 3, 1992, pp [3] O. Akhrf, F. A. Okou, L. A. Dessan, R. Champagne, Applcaon of Mularable Feeback Lnearzaon Scheme for Roor Angle Sably an Volage Regulaon of Power Sysems, IEEE Trans on. Power Sysems, Vol. 14, N 2, 1999, pp [4] Q. Zhao, J.Jang, Robus Conroller Desgn for Generaor Excaon Sysems, IEEE Trans on. Energy Conerson, Vol. 10, N 2, 1995, pp [5] Z. X, G. Feng, D. Cheng, an Q. Lu, Nonlnear ecenralze saurae conroller esgn for power sysems, IEEE Trans. on Conrol Sysems Technology, Vol. 11, N 4, 2003, pp [6] Y. Wang, G. Guo, an D. J. Hll, Robus ecenralze nonlnear conroller esgn for mulmachne power sysems, Auomaca, Vol. 33, N 9, 1997, pp [7] W. Ln, T. Shen, Robus passy an feeback esgn for mnmum-phase nonlnear sysems wh srucural uncerany. Auomaca, ol. 35, 1999, pp [8] J. Chapman, M. Ilc, C. Kng, L. Eng, an H. Kaufman, Sablzng a mulmachne power sysem a ecenralze feeback lnearzng excaon conrol, IEEE Trans. on Power Sysems, ol. 8, 1993, pp [9] L. Gao, L. Chen, Y. Fan an H. Ma, A nonlnear conrol esgn for power sysems, Auomaca, Vol. 28, N 5, 1992, pp [10] C. A. Kng, J. W. Chapman, an M. D. Ilc, Feeback lnearzng excaon conrol on a fullscale power sysem moel. IEEE Transacons on Power Sysems, Vol. 2, 1994, pp [11] S. Jan, F. Khorram an B. Faranesh, Aape nonlnear excaon conrol of power sysem wh unknown nerconnecons, IEEE Transacons on Conrol Sysems Technology, Vol. 2, 1994, pp [12] Y. Tan an Y. Wang, Augmenaon of ransen sably usng a supperconucon col an aape nonlnear conrol, IEEE Trans. On Power Sysems, ol. 13, N 2, 1998, pp [13] Y. Wang, D. J. Hll, R. H. Mleon, an L. Gao, Transen sablzaon of power sysems wh an aape conrol law, Auomaca, Vol. 30, 1994, pp [14]T. Shen, S. Me, Q. Lu, W. Hu, an K. Tamura, Aape nonlnear excaon conrol wh L2 surbance aenuaon for power sysems, Auomaca, Vol. 39, N 1, 2003, pp [15]Y. Wang, G. Guo, an D. Hll, Robus ecenralze nonlnear conroller esgn for mulmachne power sysems, Auomaca, Vol. 33, N 9, 1997, pp [16] M. Krsc, I. Kanellakopoulos, an P.V. Kokooc, Nonlnear an Aape Conrol Desgn. New York: Wley Inerscence, [17] P. M. Anerson, A. A. Foua, Power sysem conrol an sably, IEEE Perss, [18] C. H. Cheng, Y. Y. Hsu, Dampng of Generaor Oscllaon Usng an Aape Sac Var Compensaeur, IEEE Trans on. Power Sysems, Vol. 7, N 2, 1992, pp [19] M. Vysagar, Nonlnear sysem Analyss, SIAM, Phlaelpha 2002.

Lesson 2 Transmission Lines Fundamentals

Lesson 2 Transmission Lines Fundamentals Lesson Transmsson Lnes Funamenals 楊尚達 Shang-Da Yang Insue of Phooncs Technologes Deparmen of Elecrcal Engneerng Naonal Tsng Hua Unersy Tawan Sec. -1 Inroucon 1. Why o scuss TX lnes srbue crcus?. Crera

More information

2/20/2013. EE 101 Midterm 2 Review

2/20/2013. EE 101 Midterm 2 Review //3 EE Mderm eew //3 Volage-mplfer Model The npu ressance s he equalen ressance see when lookng no he npu ermnals of he amplfer. o s he oupu ressance. I causes he oupu olage o decrease as he load ressance

More information

Sensorless Speed Control of Salient Pole PMSM According to the Backstepping Observer

Sensorless Speed Control of Salient Pole PMSM According to the Backstepping Observer Proceengs of he Inernaonal Conference on Recen Avances n Elecrcal Sysems, Tunsa, 26 Sensorless Spee Conrol of Salen Pole PMSM Accorng o he Backseppng Observer S. Naj S. Benacha Elecrcal Engneerng Deparmen

More information

Chapter 6: AC Circuits

Chapter 6: AC Circuits Chaper 6: AC Crcus Chaper 6: Oulne Phasors and he AC Seady Sae AC Crcus A sable, lnear crcu operang n he seady sae wh snusodal excaon (.e., snusodal seady sae. Complee response forced response naural response.

