ROTOR RESISTANCE IDENTIFICATION USING NEURAL NETWORKS FOR INDUCTION MOTOR DRIVES IN THE CASE OF INSENSITIVITY TO LOAD VARIATIONS *

Size: px
Start display at page:

Download "ROTOR RESISTANCE IDENTIFICATION USING NEURAL NETWORKS FOR INDUCTION MOTOR DRIVES IN THE CASE OF INSENSITIVITY TO LOAD VARIATIONS *"

Transcription

1 Ianian Jounal of Scinc & Tchnology, Tanaction B, Engining, Vol. 30, No. B2 Pintd in Th Ilamic Rpublic of Ian, 2006 Shiaz Univity ROTOR RESISTANCE IDENTIFICATION USING NEURA NETWORKS FOR INDUCTION MOTOR DRIVES IN THE CASE OF INSENSITIVITY TO OAD VARIATIONS M. EBRAHIMI, E. REZAEI, B. VASEGHI AND M. DANESH Dpt. of Elc. Eng., Ifahan Univity of Tchnology, Ifahan, I. R. of Ian Abtact Fo induction moto div contolld by th indict oto flux ointd contol (IRFOC), th oto itanc vaiation ult in an undiabl coupling btwn th flux and th toqu of th machin, and lo of dynamic pfomanc. Thi pap pnt a chm fo th timation of oto itanc uing a nual ntwok (NN) block. In thi ytm th flux and toqu hav bn timatd by uing tato voltag and cunt. A back-popagation NN civ th flux and toqu o and a uppod oto itanc at th input and timat th actual oto itanc at th output, which i ud in th contol of an indict vcto-contolld div ytm. Th nual ntwok ha bn taind off lin with th mathmatical modl of th contol chm in dtuning opation. IRFOC contol, ud with th NN timato, ha bn tudid in th dtuning condition. Th pfomanc of th contoll i good, vn whn th oto tim contant i incad fom nominal at to twic th nominal valu, a wll a toqu vaiation. In thi mthod, timation i don quickly and accuatly, and it dign i impl. Simulation ult fo a 3-hp induction moto divn by a cunt-gulatd pul width modulation CRPWM invt with an indict vcto contoll a pntd to validat th ffctivn of th popod tchniqu fo th pupo of impoving th pfomanc and obutn of th div. Kywod Nual ntwok, vcto contol, induction moto, oto itanc, fild ointd contol, flux timation, toqu timation 1. INTRODUCTION Vcto contol i bcoming a tandad tool fo indutial moto div. Two diffnt appoach a poibl in th aa of vcto contol: th dict vcto contol in which th oto flux poition and amplitud a timatd, and th indict vcto contol in which only th oto flux poition i ud [1, 2]. Th indict oto flux ointd contol mthod (IRFOC) off th mot intting chaactitic and i thu widly ud in high pfomanc div [3]. Th main fatu of th IRFOC a th implicity of it implmntation and th linaity of it tady tat toqu lip chaactitic. So, it contitut a judiciou and attactiv choic fo a gnalizd implmntation of high pfomanc adjutabl pd ac div uing induction moto. Th IRFOC i a fd-fowad contol mthod and i vy nitiv to th vaiation of moto paamt [4, 5]. Thi i du to th fact that all indict mthod of fild ointation a bad on th inv modl of th machin [3] with contant paamt. Indict vcto contol of an induction moto pnt good tacking fo flux and immdiat tacking fo toqu. With gad to th fact that a uccful implmntation of th fild-ointd contol qui Rcivd by th dito May 4, 2003; final vid fom Dcmb 18, Coponding autho

2 224 M. Ebahimi / t al. an accuat calculation of th lip fquncy, a mathmatical modl of th machin i ud. Th o in th modl paamt can cau incomplt dcoupling btwn flux and toqu; th ult i a mimatch btwn th toqu command and th moto toqu in th tady tat mod on th on hand, and an ocillatoy pon of th tanint toqu on th oth [4]. Dtuning of oto tim contant i th mot ffctiv in unuccful implmntation of an IRFOC chm [5], and unfotunatly it may vay widly with th opational paamt of th moto uch a tmpatu, fquncy and th atuation lvl of th machin. High pfomanc contol qui an accuat timat of th machin paamt in all opating point; it hould b don continuouly on-lin to obtain a liabl timat of machin vaiabl. Vaiou chm hav bn popod fo oto tim contant adaptation uch a th modl fnc adaptiv contol (MRAC) tchniqu [6, 7]. Thi adaptation i low and load nitiv. Som of th tchniqu injct diffnt tt ignal [8]. An xtndd kalman filt ha alo bn mployd [9]. Som oth mthod lik cuiv lat qua mthod hav bn popod in [10, 11]. Atificial nual ntwok (ANN) mthod fo th timation of oto tim contant and induction moto paamt w alo invtigatd [12-16]. Howv, mot of th tchniqu qui xtniv onlin mathmatical calculation, which will ctainly inca th hadwa complxiti and cot. Alo om of thm a unobut in load toqu vaiation cau, making thm unuitabl fo pactical application. Hnc a impl univally accptabl mthod i yt to b dicovd [17, 18]. Th popod timation block in thi pap conit of two pat. At fit, flux and toqu a timatd by uing th maud voltag and cunt. Thn, a nual ntwok timato, which i fd by flux and toqu o and a uppod oto itanc, timat th actual oto itanc. Thi mthod ha hown om advantag uch a tability, liability, apid convgnc and obutn ov load toqu vaiation. In ction 2, th oto tim contant timation chm popod in th litatu hav bn viwd. Sction 3 dcib th dynamic modling of indict vcto contol of an induction moto. Th pincipl of atificial nual ntwok a pntd in ction 4. Th pincipl of th popod oto itanc timato, including oto flux and toqu timation, nual ntwok timato and it taining pocdu a pntd in ction 5. Sytm imulation tudi a includd in ction 6. Concluding mak a finally povidd in ction REVIEW OF ROTOR TIME CONSTANT ESTIMATION TECHNIQUES Th timation of th oto tim contant contitut a ubjct of intt fo val ach tam, and val olution hav bn popod in th litatu [6-18]. Mot of th mthod qui intniv calculation to convg and a tim conuming [8, 9]. Futhmo, thy ith qui accuat knowldg of tato itanc [8, 14] o a adaptd only fo pcific opating condition and a nitiv to load changing [6]. Th modl fnc adaptiv contol (MRAC) ha bn ud in fnc [6, 7]. Thi mthod qui calculation of two function, F and F, uing contol vaiabl that nu th condition of flux ointation and machin vaiabl, pctivly. Th diffnc btwn function F and F contitut a condition of d-tuning and mut b cancld. In thi mthod, pci timation of tato itanc R i mandatoy. Rfnc [9] popo uing Extndd Kalman Filt (EKF) to timat oto itanc. It ha modld th oto itanc a an additional tat vaiabl of th machin, and th hamonic contnt gnatd by th PWM invt i modld a whit Gauian noi. Thi mthod qui intniv calculation and manipulation of lag matic and vcto. Moov, bfo implmntation, an off-lin Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2 Apil 2006

3 Roto itanc idntification uing nual ntwok fo 225 calculation i ncay, uing input vaiabl coponding to a ctain opating point (linaization). Thi mthod pnt th ik of nonconvgnc, pcially if th opating condition a diffnt fom tho ud fo off-lin calculation. Th concpt of a dviation angl of th flux vcto along d-axi ha bn pntd in fnc [10]. Calculation of thi angl qui knowldg of tato voltag and cunt, and dpnd on th tato itanc R, mutual inductanc M and oto inductanc. Sinc tato itanc i ud, thi timation chm cannot b liably ud in a low pd gion; hnc, an altnativ pci idntification poc mut b availabl. Th cuiv lat qua (RS) [11] mthod i hown to povid a poo timat of th oto itanc, with o of 20-30% in th timatd valu compad with th poibl thmal vaiation in oto itanc of up to 50%. Atificial nual ntwok (ANN) mthod fo th timation of th oto tim contant of th induction moto w alo invtigatd. In [12], an adaptation chm bad on th tady tat quation of a cunt-fd induction moto i popod. It pincipal limitation a latd to: th dynamic tim pon, which i low than th popod timato; th lction citia of th taining data t that mut pcily pnt th opating condition of th moto; and th taining tim of th ANN, which can b xciv. Th ult of [13, 14] how that th ytm convg within 75 m and 2. Howv, th mthod pnt th ik of low convgnc. Th ult of [15] i fo on amount of toqu fnc, o it will b nitiv to load vaiation. 3. DYNAMIC MODEING OF INDIRECT ROTOR FUX ORIENTED CONTRO OF AN INDUCTION MOTOR In an IRFOC, th ynthi of th unit vcto i indpndnt of th machin tminal condition. Fig. 1 xplain th pincipl [3]. At any intant, th q lctical axi i at angula poition θ with pct to th q axi. Th angl θ i givn by th um of oto angula poition θ and lip angula poition θ l. Th oto flux ψ i alignd with th d axi. q i q θ l θ Mch. axi q θ i d ψˆ d Fig. 1. Phao diagam fo indict vcto contol Th following quation a valid fo otating fam d -q quivalnt cicuit d ω dψ dt q R ψ q m R iq ω ψ l d = 0 (1) Apil 2006 Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2

