Monitoring and diagnostic methods for eccentricity faults in the induction motor

Size: px
Start display at page:

Download "Monitoring and diagnostic methods for eccentricity faults in the induction motor"

Transcription

1 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, Skikda Univity, **Dpatmnt of Elctical, Annaba Univity, ***aboatoy of GREAH E Hav Univity, dimiti.lfbv@univ-hav Abtact Thi wok concn th monitoing and diagnoi of ccnticity fault in induction moto. Th ucc of th typ of lctic moto i mainly du to it implicity of contuction, mchanical obutn, and low cot of manufactuing. Thfo, it i fquntly ud in indutial application. Th ngin a ubjctd duing opation to diffnt kind of containt (thmal, lctical, magntic, mchanical and nvionmntal. Th accumulation of th containt lad to dfct in diffnt pat of th ngin, which ult in lot poduction and cotly pai. Th monitoing and diagnoi of fault hav bcom majo nciti to dtct failu of lctic moto. In thi pap, w dvlop an appoach fo th dtction and diagnoi of fault ccnticiti in induction moto. To thi nd, w build modl fo ach mod of ngin opation (nomal opation and faulty bhavio. W dtct on lin th fault with th analyi of idual obtaind fom th fnc modl. W diagno th fault by th analyi of idual obtaind fom faulty modl. Kywod Monitoing, diagnoi, fault dtction, induction moto, idual. I. INTRODUCTION (HEADING Th occunc of fault in induction moto ult in pai cot and lot poduction []. To afguad th intt of th compani and nu th afty of pon and quipmnt, it i ntial to dvlop monitoing and diagnoi faciliti. Sval mthod xit [], [3] and [7]. Th choic of th mthod i linkd to th knowldg that you wih to acqui about th ytm, but alo to th xpctd complxity. In ou tudy, w popo a mthod bad on th analyi of idual fom fnc (i.. fault f and faulty modl. Thi mthod ha two tp: - Onlin fault dtction ; - Offlin fault diagnoi. Th pincipl of thi mthod i illutatd by th following chm: u(t Machin Rfnc Modl Figu. On lin dtction Th figu pnt th pincipl of fault dtction by uing th o ulting fom th compaion of th modl output with th actual maumnt on ngin. Th cond tp i th diagnoi of th fault bad on th compaion of th maumnt codd at th fit tp with th xpctd valu timatd with th faulty modl. Collctd Input Squnc (t Faulty modl ( u Faulty Modl y ( 3 (3 Collctd Output Squnc y(t Faulty Modl (n Fig.. Offlin diagnoi y Ridual ( t - y ( t y n (t - n 3 5