More information

Revision: June 12, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: June 12, E Main Suite D Pullman, WA (509) Voice and Fax .: apacors Reson: June, 5 E Man Sue D Pullman, WA 9963 59 334 636 Voce an Fax Oerew We begn our suy of energy sorage elemens wh a scusson of capacors. apacors, lke ressors, are passe wo-ermnal crcu elemens.

More information

Decentralised Sliding Mode Load Frequency Control for an Interconnected Power System with Uncertainties and Nonlinearities

Decentralised Sliding Mode Load Frequency Control for an Interconnected Power System with Uncertainties and Nonlinearities Inernaonal Research Journal of Engneerng and echnology IRJE e-iss: 2395-0056 Volume: 03 Issue: 12 Dec -2016 www.re.ne p-iss: 2395-0072 Decenralsed Sldng Mode Load Frequency Conrol for an Inerconneced Power

More information

First-order piecewise-linear dynamic circuits

First-order piecewise-linear dynamic circuits Frs-order pecewse-lnear dynamc crcus. Fndng he soluon We wll sudy rs-order dynamc crcus composed o a nonlnear resse one-por, ermnaed eher by a lnear capacor or a lnear nducor (see Fg.. Nonlnear resse one-por

More information

AMPLITUDE CONTROL OF A SELF-VIBRATION MACHINE

AMPLITUDE CONTROL OF A SELF-VIBRATION MACHINE ENOC 28, San Peersburg, Russa, June, 3 July, 4 28 AMPLITUDE CONTROL OF A SELF-VIBRATION MACHINE Yuusuke Uchyama Grauae School of Sysems an Informaon Engneerng Unversy of Tsukuba Japan uchyama@aosuna.esys.sukuba.ac.jp

More information

Delay-Range-Dependent Stability Analysis for Continuous Linear System with Interval Delay

Delay-Range-Dependent Stability Analysis for Continuous Linear System with Interval Delay Inernaonal Journal of Emergng Engneerng esearch an echnology Volume 3, Issue 8, Augus 05, PP 70-76 ISSN 349-4395 (Prn) & ISSN 349-4409 (Onlne) Delay-ange-Depenen Sably Analyss for Connuous Lnear Sysem

More information

Energy Storage Devices

Energy Storage Devices Energy Sorage Deces Objece of Lecure Descrbe he consrucon of a capacor and how charge s sored. Inroduce seeral ypes of capacors Dscuss he elecrcal properes of a capacor The relaonshp beween charge, olage,

More information

Coupling series two five-phase asynchronous machine powered by a single voltage inverter

Coupling series two five-phase asynchronous machine powered by a single voltage inverter Leonaro Journal of Scences SS 83-33 ssue 7, July-December p 9- Couplng seres wo fve-phase asynchronous machne powere by a sngle volage nverer Samr ABBAR *, Karm FELLAH, Foua BEKHORS Elecrcal Engneerng

More information

An Adaptive Fuzzy Control Method for Spacecrafts Based on T-S Model

An Adaptive Fuzzy Control Method for Spacecrafts Based on T-S Model ELKOMNIKA, Vol., No., Noveber 20, pp. 6879~6888 e-issn: 2087-278X 6879 An Aapve Fuzzy Conrol Meho for Spacecrafs Base on -S Moel Wang Q*, Gao an 2, He He School of Elecronc Inforaon Engneerng, X an echnologcal

More information

Existence and Uniqueness Results for Random Impulsive Integro-Differential Equation

Existence and Uniqueness Results for Random Impulsive Integro-Differential Equation Global Journal of Pure and Appled Mahemacs. ISSN 973-768 Volume 4, Number 6 (8), pp. 89-87 Research Inda Publcaons hp://www.rpublcaon.com Exsence and Unqueness Resuls for Random Impulsve Inegro-Dfferenal

More information

On One Analytic Method of. Constructing Program Controls

On One Analytic Method of. Constructing Program Controls Appled Mahemacal Scences, Vol. 9, 05, no. 8, 409-407 HIKARI Ld, www.m-hkar.com hp://dx.do.org/0.988/ams.05.54349 On One Analyc Mehod of Consrucng Program Conrols A. N. Kvko, S. V. Chsyakov and Yu. E. Balyna

More information

Chapters 2 Kinematics. Position, Distance, Displacement

Chapters 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 information

( ) () we define the interaction representation by the unitary transformation () = ()

( ) () 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 information

Solution in semi infinite diffusion couples (error function analysis)

Solution 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

10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current :

10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current : . A. IUITS Synopss : GOWTH OF UNT IN IUIT : d. When swch S s closed a =; = d. A me, curren = e 3. The consan / has dmensons of me and s called he nducve me consan ( τ ) of he crcu. 4. = τ; =.63, n one

More information

Decentralized Control for Time-Delay Interconnected Systems Based on T-S Fuzzy Bilinear Model

Decentralized Control for Time-Delay Interconnected Systems Based on T-S Fuzzy Bilinear Model ensors & ransucers Vol. 75 Issue 7 July 24 pp. 32-37 ensors & ransucers 24 by IFA Publshng. L. hp://www.sensorsporal.com Decenralze Conrol for me-delay Inerconnece ysems Base on - Fuzzy Blnear Moel * Guo