4 226 M. Ebahimi / t al. dψ dt d R ψ d m R id ω ψ l q = 0 (2) Fo dcoupling contol it i diabl that T 3 P m = ( ) ( iqψ d idψ ) (3) 2 2 q q dψ ψ q = = 0 (4) dt d ψ =ψˆ = con tant (5) dψ dt Subtituting th fit two condition, Eq. (1) and (2) can b implifid a: d = 0 (6) m R ω l = ( ) iq (7) ψˆ R dψˆ ψˆ dt = mid (8) q Subtituting ψ = 0 and ψ d = ψˆ in th toqu xpion yild Th quation abov, togth with mchanical quation T 3 P = ( ) ψˆ (9) 2 2 m iq 2 dω ( ) J = T Tl (10) p dt dcib th machin modl in dcoupling contol. Figu 2 how a ytm uing th indict mthod of vcto contol. i d fo th did ψ i dtmind fom Eq. (8), and iq fo th did T i dtmind fom Eq. (9). Th t valu of lip ω l i latd to cunt i q by Eq. (7). Th lip fquncy ω l i addd to oto pd ω to obtain ω and θ. In continuation, th computation fo th coodinat chang and two-pha to th-pha tanfom will b caid out. Th th pha cunt command i poducd by a CRPWM and fd to an induction moto. A uccful implmntation of th indict fild-ointd contol qui an accuat calculation of th lip fquncy ( Eq. (7)). Th accuacy of thi lip fquncy calculation dpnd lagly on th accuacy of th moto paamt, pcially on th oto tim contant [4]. Hnc, an on-lin adaptation/timation of th oto tim contant i ncay fo a coct fild-ointd opation. 4. PRINCIPES OF ARTIFICIA NEURA NETWORKS Atificial nual ntwok u a dn intconnction of computing nod to appoximat nonlina function [19-21]. A hown in Fig. 2, ach nod contitut a nuon and pfom th multiplication of it input ignal by contant wight, um up th ult and map th um to a nonlina activation function φ; th ult a thn tanfd to it output. A fd-fowad ANN i oganizd in lay: an input lay, on o mo hiddn lay, and an output lay. Th mathmatical modl of a nuon i givn by Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2 Apil 2006

5 Roto itanc idntification uing nual ntwok fo 227 N y = ϕ wi. xi b (11) i= 1 wh: (x 1, x 2,,x N ) a input fom th pviou lay nuon, (w 1, w 2,,w N ) a th coponding wight and b i th bia of th nuon. φ i gnally th logaithmic o tangnt igmoidal activation function. X 1 W 1 1 X 2... W 2 W N b y X N Fig. 2. Stuctu of nual ntwok lmnt Th ANN i taind by a laning algoithm that pfom th adaptation of wight of th ntwok itativly until th o btwn tagt vcto and th output of th ANN i l than an o goal. Th mot popula laning algoithm fo multilay ntwok i th back-popagation algoithm and it vaiant. 5. PRINCIPES OF THE PROPOSED ROTOR RESISTANCE ESTIMATOR Ou goal i to dvlop a tchniqu fo timating th oto itanc uing only tato voltag and cunt. It conit of two pat; th fit i a flux and toqu timation block who input a voltag and cunt. It do not dpnd on oto itanc. In continuation, th timatd flux and toqu a compad with thi command and th o a computd. If th oto itanc in an indict vcto contoll qual to actual oto itanc of an induction moto, th o will b qual to zo. Othwi, if th oto itanc ha any chang, th o will appa; manwhil, th magnitud of o of flux and toqu dpnd on load toqu vaiation. Bcau th whol ytm i nonlina and complx, it i not poibl to timat th oto itanc imply by uing th vaiabl; o, in th cond pat a nual ntwok (NN) ha bn ud a a oto itanc timato. Th whol ytm i hown in Fig. 3. AC Rc. ψ T 4 3P m 1 m m R ω l i d i q 1 S j θ 2 3 θ id i q 1 S ω ia ib i c _ VSI ψ _ ψ _ Sampl & Hold T ia ib ic Hyti Band i abc Toqu & Flux Etimato IM Spd Sno v abc T Nual Ntwok Fig. 3. Block diagam of indict vcto contol of an induction moto div and nual ntwok oto itanc timato Apil 2006 Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2

6 228 M. Ebahimi / t al. a) Roto flux and toqu timation modl In th popod ytm, th input of NN block a flux and toqu o. So th vaiabl mut b timatd. It i poibl to tablih a flux and toqu modl which do not u th monitod pd, but u only th monitod valu of tato voltag and cunt. Thi modl do not dpnd on oto itanc; o, th timatd flux and toqu a accuat and coct, vn if th oto itanc ha om vaiation du to tmpatu vaiation and kin ffct. Fo thi pupo, tminal pha voltag and cunt a nd, and thn thy a tanfomd fom a th-pha ytm to th tationay d -q fnc fam. Th following quation of tato voltag and flux can b wittn fom tationay fam quivalnt cicuit [22]. v v q d q d = R iq ψ q (12) dt d = R id ψ d (13) dt iq miq ψ = (14) d id mid Th oto cunt can b divd fom tato voltag and cunt a: ψ = (15) 1 i q = ( vq Riq ) dt m 1 i d = ( vd Rid ) dt m m m q i d i (16) (17) Th oto flux can b wittn a: q iq miq ψ = (18) Th oto flux and toqu quation a T d id mid ψ = (19) 2 2 d ψ q ψ = ψ (20) 3 p m = ( iqψ d idψ q ) (21) 2 2 A computation flow diagam fo timating flux and toqu i hown in Fig. 4. ia ib ic 3 2 i q i d R S m m ψ q 1 i q m ψ q 3 P m ( i q ψ d idψ q ) 2 2 T va vb vc 3 2 v q v d R S m m ψ d 1 i d m ψ d ( ψ ) ( ψ ) 2 q 2 d ψ Fig. 4. Etimation of toqu and oto flux fom tato cunt and voltag Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2 Apil 2006

7 Roto itanc idntification uing nual ntwok fo 229 b) Nual ntwok timato tuctu Th tuctu of th popod fd-fowad nual ntwok ud fo timation i indicatd in Fig. 5. Th ntwok i a MP typ nual ntwok with fou lay, i.., input lay, two hiddn lay, and th output lay. Th cicl in th ntwok pnt th nuon. Th input and output lay hav nuon qual to th pctiv numb of ignal, wha ach of th hiddn lay in th pnt dign ha 10 nuon. Th topology i dfind a ntwok. Th ntwok i fully connctd, i.., th output of ach nuon i connctd to all th nuon in th fowad lay though a wight. Bid, a bia ignal i coupld to all th nuon of th hiddn and output lay though a wight [23]. Th hiddn lay and output lay nuon hav a igmoid typ nonlina tanf function givn a: 1 f ( x) = (22) ( xθ ) 1 wh θ i th bia. Th nonlina tanf function aociatd with nuon giv nonlina mapping popty of th ntwok [19]. T R c R t ψ T Fig. 5. Topology of th nual ntwok fo oto itanc timation Th input vaiabl ignal a convtd to p-unit fom though th nomaliz gain, and thn aft computation, th output i bought back to actual valu though dnomaliz gain, a indicatd. Th taining and th opating pocdu a xplaind in th following ction. c) Taining pocdu Th taining pocdu ud in th pnt pojct can b ummaizd a follow: Simulat th induction moto div ytm a hown in Fig. 3 by MATAB/SIMUINK Gnat th input/output data tabl fo diffnt opating condition a hown in Fig. 6-a. Th input data copond to th timatd flux and toqu o, toqu command and th amount of oto itanc in contoll R c. Th output data copond to th did timatd oto itanc R a. Convt th data tabl to p-unit fom and fd to th nual ntwok imulato pogam locatd in PC. Aign andom wight initially to th ntwok by th imulato. Slct an input/output data pai fom th tabl. Fo th givn input data pattn calculat th ntwok output and compa with th did data output to div th o pattn. A hown in Fig. 6-b fom th o pattn, comput and adjut th ntwok wight by a backpopagation algoithm (gadint dcnt with adaptiv laning at) o that th nw o i mall. Rpat th abov tp with ach t of input/output data pattn until th m o fo th nti taining t convg blow th did thhold valu. Aft compltion of th taining, tt th ntwok pfomanc with abitay input pattn to nu uccful taining. Apil 2006 Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2