2 Pocding of th Intnational Confnc on Cicuit, Sytm, Signal II. REFERENCE MODE DESIGN Th fnc modl i bad on an appoximation of magntically coupld cicuit wh th cunt in ach mh of th oto cag i an indpndnt vaiabl [], [9]. In th following quation X tand fo a vaiabl of tato and X fo a vaiabl of oto. Th modl ud in imulation i pntd by quation (: d [ v, ] = [ R, ][ I, ] [ Ψ, ] ( dt Th quation of th cunt flow i pntd by (: [, (,(,(,(,( Ψ ] = [ ][ I ] [ ][ I ] ( Th vcto of voltag and cunt in th tato and oto a: T T [ v ] = [ va, vb, vc] ; I ] [ ia, ib, ic ] [ ] = [...] [ I ] [ i, i, i",... in, i b [ = (3 v ; = ] ( Th dimnion of tato cunt i x3 and th oto cunt i of dimnion x(n b. Th tato paamt copond to th matic R and of dimnion 3x3: R [ R ] = a R a R a aa ab ac [ = ] ba bb bc ( ca cb cc (5 ( Rb R Rb Rb Rb ( Rb R Rb [ R ] = ( Rb R Rb Rb Rb ( Rb R R ( R NbR p ( b ( b... ( N b b ( b p ( b... Nb [ = ] ( N b N... p ( b b b... N b (9 with; b : th lakag inductanc of a oto ba, : th lakag inductanc of a potion of a ing hot-cicuit, p = jj : th inductanc of th oto mh j. ij : th mutual inductanc btwn th i th and j th oto mh with i j. III. FAUT ECCENTRICITIES Th ccnticity of th moto i dfind a an aymmty in th ai gap btwn th tato and oto. Th ccnticity i dividd into two catgoi: tatic ccnticity and dynamic ccnticity. Th tatic ccnticity i chaactizd by th fact th cnt of th oto i not qual to th tato cnt [] []. Th dynamic ccnticity i chaactizd by th fact th cntal ngin tun aound th cnt of th tato. Th figu 3, ow th pincipl of both ccnticity. with ii = p f, ii, i th inductanc of th i th pha and ij i th tato mutual inductanc btwn th i th and j th pha (i j. Th inductanc btwn th tato pha and th oto mh i pntd by th matix of dimnion 3x(N b : [ ] = a b c a b c an b bn b cn b with ij th mutual inductanc btwn th tato pha i (i=a, b and c and ing hotd. Th matic of th oto itanc and inductanc a of dimnion [(N b x(n b ], thy a pntd by quation ( and (9. a b c (7 Fig.3. Static and dynamic ccnticiti t tand fo th dimnion of th gap. Th pnc of ai gap ccnticity i modld by quation (: ( θ, θ =.co( θ a.co( θ θ a ( with th iz of th gap in th abnc of fault, a =. i th paamt of tatic ccnticity, a = d. i th amount of dynamic ccnticity, and d a pctivly th od of

3 Pocding of th Intnational Confnc on Cicuit, Sytm, Signal tatic and dynamic ccnticity, θ i th angula poition in a coodinat ytm latd to th tato, θ i th angula poition of oto lativ to tato [], [], -Ca of tatic ccnticity a =, th xpion ( bcom: ( θ a co( θ = ( Ca of dynamic ccnticity a =, th xpion ( bcom: ( θ, θ.co( θ θ = a ( 3-Ca of mixd ccnticity a and a TIME [] Fig.. Stato cunt (A in function of tim ( fo halthy bhavio In th pnc of ccnticity fault, th gap function changd a th induction: - - ii ( θ = µ ax / π ax / moy F ( θ, P ( θ, Bi ( θ, ( θ, θ, z dθ. dz (3 Th mutual inductanc btwn winding i and j, i pntd by: TIME [] Fig.5. Stato cunt (A in function of tim ( fo tatic ccnticity bhavio ij ( θ = µ ax / π Bi ax / moy F ( θ, F ( θ, P ( θ, ( θ, ( θ, θ, z dθ. dz Bj ( F BJ with, ( θ, θ, z : th MMF of th winding j, P( θ, θ, z : th pmanc of th aigap, moy ( θ, θ, z : th man adiu of th ai-gap. IV. RESUTS AND ANAYSIS IV.. OVERVIEW OF SIMUATION In thi aticl th bhavio of th ngin i imulatd including a Gauian maumnt noi of zo man valu and amplitud.. Th figu to 7 how th cunt pha of th tato induction moto in diffnt opation mod. Figu dpict th pha A fo th halthy ngin. Figu 5 dpict th am cunt with a tatic ccnticity fault imulatd aft th intant.5 cond. Figu tand fo a dynamic ccnticity fault imulatd aft cond. Finally, figu 7 dpict th cunt fo a mixd ccnticity fault imulatd aft.5 cond TIME [] Fig.. Stato cunt (A in function of tim ( fo dynamic ccnticity fault TIME [] Fig.7. Stato cunt (A in function of tim ( fo mixd ccnticity fault IV.. DETECTION OF FAUTS Thi tag concn th on-lin dtction of fault, bad on th analyi of idual (t obtaind by compaion of maumnt and timat ulting fom th modl halthy. 7