More information

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy Arcle Inernaonal Journal of Modern Mahemacal Scences, 4, (): - Inernaonal Journal of Modern Mahemacal Scences Journal homepage: www.modernscenfcpress.com/journals/jmms.aspx ISSN: 66-86X Florda, USA Approxmae

More information

Using Gravitational Search Algorithm to Design of an Optimal Active Power Controller for AC-DC Transmission Systems

Using Gravitational Search Algorithm to Design of an Optimal Active Power Controller for AC-DC Transmission Systems Inernaonal Research Journal of Engneerng an Technology (IRJET) e-issn: 2395-0056 Volume: 02 Issue: 02 ay-2015 www.re.ne p-issn: 2395-0072 Usng Gravaonal Search Algorhm o Desgn of an Opmal Acve Power Conroller

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

[ ] 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 information

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS R&RATA # Vol.) 8, March FURTHER AALYSIS OF COFIDECE ITERVALS FOR LARGE CLIET/SERVER COMPUTER ETWORKS Vyacheslav Abramov School of Mahemacal Scences, Monash Unversy, Buldng 8, Level 4, Clayon Campus, Wellngon

More information

Current Distribution Analysis for High Temperature Superconducting Cable Considering Hysteresis Characteristics

Current Distribution Analysis for High Temperature Superconducting Cable Considering Hysteresis Characteristics Curren Dsrbuon Analyss for Hgh Temperaure uperconucng Cable Conserng Hyseress Characerscs huhong WANG a, Je QIU a, Xnyng LIU a, Zhxuan WANG a, Janguo ZHU b, Youguang GUO b, Zh We LIN b, Y WANG b an We

More information

Relative controllability of nonlinear systems with delays in control

Relative controllability of nonlinear systems with delays in control Relave conrollably o nonlnear sysems wh delays n conrol Jerzy Klamka Insue o Conrol Engneerng, Slesan Techncal Unversy, 44- Glwce, Poland. phone/ax : 48 32 37227, {jklamka}@a.polsl.glwce.pl Keywor: Conrollably.

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Lnear Response Theory: The connecon beween QFT and expermens 3.1. Basc conceps and deas Q: ow do we measure he conducvy of a meal? A: we frs nroduce a weak elecrc feld E, and hen measure

More information

Sliding mode control without reaching phase for multimachine power system combined with fuzzy PID based on PSS

Sliding mode control without reaching phase for multimachine power system combined with fuzzy PID based on PSS WSEAS RANSACIONS on SYSEMS and CONROL Faza Db, haddou Ben Mezane, Ismal Boumhd Sldng mode conrol whou reachng phase for mulmachne power sysem combned wh fuzzy PID based on PSS FAIZA DIB, HADDOUJ BEN MEZIANE,

More information

Comb Filters. Comb Filters

Comb Filters. Comb Filters The smple flers dscussed so far are characered eher by a sngle passband and/or a sngle sopband There are applcaons where flers wh mulple passbands and sopbands are requred Thecomb fler s an example of

More information

Notes on the stability of dynamic systems and the use of Eigen Values.

Notes on the stability of dynamic systems and the use of Eigen Values. Noes on he sabl of dnamc ssems and he use of Egen Values. Source: Macro II course noes, Dr. Davd Bessler s Tme Seres course noes, zarads (999) Ineremporal Macroeconomcs chaper 4 & Techncal ppend, and Hamlon

More information

HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD

HEAT 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 information

A capacitor consists of two conducting plates, separated by an insulator. Conduction plates: e.g., Aluminum foil Insulator: air, mica, ceramic, etc

A capacitor consists of two conducting plates, separated by an insulator. Conduction plates: e.g., Aluminum foil Insulator: air, mica, ceramic, etc 3//7 haper 6 apacors and Inducors Makng preparaon for dynamc crcus, whch hae far more applcaons han he sac crcus we hae learned so far. 6. apacors Sore energy n elecrc feld nsulaor onducng plaes A capacor

More information

Robustness Experiments with Two Variance Components

Robustness Experiments with Two Variance Components Naonal Insue of Sandards and Technology (NIST) Informaon Technology Laboraory (ITL) Sascal Engneerng Dvson (SED) Robusness Expermens wh Two Varance Componens by Ana Ivelsse Avlés avles@ns.gov Conference

More information

GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim

GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim Korean J. Mah. 19 (2011), No. 3, pp. 263 272 GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS Youngwoo Ahn and Kae Km Absrac. In he paper [1], an explc correspondence beween ceran

More information

Hopf Bifurcation and Sliding Mode Control of Chaotic Vibrations in a Four-dimensional Hyperchaotic System

Hopf Bifurcation and Sliding Mode Control of Chaotic Vibrations in a Four-dimensional Hyperchaotic System Hopf Bfurcaon an Slng Moe Conrol of Chaoc Vbraons n a Four-mensonal Hyperchaoc Sysem Wen-ju Du, Jan-gang Zhang an Shuang Qn Absrac he basc ynamc properes of a four mensonal hyperchaoc sysem are nvesgae