8 230 M. Ebahimi / t al. ψ T R a R c Indict Vcto Contol of Induction Moto Flux and Toqu Etimation ψ T ψ T ψ T (a) (b) Fig. 6. (a) Gnation of input/output data tabl (b) Pocdu of taining nual ntwok T R c ψ T R t R a Wight Adjutmnt Algoithm 6. SYSTEM SIMUATION STUDIES A 3-hp induction moto wa ud to imulat th indict vcto contol of Fig. 3. Rating and paamt of th machin a givn in th appndix. In thi ytm th actual flux and toqu a timatd by uing tato voltag and cunt, and th oto itanc i timatd by a nual ntwok, thi timatd valu of th oto itanc i ud by IRFOC contoll intad of a contant valu. a) Gnat matic of data and taining NN A matix of input and output data in diffnt opating condition mut b gnatd to u fo taining th NN. Th input data matix (23) copond to th o of flux ψ, o of toqu T, toqu command T and th oto itanc that i ud in th contoll R c. [ input data] [ T T R ] = ψ (23) Th output data matix (24) copond to th did timatd oto itanc R a. [ data] [ ] Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2 Apil 2006 R a c output = (24) To gnat th data matic, th abov imulatd ytm wa ttd fo diffnt valu of R c, R a and T. To achiv thi pupo, th toqu command T wa vaid fom 0.2 pu to 1 pu in 5 tp, ach of which it wa incad 0.2 pu. Th actual oto itanc R a wa vaid fom 1 pu to 2 pu in 9 tp, ach of which it wa incad pu. Th oto itanc in th contoll wa vaid fom 1 pu to 2 pu in 9 tp, in ach of which it wa incad pu. A a ult of th chang of paamt, th will b 405 ca. Th IRFOC of an induction moto with a flux and toqu timation block wa imulatd fo all of th ca. In ach ca, th o of flux ψ and that of toqu T w divd and avd, and alo T, R c and R a w avd. A a ult, th matic of input and output data with 405 ow w poducd. By uing th matic of input and output data a NN ha bn taind by backpopagation algoithm, a wa xplaind in ction 6-2.Th initial laning at η1,η2 and th momntum gain α w t to 0.35, 0.4 and 0.7, pctivly. Th convgnc thhold o lvl wa t to Aft itation th o lvl obtaind thhold o. b) Simulation ult Aft atifactoy taining with th hlp of th imulato pogam, th wight a downloadd to th pototyp ntwok and attmpt a mad to opat th div ytm of Fig. 2 with an NN a an timato. Th ytm ha bn tudid in th ca: Ca a: Th nominal oto itanc of 0.4 Ω wa takn fo th contoll vn though th actual oto itanc wa 0.8 Ω du to incaing th tmpatu. At 2 Sc. th NN timato i activatd, and th

9 Roto itanc idntification uing nual ntwok fo 231 oto itanc i timatd immdiatly. Fig. 7a how th actual and timatd oto itanc, whil Fig. 7b how th pcntag of o bfo and aft uing NN timato. Thi o i l than % 0.01 aft uing th NN. Fig. 7c how th command toqu and lctomagntic toqu bfo and aft uing NN timato. Th command toqu i 5 Nm, th actual toqu i 3 Nm bfo uing NN timato and 5 Nm aft uing it. Fig. 7d how th command and actual flux bfo and aft uing NN. Th command flux i 0.45 Wb and th actual flux i 0.5 Wb bfo uing NN. Th ult how that bfo uing NN a an timato th flux and toqu hav ocillation and om tady tat o. At 4 Sc. th command toqu dca to 2 Nm and th vcto contol i don uccfully, thu th actual toqu and flux follow thi command accuatly. Tim(c) Fig. 7. Th pfomanc of th div bfo and aft uing NN timato, (a) actual and timatd oto itanc, (b) pcntag of timatd oto itanc o, (c) command and actual toqu, (d) command and actual flux, () oto pd Apil 2006 Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2

10 232 M. Ebahimi / t al. Ca b: Th pfomanc of th div without a oto itanc timato ha bn tudid. Th oto itanc gadually chang du to tmpatu chang caud by toqu cunt changing. In Fig. 8a and 8c th vaiation of oto itanc and command toqu a hown. At fit, it i aumd that th command toqu i qual to zo, and th oto itanc i qual to 0.4 Ω. At 2 Sc. th command toqu i incad to 2 Nm, and th oto itanc bgin to inca xponntially, aching to Ω. At 7 Sc. th toqu i incad to 5 Nm, and th itanc i incad to 0.8 Ω. Thn, th toqu i dcad to 3 Nm at 15 Sc. and th itanc i xponntially dcad to Ω. In thi ca, th i no timato, o th actual oto itanc ha om vaiation, howv th amount of oto itanc in th contoll block ha bn fixd to 0.4 Ω. Th pcntag of o btwn thm i hown in Fig. 8b. In Fig. 8c and 8d th command and actual toqu and flux a hown. Th ult how that th pfomanc of vcto contoll without th timato will b ditactd, o th flux and toqu hav om ocillation whn th command toqu i changd and th i om tady tat o in thm. Tim(c) Fig. 8. Th pfomanc of th div without any timato, th oto itanc ha a gadual chang, (a) actual oto itanc, (b) pcntag of timatd oto itanc o, (c) command and actual toqu, (d) command and actual flux, () oto pd Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2 Apil 2006

11 Roto itanc idntification uing nual ntwok fo 233 Ca c: Th oto itanc ha a gadual chang lik ca b, but it i aumd that th nual ntwok timato ha bn activatd inc th bginning of th poc. Th witching fquncy of th ntwok wa 5 Hz, hnc th nual ntwok fquncy wa chon to giv th plant nough tim to tabiliz it output. Th actual oto itanc and timatd itanc a hown in Fig. 9a. Th timatd oto itanc cloly follow th actual oto itanc. Th magnitud of thi timation o i hown in Fig. 9b, th maximum o i l than ±3%. In Fig. 9c and 9d, th command and actual toqu and flux a hown. Th ult how that th vcto contol i valid whn th oto itanc ha om changing, and NN timato i activatd. Th actual flux i fixd to it command valu, and th actual toqu i tacking it command valu, without any ocillation o tady tat o. Tim(c) Fig. 9. Th pfomanc of th div with NN timato, th oto itanc ha a gadual chang, (a) actual and timatd oto itanc, (b) pcntag of timatd oto itanc o, (c) command and actual toqu, (d) command and actual flux, () oto pd Apil 2006 Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2

12 234 M. Ebahimi / t al. 7. CONCUSIONS In thi pap, a impl algoithm ha bn dvlopd fo th timation of oto itanc ud in indict oto flux ointd contol of induction moto div. Thi timato i bad on nual ntwok pincipl and qui only a maumnt of accibl vaiabl (voltag and cunt). By uing th vaiabl, th flux and th toqu a timatd. In th nxt tag, a fou-lay nual ntwok with tuctu i fd by th o of toqu, o of flux, command toqu, and th amount of oto itanc in contoll to timat th actual valu of oto itanc. Th NN laning poc ha bn pfomd off-lin bad on th mathmatical modl of th IRFOC ytm. Th comput imulation ult hav hown th validity and th faibility of th popod mthod. Th witching fquncy of th nual ntwok wa 5 Hz and th pfomanc of th timato wa found to b xcllnt in a wid ang of oto itanc vaiation fom 0.4 Ω to 0.8 Ω. Th ytm can adjut intantanouly and compnat th vaiation of oto itanc caud by hating o ddy cunt. Th maximum timation o i l than ±3%. Accuat, fat timation, implicity of dign and innitivity to load vaiation a th advantag of thi mthod. Th popod mthod could b imply adaptd to u in th oth chm of flux ointation; namly, tato and ai gap flux ointation. Acknowldgmnt- Th autho would lik to acknowldg th financial uppot povidd by Ifahan Univity of Tchnology. NOMENCATURE i d, i q tato cunt in d- and q-axi m, oto and magntizing inductanc tato inductanc P numb of pol R oto itanc R a timatd oto itanc R c oto itanc that i ud in th contoll tato itanc R T T, T l command toqu dvlopd and load toqu υ d, υ q tato voltag in d-and q-axi ψ d, ψ q oto flux in d-and q-axi ψ oto flux ψ, tato flux in d-and q-axi d ψ q REFERENCES 1. ipo, T. & Novotny, D. (1985). Intoduction to fild ointation and high pfomanc div. Tutoial cou, IEEE AS, Ebahimi, M., Sifi, H., Shoulai, A. & Saaf, H. S. (1999). A oftwa modification pocdu fo convion of a cal contoll to a vcto typ fo an induction moto. Ianian Jounal of Scinc and Tchnology, 23, Bo, K. (1986). Pow lctonic and AC div. Pntic-Hall. Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2 Apil 2006