4 Pocding of th Intnational Confnc on Cicuit, Sytm, Signal t t y ( (5 ( t y(t i th cunt maumnt at tim t and y (t i th timatd cunt uing th modl halthy at th am tim Ridu With mixd Fault. Ridu With Noic TIME [] x Fig.. Ridual (A in function of tim ( obtaind fo a mixd ccnticity fault TIME [] x Fig.. Ridual (A in function of tim ( obtaind with halthy bhavio Ridu With Static Fault TIME [] x Fig.9. Ridual (A in function of tim ( obtaind fo a tatic ccnticity fault... Ridu With Dynamic Fault Th analyi of idual i obtaind by compaing th idual valu with a thhold. Such an analyi i fficint to dtct th fault and alo to timat with a good accuacy th tim of failu. Indd, bfo th fault occud, th idual a aound zo with mall vaiation du to noi maumnt. In th ca of tatic o mixd fault th amplitud of idual inca ignificantly in compaion with th maumnt noi. Fo dynamic fault, th dtction and timation of t d can b obtaind uing a quntial algoithm fo chang dtction (maximum liklihood o cumulativ um. Th timatd tim of failu a: t d (tatic fault =.5. t d (dynamic fault =.. t d (mixd fault =.5. IV.3. DIAGNOSIS OF FAUTS Th diagnoi i pfomd offlin, bad on th analyi of idual, 3 and fom th compaion of maumnt and timat obtaind with th th faulty modl (tatic, dynamic and mixd ccnticiti ( t t f ( y ( t, y ( t t f ( y ( t, y ( t, td 3 ( t t f ( y ( t, y 3 ( t, td ( t, td ( TIME [] x Fig.. Ridual (A in function of tim ( obtaind fo a dynamic ccnticity fault y (t i th timatd cunt uing th faulty modl with tatic ccnticity fault, y 3 (t i th timatd cunt uing th faulty modl with dynamic ccnticity fault and y (t i th timatd cunt uing th faulty modl with th mixd ccnticity fault. Th function f(.; i a witching function uch that f(t=y (t fo t<td and f(t=f i (t, i=,, fo t t d. IV.3.. CASE OF STATIC ECCENTRICITY t conid th ca of a tatic ccnticity fault that occu at tim t =.5. Thi fault i dtctd accoding to (t (figu 9 and th dtction tim i.5. Th idual ud fo

5 Pocding of th Intnational Confnc on Cicuit, Sytm, Signal diagnoi a dpictd in figu to. Th idual (t i aound wha th idual 3 (t and (t inca ignificantly aft t = TIME [] Fig. 5. Ridual (A in function of tim ( obtaind fo a dynamic ccnticity fault TIME []. Fig.. Ridual (A in function of tim ( obtaind fo a tatic ccnticity fault TIME [] Fig.. Ridual 3 (A in function of tim ( obtaind fo a dynamic ccnticity fault TIME [].3 Fig. 3. Ridual 3 (A in function of tim ( obtaind fo a tatic ccnticity fault TIME [] Fig. 7. Ridual (A in function of tim ( obtaind fo a dynamic ccnticity fault TIME [] Fig.. Ridual (A in function of tim ( obtaind fo a tatic ccnticity fault IV.3.. CASE DYNAMIC OF ECCENTRICITY t conid th ca of a dynamic ccnticity fault that occu at tim t =. Thi fault i dtctd accoding to (t (figu and th dtction tim i.. Th idual ud fo diagnoi a dpictd in figu 5 to 7. IV.3.. CASE MIXED OF ECCENTRICITY t conid th ca of a mixd ccnticity fault that occu at tim t =.5. Thi fault i dtctd accoding to (t (figu and th dtction tim i.5. Th idual ud fo diagnoi a dpictd in figu to. 9