More information

CHAPTER II AC POWER CALCULATIONS

CHAPTER II AC POWER CALCULATIONS CHAE AC OWE CACUAON Conens nroducon nsananeous and Aerage ower Effece or M alue Apparen ower Coplex ower Conseraon of AC ower ower Facor and ower Facor Correcon Maxu Aerage ower ransfer Applcaons 3 nroducon

More information

Comparitive Analysis of P-I, I-P, PID and Fuzzy Controllers for Speed Control of DC Motor

Comparitive Analysis of P-I, I-P, PID and Fuzzy Controllers for Speed Control of DC Motor Comarve Analyss of P-, -P, PD an Fuzzy Conrollers for ee Conrol of DC Moor M Venkaa Ganesh Bau 1, Dr. R.rnu Nak 2 1PG uen, De of EEE, Anhra Unversy[A], Vsakhaanam, na 2Asssan Professor, De of EEE, Anhra

More information

Cubic Bezier Homotopy Function for Solving Exponential Equations

Cubic 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 information

Lecture 18: The Laplace Transform (See Sections and 14.7 in Boas)

Lecture 18: The Laplace Transform (See Sections and 14.7 in Boas) Lecure 8: The Lalace Transform (See Secons 88- and 47 n Boas) Recall ha our bg-cure goal s he analyss of he dfferenal equaon, ax bx cx F, where we emloy varous exansons for he drvng funcon F deendng on

More information

On computing differential transform of nonlinear non-autonomous functions and its applications

On computing differential transform of nonlinear non-autonomous functions and its applications On compung dfferenal ransform of nonlnear non-auonomous funcons and s applcaons Essam. R. El-Zahar, and Abdelhalm Ebad Deparmen of Mahemacs, Faculy of Scences and Humanes, Prnce Saam Bn Abdulazz Unversy,

More information

Implementation of Quantized State Systems in MATLAB/Simulink

Implementation of Quantized State Systems in MATLAB/Simulink SNE T ECHNICAL N OTE Implemenaon of Quanzed Sae Sysems n MATLAB/Smulnk Parck Grabher, Mahas Rößler 2*, Bernhard Henzl 3 Ins. of Analyss and Scenfc Compung, Venna Unversy of Technology, Wedner Haupsraße

More information

P R = P 0. The system is shown on the next figure:

P R = P 0. The system is shown on the next figure: TPG460 Reservor Smulaon 08 page of INTRODUCTION TO RESERVOIR SIMULATION Analycal and numercal soluons of smple one-dmensonal, one-phase flow equaons As an nroducon o reservor smulaon, we wll revew he smples

More information

EG Low Voltage CMOS Fully Differential Current Feedback Amplifier with Controllable 3-dB Bandwidth

EG Low Voltage CMOS Fully Differential Current Feedback Amplifier with Controllable 3-dB Bandwidth EG0800330 Low olage CMS Fully Derenal Curren Feedback Ampler wh Conrollable 3dB Bandwdh Ahmed H. Madan 2, Mahmoud A. Ashour, Solman A. Mahmoud 2, and Ahmed M. Solman 3 adaon Engneerng Dep., NCT, EAEA Caro,

More information

FAIPA_SAND: An Interior Point Algorithm for Simultaneous ANalysis and Design Optimization

FAIPA_SAND: An Interior Point Algorithm for Simultaneous ANalysis and Design Optimization FAIPA_AN: An Ineror Pon Algorhm for mlaneos ANalyss an esgn Opmzaon osé Hersos*, Palo Mappa* an onel llen** *COPPE / Feeral Unersy of Ro e anero, Mechancal Engneerng Program, Caa Posal 6853, 945 97 Ro

More information

2. Electric Circuit Theory

2. Electric Circuit Theory . Elecrc rcu Theory J Deparmen of Elecrcal, Elecronc, and Informaon Engneerng (DEI) - Unersy of ologna Elecrc crcu heory and Elecromagnec heory are he wo fundamenal heores upon whch all branches of elecrcal

More information

ISSN MIT Publications

ISSN MIT Publications MIT Inernaonal Journal of Elecrcal and Insrumenaon Engneerng Vol. 1, No. 2, Aug 2011, pp 93-98 93 ISSN 2230-7656 MIT Publcaons A New Approach for Solvng Economc Load Dspach Problem Ansh Ahmad Dep. of Elecrcal

More information

Chapter 5. Circuit Theorems

Chapter 5. Circuit Theorems Chaper 5 Crcu Theorems Source Transformaons eplace a olage source and seres ressor by a curren and parallel ressor Fgure 5.-1 (a) A nondeal olage source. (b) A nondeal curren source. (c) Crcu B-conneced

More information

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS

THE 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 information

Variants of Pegasos. December 11, 2009

Variants 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 information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 0 Canoncal Transformaons (Chaper 9) Wha We Dd Las Tme Hamlon s Prncple n he Hamlonan formalsm Dervaon was smple δi δ Addonal end-pon consrans pq H( q, p, ) d 0 δ q ( ) δq ( ) δ