13 Roto itanc idntification uing nual ntwok fo Kihman, R. (1991). A viw of paamt nitivity and adaptation in indict vcto contolld induction moto div ytm. IEEE Tan. on Pow Elc., 6(4), D Donk, R. W. (1994). Paamt nitivity of indict unival fild-ointd contoll. IEEE Tan. on Pow Elc., 9(4), Rowan, T. (1991). A impl on-lin adaptation fo indict fild ointation of an induction machin. IEEE Tan. on Induty Application, 37, Guz, P. P. (2000). Induction moto pac vcto contol uing adaptiv fnc modl dict and indict mthod. Poc. IEEE ISIE'2000, Publo, Mxico, Matuo, T. & ipo, T. A. (1993). A nw mthod fo oto tim contant tuning in indict fild ointd contol. IEEE Tan. on Pow Elc., 8(3), in, F. S. (1996). Application of EKF and RS timato in induction moto div. IEEE PESC, 1, Bavno, Italy, in, W. & Vnkatan, R. (1992). A nw adaptiv contol chm fo indict vcto contol ytm. Poc. IEEE IAS Annu. Mting, 1, Houton, USA, Bouak, M. & Capolino, G. (1992). Rcuiv lat qua oto tim contant idntification fo vcto contolld induction machin. Elc. Mach. Pow Syt., 20(2), Ba-Razzouk, A., Chiti, A. & Olivi, G., (1996). Atificial nual ntwok oto tim contant adaptation in indict fild ointd contol div. Poc. IEEE,1, Mayalh, S. & Bayindi, N. S. (1998). on-lin timation of oto itanc of an induction moto uing cunt nual ntwok. Elctonic ltt, 34(8). 14. Kaanayil, B., Rahman, M. F. & Gantham, C. (2001). Roto itanc idntification uing atificial nual ntwok fo an indict vcto contolld induction moto div. in Poc. IEEE IECON 01, Dnv, USA, Ebahimi, M., Shoulai, A., Sifi, H. & Tahani, V. (1997). Compnation of oto tim contant vaiation in induction machin uing atificial nual ntwok. Intnational Jounal of Engining Scinc, 8(2a), Fodo, D., Giva, G. & Pofumo, F. (1995). Compnation of paamt vaiation in induction moto div uing a nual ntwok. Conf. Rc. PESC 95, Atlanta, USA, Ba-Razzouk, A., Chiti, A. & Sicad, P. (2002). Implmntation of a DSP bad al-tim timato of induction moto oto tim contant. IEEE Tan. on Pow Elc., 17(4). 18. Toliyat, H. & Afn, M. S. (1999). Roto tim contant updating chm fo a oto flux ointd induction moto div. IEEE Tan. on Pow Elc., 14(5). 19. Haykin, S. (1994). Nual ntwok, a comphniv foundation. Macmillan Collg publihing Company. 20. awnc, J. (1993). Intoduction to nual ntwok. Califonia Scintific Softwa P. 21. Sinncio, E. S. & au, C. (1992). Atificial nual ntwok. NwYok: IEEE P, Va, P. (1990). Vcto contol of AC Machin. Oxfod Scinc Publication. 23. Ebahimi, M. (2003). Roto itanc idntification uing nual ntwok fo an induction moto div. Rach Pojct Rpot, Ifahan Univity of Tchnology. Induction moto data APPENDIX Ratd pow 3 hp Numb of pol, p 4 Ratd tato voltag 220 V Roto itanc, R Ω Apil 2006 Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2

14 236 M. Ebahimi / t al. Stato itanc, R Ω Magntizing itanc, X m Ω Roto lakag actanc, X l Ω Stato lakag actanc, X l Ω Mchanical intia contant, J kg.m 2 Ianian Jounal of Scinc & Tchnology, Volum 30, Numb B2 Apil 2006

Studying the Steady State Performance Characteristics of Induction Motor with Field Oriented Control Comparing to Scalar Control

Studying the Steady State Performance Characteristics of Induction Motor with Field Oriented Control Comparing to Scalar Control EJERS, Euopan Jounal of Engining Rach and Scinc Studying th Stady Stat fomanc Chaactitic of nduction Moto with Fild Ointd Contol Compaing to Scala Contol Hamdy Mohamd Soliman Abtact Fild ointd contol i

More information

Robustness Evaluation of SMO in Sensorless Control of BLDC Motor under DTC Scheme

Robustness Evaluation of SMO in Sensorless Control of BLDC Motor under DTC Scheme Robutn Ealuation of SMO in Snol Contol of BDC Moto und DTC Schm Giija P.., Studnt Mmb, IEEE, and Pinc A., Mmb, IEEE Abtact-- Dict Toqu Contol (DTC i a mthod to contol th toqu in aiabl fquncy di. Thi pap

More information

SLIDING MODE VECTOR CONTROL OF THREE PHASE INDUCTION MOTOR

SLIDING MODE VECTOR CONTROL OF THREE PHASE INDUCTION MOTOR SLIDING MODE VECTOR CONTROL OF THREE PHASE INDUCTION MOTOR A THESIS SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF Mat of Tchnology in Pow Contol and Div By SOBHA CHANDRA BARIK

More information

Sliding Mode Observer Based Sensorless Control of BLDC Motor under DTC Scheme

Sliding Mode Observer Based Sensorless Control of BLDC Motor under DTC Scheme ISSN (Onlin): 2278 8875 Intnational Jounal of Adancd Rach in Elctical, Elctonic and Intumntation Engining (An ISO 3297: 2007 Ctifid Oganization) Vol. 2, Iu 11, Nomb 2013 Sliding Mod Ob Bad Snol Contol

More information

Monitoring and diagnostic methods for eccentricity faults in the induction motor

Monitoring and diagnostic methods for eccentricity faults in the induction motor Pocding of th Intnational Confnc on Cicuit, Sytm, Signal Monitoing and diagnotic mthod fo ccnticity fault in th induction moto A. Mtatla*,S. Bnzahioul*, T. Bahi**, and D. fbv*** *Dpatmnt of Elctomchanical,

More information

COMPSCI 230 Discrete Math Trees March 21, / 22

COMPSCI 230 Discrete Math Trees March 21, / 22 COMPSCI 230 Dict Math Mach 21, 2017 COMPSCI 230 Dict Math Mach 21, 2017 1 / 22 Ovviw 1 A Simpl Splling Chck Nomnclatu 2 aval Od Dpth-it aval Od Badth-it aval Od COMPSCI 230 Dict Math Mach 21, 2017 2 /

More information

Closed Loop Speed Control of Induction Generator with Scalar-Control Inverters

Closed Loop Speed Control of Induction Generator with Scalar-Control Inverters Availabl onlin at www.cincdict.com Eng Pocdia 34 (013 ) 371 381 10th Eco-Eng and Matial cinc and Engining (EME01) Clod Loop pd Contol of Induction Gnato with cala-contol Invt Anaphat Upaan and Yuttana

More information

DIRECT TORQUE CONTROL OF MULTILEVEL INVERTER- FED INDUCTION MACHINES A SURVEY

DIRECT TORQUE CONTROL OF MULTILEVEL INVERTER- FED INDUCTION MACHINES A SURVEY 31 t July 2012. Vol. 41 No.2 2005-2012 JAI & LLS. All ight vd. DIREC ORQUE CONROL OF MULILEVEL INVERER- FED INDUCION MACHINES A SURVEY 1 NAZIHA AHMAD AZLI, 2 NORJULIA MOHD NORDIN, 3 NIK RUMZI NIK IDRIS

More information

Extinction Ratio and Power Penalty

Extinction Ratio and Power Penalty Application Not: HFAN-.. Rv.; 4/8 Extinction Ratio and ow nalty AVALABLE Backgound Extinction atio is an impotant paamt includd in th spcifications of most fib-optic tanscivs. h pupos of this application

More information

References. Basic structure. Power Generator Technologies for Wind Turbine. Synchronous Machines (SM)

References. Basic structure. Power Generator Technologies for Wind Turbine. Synchronous Machines (SM) Gnato chnologi fo Wind ubin Mhdad Ghandhai mhdad@kth. Rfnc 1. Wind Plant, ABB, chnical Alication Pa No.13.. WECC Wind Plant Dynamic Modling Guid, WECC Rnwabl Engy Modling ak Foc. 3. Wind ubin Plant Caabiliti

More information

Lecture 2: Frequency domain analysis, Phasors. Announcements

Lecture 2: Frequency domain analysis, Phasors. Announcements EECS 5 SPRING 24, ctu ctu 2: Fquncy domain analyi, Phao EECS 5 Fall 24, ctu 2 Announcmnt Th cou wb it i http://int.c.bkly.du/~5 Today dicuion ction will mt Th Wdnday dicuion ction will mo to Tuday, 5:-6:,

More information

Induction Motor Flux Estimation using Nonlinear Sliding Observers

Induction Motor Flux Estimation using Nonlinear Sliding Observers Jounal of Mathmatic and Statitic (): 6-69 007 ISSN 9-6 007 Scinc Publication Induction Moto Flux Etimation uing Nonlina Sliding Obv Hakiki Khalid Mazai Bnyounè and Djab Sid Ahmd Laboatoi d Automatiqu t

More information

Steady-State Analysis and Control of Double Feed Induction Motor

Steady-State Analysis and Control of Double Feed Induction Motor ntnational Jounal of Elctonic and Elctical Engining 6 2012 Stady-Stat Analyi and Contol of Doubl Fd nduction Moto H. Sdiki, Dj. Ould Abdlam, T. Otman-chif, A. Bchouch, K. Mbah Abtact Thi pap xplo tady-tat

More information

Direct Power Control of a Doudly Fed Induction Generator with a Fixed Switching Frequency

Direct Power Control of a Doudly Fed Induction Generator with a Fixed Switching Frequency Dict Pow Contol of a Doudly Fd Induction Gnato with a Fixd Switching Fquncy Won-Sang i, Sung-Tak Jou, yo-bu L School of Elctical and Coput Engining Ajou Univity, Suwon, oa kyl@ajou.ac.k Stv Watkin Fladh

More information

Inertia identification based on adaptive interconnected Observer. of Permanent Magnet Synchronous Motor

Inertia identification based on adaptive interconnected Observer. of Permanent Magnet Synchronous Motor Intnational Jounal of Rsach in Engining and Scinc (IJRES) ISSN (Onlin): 232-9364, ISSN (Pint): 232-9356 www.ijs.og Volum 3 Issu 9 ǁ Sptmb. 25 ǁ PP.35-4 Intia idntification basd on adaptiv intconnctd Obsv

More information

Solutions to Supplementary Problems

Solutions to Supplementary Problems Solution to Supplmntay Poblm Chapt Solution. Fomula (.4): g d G + g : E ping th void atio: G d 2.7 9.8 0.56 (56%) 7 mg Fomula (.6): S Fomula (.40): g d E ping at contnt: S m G 0.56 0.5 0. (%) 2.7 + m E

More information

Three-Level Five-Phase Space Vector PWM Inverter for a Two Five-Phase Series Connected Induction Machine Drive

Three-Level Five-Phase Space Vector PWM Inverter for a Two Five-Phase Series Connected Induction Machine Drive Engy an Pow Engining, 21, 1-17 oi:1.4236/p.21.213 Publih Onlin Fbuay 21 (http://www.cip.og/jounal/p) Th-Lvl Fiv-Pha Spac Vcto PWM Invt fo a Two Fiv-Pha Si Connct Inuction Machin Div N. R. ABJADI 1, J.