6 Pocding of th Intnational Confnc on Cicuit, Sytm, Signal TIME [] Fig.. Ridual (A in function of tim ( obtaind fo a mixd ccnticity fault S ftatic fdynamic fmixtd = 3 VI. CONCUSION (7 In thi pap, w applid a mthod fo dtcting and diagnoing ccnticity fault in th induction moto. Th idual obtaind fom th halthy modl lad to th dtction of fault and to th timation of th tim of failu. Th idual obtaind fom th faulty modl lad to th diagnoi of fault typ. Th ult obtaind a atifactoy fo th onlin dtction and offlin diagnoi of fault whn th fault a uncolatd and thi magnitud a ignificantly lag TIME [] Fig. 9. Ridual 3 (A in function of tim ( obtaind fo a mixd ccnticity fault Numb of ba oto: q =, VII. MOTOR PARAMETERS Stato itanc: R =9. Ω, Ba itanc: R =* - Ω, Ba inductanc: Ring itanc: b =.* - H, cb R =3.79* Ω, Ring inductanc: c =* -9 H, Numb of pol.p=, Intia momnt: J =.5, Fquncy: t f =5 Hz Roto diamt: R =.55.7* -3 m, Pmability: µ =*π * -7, Inductanc lo: f =.H Magnitud of noi: b =.; Numical incmnt: h = REFERENCES TIME [] Fig.. Ridual (A in function of tim ( obtaind fo a mixd ccnticity fault V. ANAYSIS OF THE RESIDUAS Fom th idual dpictd on figu to, it i poibl to idntify th fault. Th ignatu of ach typ of fault i diffnt and th matix of ignatu can b dtaild fom th obtaind idual (accoding to th u of uitabl thhold: [] M.E.H. Bnbouzid, Bibliogaphy on induction moto fault dtction and diagnoi, IEEE Tanaction on Engy Convion, Vol., N., Dcmb 999. [] W. T. Thomon, A. Badou, On lin cunt monitoing and application of a finit lmnt mthod to pdict th lvl of tatic ai-gap ccnticity in th-pha induction moto, IEEE Tanaction on ngy Convion, Vol. 3, N., pp , Dcmb 99. [3] T.M. ayadi,. Abd, N. Khnf, Stuctu nuonal hybid pou l diagnotic d défaut tatoiqu d la machin aynchon, th Intnational Confnc on Comput Intgatd Manufacting CIP 7 [] S. Nandi, M. Bhaadwaj, H. A. Toliyat, Pfomanc analyi of a thpha induction moto und mixd xcnticity condition. IEEE Tanaction on Engy Convion, Vol. 7, N. 3, Sptmb,. [5] [] M. E. H. Bnbouzid, M. Viia, C. Thy, Induction moto' fault dtction and localization uing tato cunt advancd ignal 9

7 Pocding of th Intnational Confnc on Cicuit, Sytm, Signal pocing tchniqu" IEEE Tanaction on Pow Elctonic, Vol., N, pp, 999. [] A. Mtatla, T. Bahi, I. Hadjadj, Diagnoi of mixd ccnticity in aynchonou machin Intnational Rviw on Modlling and Simulation, Vol,, N, Italy,. [7] R. N. Andiamalala, H. Razik,. Baghli, F. M. Sago, Eccnticity fault diagnoi of a dual-tato winding induction machin div coniding th lotting ffct, IEEE tanction on Indutial lctonic, Vol.55, N., Dcmb. [] A. M. Awadallah, M.M. Moco, application of ai toul in fault diagnoi of lctical macin and div-an ovviw, IEEE Tanaction on ngy convion, vol., N., pp 5-5, Jun 3. [9] H. A. Toliyat, T. A. ipo, Tanint analyi of cag induction machin und tato, oto ba and nd ing fault, IEEE Tanaction on Engy Convtiion, Vol,, pp. -7, Jun 995. [] W. T. Thomon, D. Rankin, D.G. Doll, On lon cunt monitoing to diagno aigap ccnticity in lag th-pha induction moto_indutial ca hitoiqu vify th pdiction, IEEE Tanaction on Engy convtion Vol,, N., Dcmb 999. [] S. Nandi, R. M. Bhaadwaj, H. A. Toliyat, Pfomanc analyi of a th-pha induction moto und mixd xcnticity condition, IEEE Tanaction on Engy Convion, Vol. 7, N. 3, pp , Sptmb. 9