More information

Track Properities of Normal Chain

Track Properities of Normal Chain In. J. Conemp. Mah. Scences, Vol. 8, 213, no. 4, 163-171 HIKARI Ld, www.m-har.com rac Propes of Normal Chan L Chen School of Mahemacs and Sascs, Zhengzhou Normal Unversy Zhengzhou Cy, Hennan Provnce, 4544,

More information

Let s treat the problem of the response of a system to an applied external force. Again,

Let s treat the problem of the response of a system to an applied external force. Again, Page 33 QUANTUM LNEAR RESPONSE FUNCTON Le s rea he problem of he response of a sysem o an appled exernal force. Agan, H() H f () A H + V () Exernal agen acng on nernal varable Hamlonan for equlbrum sysem

More information

SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β

SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β SARAJEVO JOURNAL OF MATHEMATICS Vol.3 (15) (2007), 137 143 SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β M. A. K. BAIG AND RAYEES AHMAD DAR Absrac. In hs paper, we propose

More information

Motion in Two Dimensions

Motion in Two Dimensions Phys 1 Chaper 4 Moon n Two Dmensons adzyubenko@csub.edu hp://www.csub.edu/~adzyubenko 005, 014 A. Dzyubenko 004 Brooks/Cole 1 Dsplacemen as a Vecor The poson of an objec s descrbed by s poson ecor, r The

More information

Delay Dependent Robust Stability of T-S Fuzzy. Systems with Additive Time Varying Delays

Delay Dependent Robust Stability of T-S Fuzzy. Systems with Additive Time Varying Delays Appled Maemacal Scences, Vol. 6,, no., - Delay Dependen Robus Sably of -S Fuzzy Sysems w Addve me Varyng Delays Idrss Sad LESSI. Deparmen of Pyscs, Faculy of Scences B.P. 796 Fès-Alas Sad_drss9@yaoo.fr

More information

WiH Wei He

WiH Wei He Sysem Idenfcaon of onlnear Sae-Space Space Baery odels WH We He wehe@calce.umd.edu Advsor: Dr. Chaochao Chen Deparmen of echancal Engneerng Unversy of aryland, College Par 1 Unversy of aryland Bacground

More information

TUTORIAL SOLUTIONS. F.1 KCL, KVL, Power and Energy Q.1. i All units in VAΩ,,

TUTORIAL SOLUTIONS. F.1 KCL, KVL, Power and Energy Q.1. i All units in VAΩ,, F TUTOIAL SOLUTIONS F. KCL, KVL, Power and Energy Q. 8 9 6 All uns n VAΩ,, Appendx F Tuoral Soluons Applyng KCL o he doed surface: + + Q. All uns n V, A, Ω Nework A Nework B Applyng KCL o he doed surface:

More information

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC CH.3. COMPATIBILITY EQUATIONS Connuum Mechancs Course (MMC) - ETSECCPB - UPC Overvew Compably Condons Compably Equaons of a Poenal Vecor Feld Compably Condons for Infnesmal Srans Inegraon of he Infnesmal

More information

Electrical and current self-induction

Electrical and current self-induction Elecrical and curren self-inducion F. F. Mende hp://fmnauka.narod.ru/works.hml mende_fedor@mail.ru Absrac The aricle considers he self-inducance of reacive elemens. Elecrical self-inducion To he laws of

More information

THERMODYNAMICS 1. The First Law and Other Basic Concepts (part 2)

THERMODYNAMICS 1. The First Law and Other Basic Concepts (part 2) Company LOGO THERMODYNAMICS The Frs Law and Oher Basc Conceps (par ) Deparmen of Chemcal Engneerng, Semarang Sae Unversy Dhon Harano S.T., M.T., M.Sc. Have you ever cooked? Equlbrum Equlbrum (con.) Equlbrum

More information

CS434a/541a: Pattern Recognition Prof. Olga Veksler. Lecture 4

CS434a/541a: Pattern Recognition Prof. Olga Veksler. Lecture 4 CS434a/54a: Paern Recognon Prof. Olga Veksler Lecure 4 Oulne Normal Random Varable Properes Dscrmnan funcons Why Normal Random Varables? Analycally racable Works well when observaon comes form a corruped

More information

R th is the Thevenin equivalent at the capacitor terminals.

R th is the Thevenin equivalent at the capacitor terminals. Chaper 7, Slun. Applyng KV Fg. 7.. d 0 C - Takng he derae f each erm, d 0 C d d d r C Inegrang, () ln I 0 - () I 0 e - C C () () r - I 0 e - () V 0 e C C Chaper 7, Slun. h C where h s he Theenn equalen

More information

Graduate Macroeconomics 2 Problem set 5. - Solutions

Graduate 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 information

FTCS Solution to the Heat Equation

FTCS Solution to the Heat Equation FTCS Soluon o he Hea Equaon ME 448/548 Noes Gerald Reckenwald Porland Sae Unversy Deparmen of Mechancal Engneerng gerry@pdxedu ME 448/548: FTCS Soluon o he Hea Equaon Overvew Use he forward fne d erence