More information

Dynamical models for fault detection in squirrel cage induction motors

Dynamical models for fault detection in squirrel cage induction motors Int. J. Citical Infatuctu, Vol., No. 1/, 7 161 Dynamical modl fo fault dtction in quil cag induction moto H. Rodíguz-Coté* Dpatmnt of Elctical and Comput Engining Nothatn Univity Boton, A 115, USA E-mail:

More information

Robustness Analysis of Stator Voltage Vector Direct Torque Control for Induction Motor

Robustness Analysis of Stator Voltage Vector Direct Torque Control for Induction Motor IX Symoium Indutial Elctonic INEL, Banja Luka, Novm 3, Routn Analyi of Stato Voltag Vcto ict oqu Contol fo Induction Moto Alkanda Ž. Rakić, Sloodan N. Vukoavić Univity of Blgad, School of Elctical Engining

More information

A Review on Direct Torque Control of Induction Motor

A Review on Direct Torque Control of Induction Motor J. M. R. Malla t. al. / Intnational Jounal of Nw chnologi in Scinc and Engining Vol. 1, Iu. 1, Jan. 2014, ISSN XXXX-XXXX A Rviw on Dict Toqu Contol of Induction Moto Jagan Mohana Rao Malla and Manti Maiya

More information

Parameter Identification of a Brushless Resolver Using Charge Response of Stator Current

Parameter Identification of a Brushless Resolver Using Charge Response of Stator Current Achiv of SID Paamt Intification of a Buhl Rolv Uing Chag Rpon of Stato Cunt D. Aa-Khaui*, F. Tootoonchian* an Z. Naii-Ghiai** Atact: Bcau of tmpatu inpnnc, high olution an noil output, uhl olv a wily u

More information

(( ) ( ) ( ) ( ) ( 1 2 ( ) ( ) ( ) ( ) Two Stage Cluster Sampling and Random Effects Ed Stanek

(( ) ( ) ( ) ( ) ( 1 2 ( ) ( ) ( ) ( ) Two Stage Cluster Sampling and Random Effects Ed Stanek Two ag ampling and andom ffct 8- Two Stag Clu Sampling and Random Effct Ed Stank FTE POPULATO Fam Labl Expctd Rpon Rpon otation and tminology Expctd Rpon: y = and fo ach ; t = Rpon: k = y + Wk k = indx

More information

MOS transistors (in subthreshold)

MOS transistors (in subthreshold) MOS tanito (in ubthhold) Hitoy o th Tanito Th tm tanito i a gnic nam o a olid-tat dvic with 3 o mo tminal. Th ild-ct tanito tuctu wa it dcibd in a patnt by J. Lilinld in th 193! t took about 4 ya bo MOS

More information

(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4)

(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4) ots lctu Th IS/LM modl fo an opn conomy is basd on a fixd pic lvl (vy sticky pics) and consists of a goods makt and a mony makt. Th goods makt is Y C+ I + G+ X εq (.) E SEK wh ε = is th al xchang at, E

More information

PERFORMANCE IMPROVEMENT OF THE INDUCTION MOTOR DRIVE BY USING ROBUST CONTROLLER

PERFORMANCE IMPROVEMENT OF THE INDUCTION MOTOR DRIVE BY USING ROBUST CONTROLLER PEFOMANCE MPOEMEN OF HE NDUCON MOO DE BY USNG OBUS CONOE S. SEAA, PG Schola,. GEEHA, ctu, N. DEAAAN, Aitant Pofo Abtact -: h tanint pon of th induction oto i obtaind by uing it d-q fnc odl. h tanint pon

More information

STRIPLINES. A stripline is a planar type transmission line which is well suited for microwave integrated circuitry and photolithographic fabrication.

STRIPLINES. A stripline is a planar type transmission line which is well suited for microwave integrated circuitry and photolithographic fabrication. STIPLINES A tiplin i a plana typ tanmiion lin hih i ll uitd fo mioav intgatd iuity and photolithogaphi faiation. It i uually ontutd y thing th nt onduto of idth, on a utat of thikn and thn oving ith anoth

More information

GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL

GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL Ioannis Iaklis Haanas * and Michal Hany# * Dpatmnt of Physics and Astonomy, Yok Univsity 34 A Pti Scinc Building Noth Yok, Ontaio, M3J-P3,

More information

FUZZY LOGIC BASED CONTROLLER FOR FIVE PHASE INDUCTION MOTOR DRIVE SYSTEM

FUZZY LOGIC BASED CONTROLLER FOR FIVE PHASE INDUCTION MOTOR DRIVE SYSTEM FUZZY LOGIC BASED CONTROLLER FOR FIVE PHASE INDUCTION MOTOR DRIVE SYSTEM Akshay M. Suyawanshi and Anant A. Kulkani 2 PG Studnt, M.B.E. Socity s Collg of, Engining, Ambajogai (M.S), India 2 PG Dpatmnt,

More information

STATISTICAL MECHANICS OF DIATOMIC GASES

STATISTICAL MECHANICS OF DIATOMIC GASES Pof. D. I. ass Phys54 7 -Ma-8 Diatomic_Gas (Ashly H. Cat chapt 5) SAISICAL MECHAICS OF DIAOMIC GASES - Fo monatomic gas whos molculs hav th dgs of fdom of tanslatoy motion th intnal u 3 ngy and th spcific

More information

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics Aakash A UNIQUE PPRTUNITY T HELP YU FULFIL YUR DREAMS Fo Class XII Studying / Passd Studnts Physics, Chmisty & Mathmatics Rgistd ffic: Aakash Tow, 8, Pusa Road, Nw Dlhi-0005. Ph.: (0) 4763456 Fax: (0)

More information

CDS 101/110: Lecture 7.1 Loop Analysis of Feedback Systems

CDS 101/110: Lecture 7.1 Loop Analysis of Feedback Systems CDS 11/11: Lctu 7.1 Loop Analysis of Fdback Systms Novmb 7 216 Goals: Intoduc concpt of loop analysis Show how to comput closd loop stability fom opn loop poptis Dscib th Nyquist stability cition fo stability

More information

SIMPLIFICATIONS AND SOLUTIONS OF DIFFRACTION FUNCTIONS IN NONLINEAR ACOUSTIC PARAMETER MEASUREMENT

SIMPLIFICATIONS AND SOLUTIONS OF DIFFRACTION FUNCTIONS IN NONLINEAR ACOUSTIC PARAMETER MEASUREMENT ICSV Cain Autalia 9- July 7 SIMPLIFICATIONS AN SOLUTIONS OF IFFRACTION FUNCTIONS IN NONLINEAR ACOUSTIC PARAMETER MEASUREMENT jilali Koutich Launt Alliè Rachid Gula and Mutapha Nadi LIEN Nancy-Univité Faculté

More information

E F. and H v. or A r and F r are dual of each other.