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

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

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

(( ) ( ) ( ) ( ) ( 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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

217Plus TM Integrated Circuit Failure Rate Models

217Plus TM Integrated Circuit Failure Rate Models T h I AC 27Plu s T M i n t g at d c i c u i t a n d i n d u c to Fa i lu at M o d l s David Nicholls, IAC (Quantion Solutions Incoatd) In a pvious issu o th IAC Jounal [nc ], w povidd a highlvl intoduction

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

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

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

Physics 202, Lecture 5. Today s Topics. Announcements: Homework #3 on WebAssign by tonight Due (with Homework #2) on 9/24, 10 PM

Physics 202, Lecture 5. Today s Topics. Announcements: Homework #3 on WebAssign by tonight Due (with Homework #2) on 9/24, 10 PM Physics 0, Lctu 5 Today s Topics nnouncmnts: Homwok #3 on Wbssign by tonight Du (with Homwok #) on 9/4, 10 PM Rviw: (Ch. 5Pat I) Elctic Potntial Engy, Elctic Potntial Elctic Potntial (Ch. 5Pat II) Elctic

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

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

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

(, ) 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

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

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

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

APPENDIX II Electrical Engineering (Archiv fur Elektrotechnik).

APPENDIX II Electrical Engineering (Archiv fur Elektrotechnik). Rintd with mission fom th ublish. APPENDIX II Elctical Engining (Achiv fu Elktotchnik). Publication P2 ISSN: 948-792 (Pint), 432-487 (Onlin) DOI:.7/s22-6-327-5 Th oiginal ublication is availabl at www.singlink.com

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

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

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

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

A Generalized Two Axes Model of a Squirrel-Cage Induction Motor for Rotor Fault Diagnosis

A Generalized Two Axes Model of a Squirrel-Cage Induction Motor for Rotor Fault Diagnosis SEBIAN JOUNAL OF ELECTICAL ENGINEEING Vol. 5, No. 1, ay 2008, 155-170 A Genealized Two Axe odel of a Squiel-Cage Induction oto fo oto Fault Diagnoi Sami Hamdani 1, Oma Touhami 2, achid Ibtiouen 2 Abtact:

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

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

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

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

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

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

Basic Interconnects at High Frequencies (Part 1)

Basic Interconnects at High Frequencies (Part 1) Basic Intcnncts at High Fquncis (Pat ) Outlin Tw-wi cabls and caxial cabls Stiplin Stiplin gmty and fild distibutin Chaactizing stiplins Micstip lin Micstip gmty and fild distibutin Chaactizing micstip

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

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

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

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

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

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

Analysis and Design of Basic Interconnects (Part 1)

Analysis and Design of Basic Interconnects (Part 1) Analysis and Dsign f Basic Intcnncts (Pat ) Outlin Tw-wi lins and caxial lins Stiplin Stiplin gmty and fild distibutin Chaactizing stiplins Micstip lin Micstip gmty and fild distibutin Chaactizing micstip

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

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

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

Altitude measurement using laser beam reflected from water surface

Altitude measurement using laser beam reflected from water surface Altitu maumnt uing la bam flct fom wat ufac Sh. Mohamma Nja an M. H. Haji Miaii Downloa fom ij.iut.ac.i at 3:35 IRDT on Monay Sptmb 7th 08 Abtact: In thi pap altitu maumnt fom wat ufac uing la bam i pnt.