More information

Multi-Objective Control and Clustering Synchronization in Chaotic Connected Complex Networks*

Multi-Objective Control and Clustering Synchronization in Chaotic Connected Complex Networks* Mul-Objecve Conrol and Cluserng Synchronzaon n Chaoc Conneced Complex eworks* JI-QIG FAG, Xn-Bao Lu :Deparmen of uclear Technology Applcaon Insue of Aomc Energy 043, Chna Fjq96@6.com : Deparmen of Auomaon,

More information

Multivariable Dynamic Model and Robust Control of a Voltage-Source Converter for Power System Applications

Multivariable Dynamic Model and Robust Control of a Voltage-Source Converter for Power System Applications Mularable Dynamc Moel an Robu Conrol of a Volage-Source Conerer for Power Syem Applcaon Ahmareza Tabeh an Reza Iraan Affne Conroller Parameerzaon for Decenralze Conrol Oer Banach Space Mchael Rokowz an

More information

ELEC 201 Electric Circuit Analysis I Lecture 9(a) RLC Circuits: Introduction

ELEC 201 Electric Circuit Analysis I Lecture 9(a) RLC Circuits: Introduction //6 All le courey of Dr. Gregory J. Mazzaro EE Elecrc rcu Analy I ecure 9(a) rcu: Inroucon THE ITADE, THE MIITAY OEGE OF SOUTH AOINA 7 Moulre Sree, harleon, S 949 V Sere rcu: Analog Dcoery _ 5 Ω pf eq

More information

Handout # 6 (MEEN 617) Numerical Integration to Find Time Response of SDOF mechanical system Y X (2) and write EOM (1) as two first-order Eqs.

Handout # 6 (MEEN 617) Numerical Integration to Find Time Response of SDOF mechanical system Y X (2) and write EOM (1) as two first-order Eqs. Handou # 6 (MEEN 67) Numercal Inegraon o Fnd Tme Response of SDOF mechancal sysem Sae Space Mehod The EOM for a lnear sysem s M X DX K X F() () X X X X V wh nal condons, a 0 0 ; 0 Defne he followng varables,

More information

Research Article Adaptive Synchronization of Complex Dynamical Networks with State Predictor

Research Article Adaptive Synchronization of Complex Dynamical Networks with State Predictor Appled Mahemacs Volume 3, Arcle ID 39437, 8 pages hp://dxdoorg/55/3/39437 Research Arcle Adapve Synchronzaon of Complex Dynamcal eworks wh Sae Predcor Yunao Sh, Bo Lu, and Xao Han Key Laboraory of Beng

More information

An introduction to Support Vector Machine

An introduction to Support Vector Machine An nroducon o Suppor Vecor Machne 報告者 : 黃立德 References: Smon Haykn, "Neural Neworks: a comprehensve foundaon, second edon, 999, Chaper 2,6 Nello Chrsann, John Shawe-Tayer, An Inroducon o Suppor Vecor Machnes,

More information

Stability Enhancement using Hybrid Power System Stabilizer Auto Tuned by Breeder Genetic Algorithm

Stability Enhancement using Hybrid Power System Stabilizer Auto Tuned by Breeder Genetic Algorithm Inernaonal Journal of lecrcal ngneerng. ISSN 974-2158 olume 4, Number 2 211, pp.29-226 Inernaonal Research Publcaon House hp://www.rphouse.com Sably nhancemen usng Hybr Power Sysem Sablzer Auo Tune by

More information

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s

Ordinary 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 information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm H ( q, p, ) = q p L( q, q, ) H p = q H q = p H = L Equvalen o Lagrangan formalsm Smpler, bu

More information

Diode rectifier with capacitive DC link

Diode rectifier with capacitive DC link . Converers Dode recfer wh capacve DC lnk 4 e lne lne D D 3 C v v [] e e D D 4 4 5 5 Fgure.: A sngle-phase dode recfer wh a capacve DC lnk. [s] Fgure.: ne-o-neural volage and DC sde volage for a sngle-phase

More information

CHAPTER 5: MULTIVARIATE METHODS

CHAPTER 5: MULTIVARIATE METHODS CHAPER 5: MULIVARIAE MEHODS Mulvarae Daa 3 Mulple measuremens (sensors) npus/feaures/arbues: -varae N nsances/observaons/eamples Each row s an eample Each column represens a feaure X a b correspons o he

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm Hqp (,,) = qp Lqq (,,) H p = q H q = p H L = Equvalen o Lagrangan formalsm Smpler, bu wce as

More information

Transient Response in Electric Circuits

Transient Response in Electric Circuits Transen esponse n Elecrc rcus The elemen equaon for he branch of he fgure when he source s gven by a generc funcon of me, s v () r d r ds = r Mrs d d r (')d' () V The crcu s descrbed by he opology equaons

More information

FI 3103 Quantum Physics

FI 3103 Quantum Physics /9/4 FI 33 Quanum Physcs Aleander A. Iskandar Physcs of Magnesm and Phooncs Research Grou Insu Teknolog Bandung Basc Conces n Quanum Physcs Probably and Eecaon Value Hesenberg Uncerany Prncle Wave Funcon