E F. and H v. or A r and F r are dual of each other. A Duality Thom: Consid th following quations as an xampl = A = F μ ε H A E A = jωa j ωμε A + β A = μ J μ A x y, z = J, y, z 4π E F ( A = jω F j ( F j β H F ωμε F + β F = ε M jβ ε F x, y, z = M, y, z 4π

More information

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then SYSTEM PERFORMANCE Lctur 0: Stady-tat Error Stady-tat Error Lctur 0: Stady-tat Error Dr.alyana Vluvolu Stady-tat rror can b found by applying th final valu thorm and i givn by lim ( t) lim E ( ) t 0 providd

More information

ORBITAL TO GEOCENTRIC EQUATORIAL COORDINATE SYSTEM TRANSFORMATION. x y z. x y z GEOCENTRIC EQUTORIAL TO ROTATING COORDINATE SYSTEM TRANSFORMATION

ORBITAL TO GEOCENTRIC EQUATORIAL COORDINATE SYSTEM TRANSFORMATION. x y z. x y z GEOCENTRIC EQUTORIAL TO ROTATING COORDINATE SYSTEM TRANSFORMATION ORITL TO GEOCENTRIC EQUTORIL COORDINTE SYSTEM TRNSFORMTION z i i i = (coωcoω in Ωcoiinω) (in Ωcoω + coωcoiinω) iniinω ( coωinω in Ωcoi coω) ( in Ωinω + coωcoicoω) in icoω in Ωini coωini coi z o o o GEOCENTRIC

More information

Tutorial 5 Drive dynamics & control

Tutorial 5 Drive dynamics & control UNIVERSITY OF NEW SOUTH WALES Electic Dive Sytem School o Electical Engineeing & Telecommunication ELEC463 Electic Dive Sytem Tutoial 5 Dive dynamic & contol. The ollowing paamete ae known o two high peomance

More information

INTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS

INTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS adjoint...6 block diagram...4 clod loop ytm... 5, 0 E()...6 (t)...6 rror tady tat tracking...6 tracking...6...6 gloary... 0 impul function...3 input...5 invr Laplac tranform, INTRODUCTION TO AUTOMATIC

More information

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation Pof. D. I. Nass Phys57 (T-3) Sptmb 8, 03 Foui_Tansf_phys57_T3 Foui tansfoms (Chapt 5) Foui intgals a gnalizations of Foui sis. Th sis psntation a0 nπx nπx f ( x) = + [ an cos + bn sin ] n = of a function

More information

Partial Fraction Expansion

Partial Fraction Expansion Paial Facion Expanion Whn ying o find h inv Laplac anfom o inv z anfom i i hlpfl o b abl o bak a complicad aio of wo polynomial ino fom ha a on h Laplac Tanfom o z anfom abl. W will illa h ing Laplac anfom.

More information

Joint Effect Analysis of Phase Noise, Carrier Frequency Offset, Doppler Spread and Nonlinear Amplifier on the Performance of OFDM System

Joint Effect Analysis of Phase Noise, Carrier Frequency Offset, Doppler Spread and Nonlinear Amplifier on the Performance of OFDM System 7th WSEAS Intnational Confnc on Application of Elctical Engining (AEE 8, ondhim, Noway, July -, 8 Joint Effct Analyi of Pha Noi, Cai Fquncy Offt, oppl Spad and Nonlina Amplifi on th Pfomanc of OFM Sytm

More information

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator Calculation of lctromotiv forc inducd by th lot harmonic and paramtr of th linar gnrator (*)Hui-juan IU (**)Yi-huang ZHANG (*)School of Elctrical Enginring, Bijing Jiaotong Univrity, Bijing,China 8++58483,

More information

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas Physics 111 Lctu 38 (Walk: 17.4-5) Phas Chang May 6, 2009 Lctu 38 1/26 Th Th Basic Phass of Matt Solid Liquid Gas Squnc of incasing molcul motion (and ngy) Lctu 38 2/26 If a liquid is put into a sald contain

More information

GRAVITATION 4) R. max. 2 ..(1) ...(2)

GRAVITATION 4) R. max. 2 ..(1) ...(2) GAVITATION PVIOUS AMCT QUSTIONS NGINING. A body is pojctd vtically upwads fom th sufac of th ath with a vlocity qual to half th scap vlocity. If is th adius of th ath, maximum hight attaind by th body

More information

FREQUENCY DETECTION METHOD BASED ON RECURSIVE DFT ALGORITHM

FREQUENCY DETECTION METHOD BASED ON RECURSIVE DFT ALGORITHM FREQUECY DETECTIO METHOD BAED O RECURIE ALGORITHM Katsuyasu akano*, Yutaka Ota*, Hioyuki Ukai*, Koichi akamua*, and Hidki Fujita** *Dpt. of ystms Managmnt and Engining, agoya Institut of Tchnology, Gokiso-cho,

More information

Induction Motor Control through AC/DC/AC Converters

Induction Motor Control through AC/DC/AC Converters Induction Moto Contol though ACDCAC Cont Abdahim Elfadili, Fouad Gii, Hamid Ouadi, Abdlmounim El Magi, uc Dugad, Abdlmajid Abouloifa To cit thi ion: Abdahim Elfadili, Fouad Gii, Hamid Ouadi, Abdlmounim

More information

Considerations Regarding the Flux Estimation in Induction Generator with Application at the Control of Unconventional Energetic Conversion Systems

Considerations Regarding the Flux Estimation in Induction Generator with Application at the Control of Unconventional Energetic Conversion Systems Conideation Regading the Flux Etimation in Induction Geneato with Application at the Contol of Unconventional Enegetic Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of

More information

ESE (Prelims) - Offline Test Series ELECTRICAL ENGINEERING SUBJECT: Electrical Machines & Systems and Signal Processing SOLUTIONS

ESE (Prelims) - Offline Test Series ELECTRICAL ENGINEERING SUBJECT: Electrical Machines & Systems and Signal Processing SOLUTIONS TEST ID: 30 ESE- 09 (Plims) - Offlin Tst Sis ELECTRICAL ENGINEERING Tst-3 SUBJECT: Elctical Machins & Systms and Signal Pocssing SOLUTIONS 0. Ans: (c) Sol: With hot-olld stl laminations max [B m ] A. A

More information

Mid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions

Mid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions Mid Ya Eamination 3 F. Matmatics Modul (Calculus & Statistics) Suggstd Solutions Ma pp-: 3 maks - Ma pp- fo ac qustion: mak. - Sam typ of pp- would not b countd twic fom wol pap. - In any cas, no pp maks

More information

8 - GRAVITATION Page 1

8 - GRAVITATION Page 1 8 GAVITATION Pag 1 Intoduction Ptolmy, in scond cntuy, gav gocntic thoy of plantay motion in which th Eath is considd stationay at th cnt of th univs and all th stas and th plants including th Sun volving

More information

Theoretical Extension and Experimental Verification of a Frequency-Domain Recursive Approach to Ultrasonic Waves in Multilayered Media

Theoretical Extension and Experimental Verification of a Frequency-Domain Recursive Approach to Ultrasonic Waves in Multilayered Media ECNDT 006 - Post 99 Thotical Extnsion and Expimntal Vification of a Fquncy-Domain Rcusiv Appoach to Ultasonic Wavs in Multilayd Mdia Natalya MANN Quality Assuanc and Rliability Tchnion- Isal Institut of

More information

ON A GENERALIZED PROBABILITY DISTRIBUTION IN ASSOCIATION WITH ALEPH ( ) - FUNCTION

ON A GENERALIZED PROBABILITY DISTRIBUTION IN ASSOCIATION WITH ALEPH ( ) - FUNCTION Intnational Jounal of Engining, Scinc and athmatic Vol. 8, Iu, Januay 8, ISSN: 3-94 Impact Facto: 6.765 Jounal Hompag: http://www.ijm.co.in, Email: ijmj@gmail.com Doubl-Blind P Riwd Rfd Opn Acc Intnational

More information

Study on the Static Load Capacity and Synthetic Vector Direct Torque Control of Brushless Doubly Fed Machines

Study on the Static Load Capacity and Synthetic Vector Direct Torque Control of Brushless Doubly Fed Machines ngis Aticl Study on Static Load Capacity Syntic cto Dict Toqu Contol Bushlss Doubly Fd Machins Chaoying Xia * Xiaoxin Hou School Elctical Engining Automation, Tianjin Univsity, No. 9 Wijin Road, Tianjin,

More information

School of Electrical Engineering. Lecture 2: Wire Antennas

School of Electrical Engineering. Lecture 2: Wire Antennas School of lctical ngining Lctu : Wi Antnnas Wi antnna It is an antnna which mak us of mtallic wis to poduc a adiation. KT School of lctical ngining www..kth.s Dipol λ/ Th most common adiato: λ Dipol 3λ/

More information

Shor s Algorithm. Motivation. Why build a classical computer? Why build a quantum computer? Quantum Algorithms. Overview. Shor s factoring algorithm

Shor s Algorithm. Motivation. Why build a classical computer? Why build a quantum computer? Quantum Algorithms. Overview. Shor s factoring algorithm Motivation Sho s Algoith It appas that th univs in which w liv is govnd by quantu chanics Quantu infoation thoy givs us a nw avnu to study & tst quantu chanics Why do w want to build a quantu coput? Pt

More information

3rd WSEAS International Conference on APPLIED and THEORETICAL MECHANICS, Spain, December 14-16,

3rd WSEAS International Conference on APPLIED and THEORETICAL MECHANICS, Spain, December 14-16, 3d WSEAS Intnational Confnc on APPLIED HEOEICAL MECHANICS, Spain, Dcmb 4-6, 007 39 Hybid Modl fo Stuctual liability With Impci Pobabilitic Chaactitic Lihong Ma, Zhiping Qiu, Xiaojun Wang Intitut of Solid

More information

Above Flux Estimation Issues in Induction Generators with Application at Energy Conversion Systems

Above Flux Estimation Issues in Induction Generators with Application at Energy Conversion Systems Acta Polytechnica Hungaica Vol. 3, No. 3, 2006 Above Flux Etimation Iue in Induction Geneato with Application at Enegy Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of

More information

EE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10.