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

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

5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS

5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS 5.61 Fall 2007 Lctu #2 pag 1 Th DEMISE of CLASSICAL PHYSICS (a) Discovy of th Elcton In 1897 J.J. Thomson discovs th lcton and masus ( m ) (and inadvtntly invnts th cathod ay (TV) tub) Faaday (1860 s 1870

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

Q Q N, V, e, Quantum Statistics for Ideal Gas. The Canonical Ensemble 10/12/2009. Physics 4362, Lecture #19. Dr. Peter Kroll

Q Q N, V, e, Quantum Statistics for Ideal Gas. The Canonical Ensemble 10/12/2009. Physics 4362, Lecture #19. Dr. Peter Kroll Quantum Statistics fo Idal Gas Physics 436 Lctu #9 D. Pt Koll Assistant Pofsso Dpatmnt of Chmisty & Biochmisty Univsity of Txas Alington Will psnt a lctu ntitld: Squzing Matt and Pdicting w Compounds:

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

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

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

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

Geometrical Analysis of the Worm-Spiral Wheel Frontal Gear

Geometrical Analysis of the Worm-Spiral Wheel Frontal Gear Gomtical Analysis of th Wom-Spial Whl Fontal Ga SOFIA TOTOLICI, ICOLAE OACEA, VIRGIL TEODOR, GABRIEL FRUMUSAU Manufactuing Scinc and Engining Dpatmnt, Dunaa d Jos Univsity of Galati, Domnasca st., 8000,

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

II. FORMULATION OF THE PROBLEM

II. FORMULATION OF THE PROBLEM Intnational Jounal of Engining Scinc Invntion ISSN (Onlin): 39 6734 ISSN (Pint): 39 676 www.ijsi.og Volum 6 Issu 9 Sptmb 7 PP. - Study of Unstady Magntohydodynamic Flow of n Incompssibl Viscous Elctically

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

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

RESEARCH ON FRESH AGRICULTURAL PRODUCT BASED ON THE RETAILER S OVERCONFIDENCE UNDER OPTIONS AND SPOT MARKETS

RESEARCH ON FRESH AGRICULTURAL PRODUCT BASED ON THE RETAILER S OVERCONFIDENCE UNDER OPTIONS AND SPOT MARKETS Intnational Jounal of Managing Infomation Tchnology (IJMIT Vol.5, No.4, Novmb 23 RESEARCH ON FRESH AGRICULTURAL PRODUCT BASED ON THE RETAILER S OVERCONFIDENCE UNDER OPTIONS AND SPOT MARKETS Kai Ni and

More information

Boise State University Department of Electrical and Computer Engineering ECE470 Electric Machines

Boise State University Department of Electrical and Computer Engineering ECE470 Electric Machines Boie State Univeity Depatment of Electical and Compute Engineeing ECE470 Electic Machine Deivation of the Pe-Phae Steady-State Equivalent Cicuit of a hee-phae Induction Machine Nomenclatue θ: oto haft

More information

Applications of Lagrange Equations

Applications of Lagrange Equations Applcaton of agang Euaton Ca Stuy : Elctc Ccut ng th agang uaton of oton, vlop th athatcal ol fo th ccut hown n Fgu.Sulat th ult by SIMI. Th ccuty paat a: 0.0 H, 0.00 H, 0.00 H, C 0.0 F, C 0. F, 0 Ω, Ω

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

6.Optical and electronic properties of Low

6.Optical and electronic properties of Low 6.Optical and lctonic poptis of Low dinsional atials (I). Concpt of Engy Band. Bonding foation in H Molculs Lina cobination of atoic obital (LCAO) Schoding quation:(- i VionV) E find a,a s.t. E is in a

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

[ ] 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

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

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

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

Fault Eccentricity Diagnosis in Variable Speed Induction Motor Drive Using DWT

Fault Eccentricity Diagnosis in Variable Speed Induction Motor Drive Using DWT AMSE JOURNAS-AMSE ETA publication-7-seie: Advance C; Vol. 7; N 3; pp 8- Submitted Oct. 8, 7; Revied Dec. 6, 7; Accepted Dec. 6, 7 http://doi.og/.88/ama_c.73 Fault Eccenticity Diagnoi in Vaiable Speed nduction

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

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

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD II.3. DETEMINTION OF THE ELETON SPEIFI HGE Y MENS OF THE MGNETON METHOD. Wok pupos Th wok pupos is to dtin th atio btwn th absolut alu of th lcton chag and its ass, /, using a dic calld agnton. In this