More information

John Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany

John Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany Herarchcal Markov Normal Mxure models wh Applcaons o Fnancal Asse Reurns Appendx: Proofs of Theorems and Condonal Poseror Dsrbuons John Geweke a and Gann Amsano b a Deparmens of Economcs and Sascs, Unversy

More information

A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION

A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION S19 A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION by Xaojun YANG a,b, Yugu YANG a*, Carlo CATTANI c, and Mngzheng ZHU b a Sae Key Laboraory for Geomechancs and Deep Underground Engneerng, Chna Unversy

More information

Econ107 Applied Econometrics Topic 5: Specification: Choosing Independent Variables (Studenmund, Chapter 6)

Econ107 Applied Econometrics Topic 5: Specification: Choosing Independent Variables (Studenmund, Chapter 6) Econ7 Appled Economercs Topc 5: Specfcaon: Choosng Independen Varables (Sudenmund, Chaper 6 Specfcaon errors ha we wll deal wh: wrong ndependen varable; wrong funconal form. Ths lecure deals wh wrong ndependen

More information

Parameter Estimation of Three-Phase Induction Motor by Using Genetic Algorithm

Parameter Estimation of Three-Phase Induction Motor by Using Genetic Algorithm 360 Journal of Elecrcal Engneerng & Technology Vol. 4, o. 3, pp. 360~364, 009 Parameer Esmaon of Three-Phase Inducon Moor by Usng Genec Algorhm Seesa Jangj and Panhep Laohacha* Absrac Ths paper suggess

More information

Testing a new idea to solve the P = NP problem with mathematical induction

Testing a new idea to solve the P = NP problem with mathematical induction Tesng a new dea o solve he P = NP problem wh mahemacal nducon Bacground P and NP are wo classes (ses) of languages n Compuer Scence An open problem s wheher P = NP Ths paper ess a new dea o compare he

More information

Performance Analysis for a Network having Standby Redundant Unit with Waiting in Repair

Performance Analysis for a Network having Standby Redundant Unit with Waiting in Repair TECHNI Inernaonal Journal of Compung Scence Communcaon Technologes VOL.5 NO. July 22 (ISSN 974-3375 erformance nalyss for a Nework havng Sby edundan Un wh ang n epar Jendra Sngh 2 abns orwal 2 Deparmen

More information

DYNAMICS ANALYSIS OF LFR MODEL FOR A SINGLE-STAGE HIGH POWER FACTOR CORRECTION DIAGONAL HALF-BRIDGE FLYBACK AC/DC CONVERTER

DYNAMICS ANALYSIS OF LFR MODEL FOR A SINGLE-STAGE HIGH POWER FACTOR CORRECTION DIAGONAL HALF-BRIDGE FLYBACK AC/DC CONVERTER Journal of he Chnese Insue of Engneers, Vol. 3, No. 4, pp. 555-567 (9) 555 DYNMICS NLYSIS OF LF MODEL FO SINGLE-STGE HIGH POWE FCTO COECTION DIGONL HLF-IDGE FLYCK C/DC CONVETE Jong-Lck Ln*, Chen-Yang Chen,

More information

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems Swss Federal Insue of Page 1 The Fne Elemen Mehod for he Analyss of Non-Lnear and Dynamc Sysems Prof. Dr. Mchael Havbro Faber Dr. Nebojsa Mojslovc Swss Federal Insue of ETH Zurch, Swzerland Mehod of Fne

More information

Tight results for Next Fit and Worst Fit with resource augmentation

Tight results for Next Fit and Worst Fit with resource augmentation Tgh resuls for Nex F and Wors F wh resource augmenaon Joan Boyar Leah Epsen Asaf Levn Asrac I s well known ha he wo smple algorhms for he classc n packng prolem, NF and WF oh have an approxmaon rao of

More information

PHYS 1443 Section 001 Lecture #4

PHYS 1443 Section 001 Lecture #4 PHYS 1443 Secon 001 Lecure #4 Monda, June 5, 006 Moon n Two Dmensons Moon under consan acceleraon Projecle Moon Mamum ranges and heghs Reerence Frames and relae moon Newon s Laws o Moon Force Newon s Law

More information

Stochastic Repair and Replacement with a single repair channel

Stochastic Repair and Replacement with a single repair channel Sochasc Repar and Replacemen wh a sngle repar channel MOHAMMED A. HAJEEH Techno-Economcs Dvson Kuwa Insue for Scenfc Research P.O. Box 4885; Safa-309, KUWAIT mhajeeh@s.edu.w hp://www.sr.edu.w Absrac: Sysems

More information

Improved Coupled Tank Liquid Levels System Based on Swarm Adaptive Tuning of Hybrid Proportional-Integral Neural Network Controller

Improved Coupled Tank Liquid Levels System Based on Swarm Adaptive Tuning of Hybrid Proportional-Integral Neural Network Controller Amercan J. of Engneerng and Appled Scences (4): 669-675, 009 ISSN 94-700 009 Scence Publcaons Improved Coupled Tan Lqud Levels Sysem Based on Swarm Adapve Tunng of Hybrd Proporonal-Inegral Neural Newor

More information

Scattering at an Interface: Oblique Incidence

Scattering at an Interface: Oblique Incidence Course Insrucor Dr. Raymond C. Rumpf Offce: A 337 Phone: (915) 747 6958 E Mal: rcrumpf@uep.edu EE 4347 Appled Elecromagnecs Topc 3g Scaerng a an Inerface: Oblque Incdence Scaerng These Oblque noes may

More information

Displacement, Velocity, and Acceleration. (WHERE and WHEN?)