EE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10. Appid M Fa 6, Nuuth Lctu # V //6 43 Advancd ctomagntic Thoy Lc # Scatting and Diffaction Scatting Fom Sma Obcts Scatting by Sma Dictic and Mtaic Sphs Coction of Scatts Sphica Wav xpansions Scaa Vcto Rading:

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLMNTARY INFORMATION. Dtmin th gat inducd bgap cai concntation. Th fild inducd bgap cai concntation in bilay gaphn a indpndntly vaid by contolling th both th top bottom displacmnt lctical filds D t

More information

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

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

More information

User s Guide. Electronic Crossover Network. XM66 Variable Frequency. XM9 24 db/octave. XM16 48 db/octave. XM44 24/48 db/octave. XM26 24 db/octave Tube

User s Guide. Electronic Crossover Network. XM66 Variable Frequency. XM9 24 db/octave. XM16 48 db/octave. XM44 24/48 db/octave. XM26 24 db/octave Tube U Guid Elctnic Cv Ntwk XM66 Vaiabl Fquncy XM9 24 db/ctav XM16 48 db/ctav XM44 24/48 db/ctav XM26 24 db/ctav Tub XM46 24 db/ctav Paiv Lin Lvl XM126 24 db/ctav Tub Machand Elctnic Inc. Rcht, NY (585) 423

More information

Simulink Model of Direct Torque Control of Induction Machine

Simulink Model of Direct Torque Control of Induction Machine Ameican Jounal of Applied Science 5 (8): 1083-1090, 2008 ISSN 1546-9239 2008 Science Publication Simulink Model of Diect Toque Contol of Induction Machine H.F. Abdul Wahab and H. Sanui Faculty of Engineeing,

More information

Last Lecture Summary ADALINE

Last Lecture Summary ADALINE Lat Lctu Summa ADALIN Analtical Solution Gadint Bad Laning Batch Laning Incmntal Laning Laning Rat Adatation Statitical Inttation Aland Bnadino al@i.it.utl.t Machin Laning 9/ ADALIN N l l l T Aland Bnadino

More information

A Comparative Study and Analysis of an Optimized Control Strategy for the Toyota Hybrid System

A Comparative Study and Analysis of an Optimized Control Strategy for the Toyota Hybrid System Pag 563 Wol Elctic Vhicl Jounal Vol. 3 - ISSN 3-6653 - 9 AVERE EVS4 Stavang, Noway, May 13-16, 9 A Compaativ Stuy an Analysis of an Optimiz Contol Statgy fo th Toyota Hybi Systm Tho Hofman 1, Thijs Punot

More information

Lecture 3.2: Cosets. Matthew Macauley. Department of Mathematical Sciences Clemson University

Lecture 3.2: Cosets. Matthew Macauley. Department of Mathematical Sciences Clemson University Lctu 3.2: Costs Matthw Macauly Dpatmnt o Mathmatical Scincs Clmson Univsity http://www.math.clmson.du/~macaul/ Math 4120, Modn Algba M. Macauly (Clmson) Lctu 3.2: Costs Math 4120, Modn Algba 1 / 11 Ovviw

More information

GRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6

GRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6 GVITTION 1. Two satllits and o ound a plant P in cicula obits havin adii 4 and spctivly. If th spd of th satllit is V, th spd of th satllit will b 1 V 6 V 4V V. Th scap vlocity on th sufac of th ath is

More information

J. Electrical Systems 12-4 (2016): Regular paper. Optimal Contribution of Energy Management of Electric Vehicles

J. Electrical Systems 12-4 (2016): Regular paper. Optimal Contribution of Energy Management of Electric Vehicles Inaf YAHIA,*, hoki Bn SALAH, Mohamd Faouzi MIMOUNI J. Elctical Sytm -4 6: 66-67 gula pap Optimal ontibution of Engy Managmnt of Elctic hicl JES Jounal of Elctical Sytm An Elctical hicl E ha th advantag

More information

Chapter 10 Time-Domain Analysis and Design of Control Systems

Chapter 10 Time-Domain Analysis and Design of Control Systems ME 43 Sytm Dynamic & Control Sction 0-5: Stady Stat Error and Sytm Typ Chaptr 0 Tim-Domain Analyi and Dign of Control Sytm 0.5 STEADY STATE ERRORS AND SYSTEM TYPES A. Bazoun Stady-tat rror contitut an

More information

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble Quantum Statistics fo Idal Gas and Black Body Radiation Physics 436 Lctu #0 Th Canonical Ensmbl Ei Q Q N V p i 1 Q E i i Bos-Einstin Statistics Paticls with intg valu of spin... qi... q j...... q j...

More information

CDS 110b: Lecture 8-1 Robust Stability

CDS 110b: Lecture 8-1 Robust Stability DS 0b: Lct 8- Robst Stabilit Richad M. Ma 3 Fba 006 Goals: Dscib mthods fo psnting nmodld dnamics Div conditions fo obst stabilit Rading: DFT, Sctions 4.-4.3 3 Fb 06 R. M. Ma, altch Gam lan: Robst fomanc

More information

Midterm Exam. CS/ECE 181B Intro to Computer Vision. February 13, :30-4:45pm

Midterm Exam. CS/ECE 181B Intro to Computer Vision. February 13, :30-4:45pm Nam: Midtm am CS/C 8B Into to Comput Vision Fbua, 7 :-4:45pm las spa ouslvs to th dg possibl so that studnts a vnl distibutd thoughout th oom. his is a losd-boo tst. h a also a fw pags of quations, t.

More information

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals Hydogn atom Engy lvls and wav functions Obital momntum, lcton spin and nucla spin Fin and hypfin intaction Hydogn obitals Hydogn atom A finmnt of th Rydbg constant: R ~ 109 737.3156841 cm -1 A hydogn mas

More information

EE8412 Advanced AC Drive Systems. Topic 6 Field Oriented control (FOC)

EE8412 Advanced AC Drive Systems. Topic 6 Field Oriented control (FOC) Advanced AC Dive Syte Topic 6 Field Oiented contol (FOC) Souce: ABB 1 Advanced AC Dive Syte Field Oiented Contol (FOC) ectue Topi Geneal Block Diaga of FOC Diect Field Oiented Contol Diect FOC with Cuent

More information

(( )( )) = = S p S p = S p p m ( )

(( )( )) = = S p S p = S p p m ( ) 36 Chapt 3. Rnoalization Toolit Poof of th oiginal Wad idntity o w nd O p Σ i β = idβ γ is p γ d p p π π π p p S p = id i d = id i S p S p d π β γ γ γ i β i β β γ γ β γ γ γ p = id is p is p d = Λ p, p.

More information

CDS 101: Lecture 7.1 Loop Analysis of Feedback Systems

CDS 101: Lecture 7.1 Loop Analysis of Feedback Systems CDS : Lct 7. Loop Analsis of Fback Sstms Richa M. Ma Goals: Show how to compt clos loop stabilit fom opn loop poptis Dscib th Nqist stabilit cition fo stabilit of fback sstms Dfin gain an phas magin an

More information

CBSE-XII-2013 EXAMINATION (MATHEMATICS) The value of determinant of skew symmetric matrix of odd order is always equal to zero.

CBSE-XII-2013 EXAMINATION (MATHEMATICS) The value of determinant of skew symmetric matrix of odd order is always equal to zero. CBSE-XII- EXAMINATION (MATHEMATICS) Cod : 6/ Gnal Instuctions : (i) All qustions a compulso. (ii) Th qustion pap consists of 9 qustions dividd into th sctions A, B and C. Sction A compiss of qustions of

More information

Loss factor for a clamped edge circular plate subjected to an eccentric loading

Loss factor for a clamped edge circular plate subjected to an eccentric loading ndian ounal of Engining & Matials Scincs Vol., Apil 4, pp. 79-84 Loss facto fo a clapd dg cicula plat subjctd to an ccntic loading M K Gupta a & S P Niga b a Mchanical Engining Dpatnt, National nstitut

More information

Electron spin resonance

Electron spin resonance Elcton sonanc 00 Rlatd topics Zman ffct, ngy quantum, quantum numb, sonanc, g-facto, Landé facto. Pincipl With lcton sonanc (ESR) spctoscopy compounds having unpaid lctons can b studid. Th physical backgound

More information

Overview. 1 Recall: continuous-time Markov chains. 2 Transient distribution. 3 Uniformization. 4 Strong and weak bisimulation

Overview. 1 Recall: continuous-time Markov chains. 2 Transient distribution. 3 Uniformization. 4 Strong and weak bisimulation Rcall: continuous-tim Makov chains Modling and Vification of Pobabilistic Systms Joost-Pit Katon Lhstuhl fü Infomatik 2 Softwa Modling and Vification Goup http://movs.wth-aachn.d/taching/ws-89/movp8/ Dcmb

More information

The Research on the Characteristics of Micro-fabrication Platform Control System

The Research on the Characteristics of Micro-fabrication Platform Control System Sno & Tanduc 4 b IFSA Publihing S. L. http://www.nopotal.com Th Rach on th Chaactitic of Mico-fabication Platfom Contol Stm upng Liu Donghng Zhang 3 iaohong Hao Zhonghan Poltchnic No. 5 Boai No. 7 Road