More information

CHAPTER 5 CIRCULAR MOTION

CHAPTER 5 CIRCULAR MOTION CHAPTER 5 CIRCULAR MOTION and GRAVITATION 5.1 CENTRIPETAL FORCE It is known that if a paticl mos with constant spd in a cicula path of adius, it acquis a cntiptal acclation du to th chang in th diction

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

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

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

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

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

Research on fresh agricultural product based on the retailer s overconfidence under options and spot markets

Research on fresh agricultural product based on the retailer s overconfidence under options and spot markets Rach on fh agicultual poduct bad on th tail ovconfidnc und option and pot makt Kai Ni, School of Economy and Tad, Hunan Univity, Changha 479, Hunan, China d_nikai@63.com Man Yu 2 School of Economy and

More information

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS It is not possibl to find flu through biggr loop dirctly So w will find cofficint of mutual inductanc btwn two loops and thn find th flu through biggr loop Also rmmbr M = M ( ) ( ) EDT- (JEE) SOLUTIONS

More information

[2009] IEEE. Reprinted, with permission, from Xu, Wei; Zhu, Jianguo; Guo, Youguang; Wang, Yi; Zhang, Yongchang; Tan, Longcheng. Equivalent Circuits

[2009] IEEE. Reprinted, with permission, from Xu, Wei; Zhu, Jianguo; Guo, Youguang; Wang, Yi; Zhang, Yongchang; Tan, Longcheng. Equivalent Circuits [009] IEEE. Rpintd, with pmission, fom Xu, Wi; Zhu, Jianguo; Guo, Youguang; Wang, Yi; Zhang, Yongchang; Tan, Longchng. Equivalnt Cicuits fo Singld-sidd Lina Induction Motos', Pocdings of IEEE Engy Convsion

More information

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center Collisionlss Hall-MHD Modling Na a Magntic Null D. J. Stoi J. J. Ramos MIT Plasma Scinc and Fusion Cnt Collisionlss Magntic Rconnction Magntic connction fs to changs in th stuctu of magntic filds, bought

More information

Molecules and electronic, vibrational and rotational structure

Molecules and electronic, vibrational and rotational structure Molculs and ctonic, ational and otational stuctu Max on ob 954 obt Oppnhim Ghad Hzbg ob 97 Lctu ots Stuctu of Matt: toms and Molculs; W. Ubachs Hamiltonian fo a molcul h h H i m M i V i fs to ctons, to

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

Eddy Currents in Permanent Magnets of a Multi-pole Direct Drive Motor

Eddy Currents in Permanent Magnets of a Multi-pole Direct Drive Motor Acta Technica Jauineni Vol. 6. No. 1. 2013 Eddy Cuent in Pemanent Magnet of a Multi-pole Diect Dive Moto G. Gotovac 1, G. Lampic 1, D. Miljavec 2 Elaphe Ltd. 1, Univeity of Ljubljana, Faculty of Electical

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

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

How!do!humans!combine!sounds!into!an! infinite!number!of!utterances? How!do!they!use!these!utterances!!to! communicate!and!express!meaning?

How!do!humans!combine!sounds!into!an! infinite!number!of!utterances? How!do!they!use!these!utterances!!to! communicate!and!express!meaning? Linguistics How!o!humans!combin!s!into!an! H h bi i infinit!numb!of!uttancs? Supcomputing an Linguistics Kis Hyln Univsity of Luvn RU Quantitativ Lxicology an Vaiational Linguistics Linguistics Linguistics

More information

A Heuristic Approach to Detect Feature Interactions in Requirements

A Heuristic Approach to Detect Feature Interactions in Requirements A Huistic Appoach to Dtct Fatu Intactions in Rquimnts Maitta Hisl Janin Souquiès Fakultät fü Infomatik LORIA Univsité Nancy2 Univsität Magdbug B.P. 239 Bâtimnt LORIA D-39016 Magdbug, Gmany F-54506 Vandœuv-ls-Nancy,

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

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