Displacement, Velocity, and Acceleration. (WHERE and WHEN?) Dsplacemen, Velocy, and Acceleraon (WHERE and WHEN?) Mah resources Append A n your book! Symbols and meanng Algebra Geomery (olumes, ec.) Trgonomery Append A Logarhms Remnder You wll do well n hs class

More information

Physics 3 (PHYF144) Chap 3: The Kinetic Theory of Gases - 1

Physics 3 (PHYF144) Chap 3: The Kinetic Theory of Gases - 1 Physcs (PYF44) ha : he nec heory of Gases -. Molecular Moel of an Ieal Gas he goal of he olecular oel of an eal gas s o unersan he acroscoc roeres (such as ressure an eeraure ) of gas n e of s croscoc

More information

Improvement of Transient Stability of VSC HVDC System with Particle Swarm Optimization Based PI Controller

Improvement of Transient Stability of VSC HVDC System with Particle Swarm Optimization Based PI Controller Improvemen of Transen Sably of SC HDC Sysem wh Parcle Swarm Opmzaon Based Conroller Improvemen of Transen Sably of SC HDC Sysem wh Parcle Swarm Opmzaon Based Conroller *N. Nayak, ** S.K Rou ray, *** P.K.

More information

Advanced time-series analysis (University of Lund, Economic History Department)

Advanced time-series analysis (University of Lund, Economic History Department) Advanced me-seres analss (Unvers of Lund, Economc Hsor Dearmen) 3 Jan-3 Februar and 6-3 March Lecure 4 Economerc echnues for saonar seres : Unvarae sochasc models wh Box- Jenns mehodolog, smle forecasng

More information

TRACKING CONTROL DESIGN FOR A CLASS OF AFFINE MIMO TAKAGI-SUGENO MODELS

TRACKING CONTROL DESIGN FOR A CLASS OF AFFINE MIMO TAKAGI-SUGENO MODELS TRACKING CONTROL DESIGN FOR A CLASS OF AFFINE MIMO TAKAGI-SUGENO MODELS Carlos Arño Deparmen of Sysems Engneerng and Desgn, Jaume I Unversy, Sos Bayna S/N, Caselló de la Plana, Span arno@esdujes Anono

More information

Response of MDOF systems

Response of MDOF systems Response of MDOF syses Degree of freedo DOF: he nu nuber of ndependen coordnaes requred o deerne copleely he posons of all pars of a syse a any nsan of e. wo DOF syses hree DOF syses he noral ode analyss

More information

EE 247B/ME 218: Introduction to MEMS Design Lecture 27m2: Gyros, Noise & MDS CTN 5/1/14. Copyright 2014 Regents of the University of California

EE 247B/ME 218: Introduction to MEMS Design Lecture 27m2: Gyros, Noise & MDS CTN 5/1/14. Copyright 2014 Regents of the University of California MEMSBase Fork Gyrosoe Ω r z Volage Deermnng Resoluon EE C45: Inrouon o MEMS Desgn LeM 15 C. Nguyen 11/18/08 17 () Curren (+) Curren Eleroe EE C45: Inrouon o MEMS Desgn LeM 15 C. Nguyen 11/18/08 18 [Zaman,

More information

Anisotropic Behaviors and Its Application on Sheet Metal Stamping Processes

Anisotropic Behaviors and Its Application on Sheet Metal Stamping Processes Ansoropc Behavors and Is Applcaon on Shee Meal Sampng Processes Welong Hu ETA-Engneerng Technology Assocaes, Inc. 33 E. Maple oad, Sue 00 Troy, MI 48083 USA 48-79-300 whu@ea.com Jeanne He ETA-Engneerng

More information

Power Electronics 7. Diode and Diode Circuits

Power Electronics 7. Diode and Diode Circuits Module 7 Dode and Dode Crcus. Inroducon 2. DC and swchng characerscs 3. Types of Power Dode 4. Dode Crcu 4.. Seres Conneced Dodes 4.2. Parallel Conneced Dodes 5. Dode behavor for dfferen loads 6. Freewheelng

More information

Department of Economics University of Toronto

Department of Economics University of Toronto Deparmen of Economcs Unversy of Torono ECO408F M.A. Economercs Lecure Noes on Heeroskedascy Heeroskedascy o Ths lecure nvolves lookng a modfcaons we need o make o deal wh he regresson model when some of

More information