More information

SENSORLESS SPEED CONTROL SYSTEMS BASED ON ADAPTIVE OBSERVERS LUENBERGER AND GOPINATH

SENSORLESS SPEED CONTROL SYSTEMS BASED ON ADAPTIVE OBSERVERS LUENBERGER AND GOPINATH Annal of the Univeity of Caiova, Electical Engineeing eie, No. 32, 2008; ISSN 1842-4805 SENSORLESS SPEED CONTROL SYSTEMS BASED ON ADAPTIVE OBSERVERS LUENBERGER AND GOPINATH Maiu-Auelian PICIU, Lauenţiu

More information

Brushless Doubly-Fed Induction Machines: Torque Ripple

Brushless Doubly-Fed Induction Machines: Torque Ripple Bushlss Doubly-Fd Induction Machins: Toqu Rippl Tim. D. Stous, Xuzhou Wang, Hn Polind, Snio Mmb, IEEE, and J. A. (Bam Fia, Fllow, IEEE Abstact-- Th Bushlss DFIM without its bush-ga and slip-ings loos pomising

More information

Swarm Intelligence Based Controller for Electric Machines and Hybrid Electric Vehicles Applications

Swarm Intelligence Based Controller for Electric Machines and Hybrid Electric Vehicles Applications Swam Intllignc Basd Contoll fo Elctic Machins and Hybid Elctic Vhicls Applications Oma Hgazy 1, Am Amin, and Joi Van Milo 1 1 Faculty of Engining Scincs Dpatmnt of ETEC- Vij Univsitit Bussl, Pow and Elctical

More information

Monte Carlo Simulation of an Optical Differential Phase-Shift Keying Communication System with Direct Detection Impaired by In-Band Crosstalk

Monte Carlo Simulation of an Optical Differential Phase-Shift Keying Communication System with Direct Detection Impaired by In-Band Crosstalk SIMUL 2012 : Th Fouth Intnational Confnc on Advancs in Systm Simulation Mont Calo Simulation of an Optical Diffntial Phas-Shift Kying Communication Systm with Dict Dtction Impaid y In-Band Cosstalk Gnádio

More information

Information Gain Ratio meets Maximal Marginal Relevance A method of Summarization for Multiple Documents

Information Gain Ratio meets Maximal Marginal Relevance A method of Summarization for Multiple Documents Pocding of th Thid NTCIR Wokhop Infomation Gain Ratio mt Maximal Maginal Rlvanc A mthod of Summaization fo Multipl Documnt Tatunoi MORI and Takuo SASAKI Gaduat School of Envionmnt and Infomation Scinc,

More information

Study on the Classification and Stability of Industry-University- Research Symbiosis Phenomenon: Based on the Logistic Model

Study on the Classification and Stability of Industry-University- Research Symbiosis Phenomenon: Based on the Logistic Model Jounal of Emging Tnds in Economics and Managmnt Scincs (JETEMS 3 (1: 116-1 Scholalink sach Institut Jounals, 1 (ISS: 141-74 Jounal jtms.scholalinksach.og of Emging Tnds Economics and Managmnt Scincs (JETEMS

More information

H 2+ : A Model System for Understanding Chemical Bonds

H 2+ : A Model System for Understanding Chemical Bonds : Modl Sytm fo Undtanding Chmical ond a - b R Th fit iu w hav to dal with i th multipl nucli; now w can hav nucla vibation and otation fo th fit tim. Impotant digion: on-oppnhim appoximation. V NN E l

More information

International Journal on Recent and Innovation Trends in Computing and Communication ISSN: Volume: 2 Issue:

International Journal on Recent and Innovation Trends in Computing and Communication ISSN: Volume: 2 Issue: Intnational Jounal on Rnt and Innovation Tnds in Computing and Communiation ISSN: 2321-8169 Volum: 2 Issu: 6 1554 1559 Modl Rfn Adaptiv Systm (MRAS) Basd Spd Snsolss Vto Contol of Indution Moto Div P N

More information

University of Toledo REU Program Summer 2002

University of Toledo REU Program Summer 2002 Univiy of Toldo REU Pogam Summ 2002 Th Effc of Shadowing in 2-D Polycyallin Gowh Jff Du Advio: D. Jacqu Ama Dpamn of Phyic, Univiy of Toldo, Toldo, Ohio Abac Th ffc of hadowing in 2-D hin film gowh w udid

More information

Instruction Execution

Instruction Execution MIPS Piplining Cpt280 D Cuti Nlon Intuction Excution C intuction: x = a + b; Ambly intuction: a a,b,x Stp 1: Stp 2: Stp 3: Stp : Stp 5: Stp 6: Ftch th intuction Dtmin it i an a intuction Ftch th ata a

More information

Simulation Of Induction Motor Modelling In MATLAB Software.

Simulation Of Induction Motor Modelling In MATLAB Software. Intrnational Journal of Enginring Rarch & Tchnology (IJERT) ol. 2 Iu 4, April - 203 Simulation Of Induction Motor Modlling In MATLAB Softwar. Naintara Wanik Dpartmnt of Elctrical Enginring,Shri Ramdobaba

More information

An Elementary Approach to a Model Problem of Lagerstrom

An Elementary Approach to a Model Problem of Lagerstrom An Elmntay Appoach to a Modl Poblm of Lagstom S. P. Hastings and J. B. McLod Mach 7, 8 Abstact Th quation studid is u + n u + u u = ; with bounday conditions u () = ; u () =. This modl quation has bn studid

More information

Neural Networks The ADALINE

Neural Networks The ADALINE Lat Lctu Summay Intouction to ua to Bioogica uon Atificia uon McCuoch an itt LU Ronbatt cton Aan Bnaino, a@i.it.ut.t Machin Laning, 9/ ua to h ADALI M A C H I L A R I G 9 / cton Limitation cton aning u

More information

(1) Then we could wave our hands over this and it would become:

(1) Then we could wave our hands over this and it would become: MAT* K285 Spring 28 Anthony Bnoit 4/17/28 Wk 12: Laplac Tranform Rading: Kohlr & Johnon, Chaptr 5 to p. 35 HW: 5.1: 3, 7, 1*, 19 5.2: 1, 5*, 13*, 19, 45* 5.3: 1, 11*, 19 * Pla writ-up th problm natly and

More information

THE ALIGNMENT OF A SPHERICAL NEAR-FIELD ROTATOR USING ELECTRICAL MEASUREMENTS

THE ALIGNMENT OF A SPHERICAL NEAR-FIELD ROTATOR USING ELECTRICAL MEASUREMENTS THE ALIGNMENT OF A SPHERICAL NEAR-FIELD ROTATOR USING ELECTRICAL MEASUREMENTS ABSTRACT Th mchanical rotator mut b corrctly alignd and th prob placd in th propr location whn prforming phrical nar-fild maurmnt.

More information

Solid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch

Solid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch Solid stat physics Lctu 3: chmical bonding Pof. D. U. Pitsch Elcton chag dnsity distibution fom -ay diffaction data F kp ik dk h k l i Fi H p H; H hkl V a h k l Elctonic chag dnsity of silicon Valnc chag

More information

The angle between L and the z-axis is found from

The angle between L and the z-axis is found from Poblm 6 This is not a ifficult poblm but it is a al pain to tansf it fom pap into Mathca I won't giv it to you on th quiz, but know how to o it fo th xam Poblm 6 S Figu 6 Th magnitu of L is L an th z-componnt

More information

Modeling of a Dielectric Barrier Discharge Lamp for UV Production

Modeling of a Dielectric Barrier Discharge Lamp for UV Production Excpt fom th Pocding of th COMSOL Confnc 28 Hannov Modling of a Dilctic Bai Dichag Lamp fo UV Poduction S Bhol* 1, R Diz 1, H Piqut 1, D L Thanh 1, B Rahmani 1, D Buo 1 1 Univité d Toulou - LAPLACE UMR5213-3162

More information

Direct Torque Control of Double Feed Induction Machine (DTC-DFIM)

Direct Torque Control of Double Feed Induction Machine (DTC-DFIM) Jounal of Advanced Reeach in Science and echnology ISSN: 232-9989 Diect oque Contol of Double Feed Induction Machine (DC-DFIM) Zemmit Abdeahim, Sadouni Radhwane 2 and Meoufel Abdelkade 2 Electical Engineeing

More information

Engineering Differential Equations Practice Final Exam Solutions Fall 2011

Engineering Differential Equations Practice Final Exam Solutions Fall 2011 9.6 Enginring Diffrntial Equation Practic Final Exam Solution Fall 0 Problm. (0 pt.) Solv th following initial valu problm: x y = xy, y() = 4. Thi i a linar d.. bcau y and y appar only to th firt powr.

More information

Sliding mode flux observer with online rotor parameter estimation for induction motors

Sliding mode flux observer with online rotor parameter estimation for induction motors Sliding mod flux obsv with onlin oto aamt stimation fo induction motos Amuliu Bogdan Poca, Mmb, IEEE and Ali Kyhani, Fllow, IEEE Abstact-- Fild ointation tchniqus without flux masumnts dnd on th aamts

More information