Torque Sensorless IM Control for EV's

Size: px
Start display at page:

Download "Torque Sensorless IM Control for EV's"

Transcription

1 oque Senole IM Contol fo EV' Kael Jezenik, Mian Roič Abtact Inuction moto (IM) pee enole contol, allowing opeation at low an zeo pee, optimizing toque epone an efficiency, i peente in the pape. he magnitue an oientation angle of the oto flux of the inuction moto ae etemine by the output of the cloe-loop oto flux obeve bae on the calculation of the extene electomotive foce (EMF) of machine. he popoe tato flux/toque cheme i obut to paamete vaiation an extenal itubance. he pouce toque i a continuou output vaiable of contol. Hawae-in-the-loop (HIL) poceue, a upplement of the conventional imulation, i a moen appoach to the teting of the opeation of algoithm without the nee fo the pototype. Pat of actual ytem ae eplace by the mathematical moel, which ae numeically calculate on-line an connecte to the actual component of the ytem by the ue of oftwae an hawae inteface. Popoe enole IM contol fo EV' i execute with the ue of the SPACE ytem containing DS113 PPC contolle boa, an the Danfo VL54 Invete. he ytem i pogamme with the ue of MALAB/Simulink. Meauement an computation of algoithm ae execute in µ. he efeence tacking pefomance i emontate by expeiment. he pefomance of the popoe metho i invetigate an veifie expeimentally on SPACE ytem. Keywo: inuction moto, toque, contol ytem, electic ive, hawae in the loop imulation 1 Intouction he numbe of application of vaiable pee an toque ive fo the popelling of the mechanical ytem ha been inceaing apily in lat ecae. Becaue of the gowing complexity of the application a eman fo the impove evelopment an teting equipment ha occue. Alo in many cae the impact of the mechanical loa attache to the ive nee to be tete befoe the actual mechanim i available o fo ome eaon it i not aviable to pefom tet on it. Conequently the ue of api pototyping appoache i gaining the impotance in the eign poce. A api pototyping technique, calle Dynamic emulation of mechanical loa, wa evelope in oe to tet the pefomance of ive in the mechanim. It i an inexpenive ueful ai fo the eign of the vaiable pee an toque contol algoithm. Dynamic emulation of mechanical loa [], [3], [4], [5], oe not equie aitional hawae (when compae to tatic emulation of mechanical loa [6], [7]), howeve uing the impove oftwae algoithm it i ucceful alo in the cae of api pee an toque change. It enable the teting of changing inetia an highly nonlinea ynamic. he toque applie by the Loa Machine i calculate uing the feeback contol algoithm. In thi pape by combining the vaiable tuctue ytem an Lyapunov eign [1] a novel liing moe algoithm of contolle/obeve fo inuction moto i evelope. hi contol metho i bae on etimation of an extene electomotive foce (EMF) an i ue to ue of liing moe pinciple obut againt vaiation of loa toque, machine paamete an extenal itubance. Fo both, contolle an obeve, thee ae ue nonlinea contol pinciple, namely etimate EMF an machine teminal voltage built a nonlinea feefowa contol, liing moe pinciple bae on tate vaiable eo ae ue a

2 feeback to guaantee tability of contol ytem. he popoe metho i invetigate an veifie in hawae in the loop imulation expeimentally. Dynamic Moel of Inuction Moto.1 Machine Dynamic Contol of inuction moto (IM) i till a challenging poblem ue to it nonlinea ynamic, limite poibility to meaue o etimate neceay tate vaiable an peence of the witching convete with it own nonlineaity a a powe moulato in contol loop. he ynamic of IM conit of mechanical motion (4), ynamic of tato electomagnetic ytem (1) an the ynamic of the oto electomagnetic ytem (): i 1 Lm Ψ = u Ri, (1) t σ L L t Ψ Lm R 1 1 = R i + p,, t L I + ω J = = L Ψ I 1 J 1, () Lm e = p Ψ i, (3) 3 L ω 1 = ( e L), (4) t J whee ω i mechanical oto angle pee, the two imenional complex pace vecto a b Ψ = Ψ, Ψ, Ψ, = Ψ a Ψ b, u, = ua u b, i, = ia i b ae tato an oto flux, tato voltage an cuent, epectively, e i moto toque, L i loa toque, J i inetia of the oto an p i the numbe of pole pai. One of the mot impotant iue in implementing iect toque contol (DC) o fiel oiente contol (FOC) tategie fo IM i to obtain eal-time intantaneou flux level an poition with ufficient accuacy fo the entie pee ange, fom almot tantill to high pee level. he ifficulty in flux etimation lie with the non-linea inuction machine moel, which i chaacteie by pee epenent an time vaying paamete. In oe to illutate thi non-linea behaviou of IM contol let u expe the eivation of evelope electical toque of IM fom (3). hi yiel fo toque vaiation: e R R p Lm + + e = ( Ψ u pωψ Ψ), (5) t σl σl 3 σl L whee inicate co pouct an inicate ot pouct. It can be ecognie fom (5), that toque vaiation i the um of two tem. he fit tem epen on the tato (R ) an oto (R ) eitance an euce the abolute value of the toque ( e ). he econ tem epeent the effect of the applie contol voltage vecto ( u ) on the toque an i epenent on the opeating conition of IM. It can be note that ome PWM voltage vecto may caue poitive toque vaiation at low ynamic EMF value an negative toque vaiation at high value of back inuce voltage. he cucial point in contol of IM i to make the electomagnetic toque an the flux of IM inepenently contollable. Similaly to toque vaiation, the oto flux vaiation can be ecibe fom (1) an () a L 1 i Ψ = Ψ u Ri Ψ σl Ψ. (6) t L m Ψ t

3 he vaiation of the oto flux i etemine with the ot pouct between oto flux an applie input voltage vecto an epen motly on tato paamete vaiation R, σ L. Both toque an flux vaiation ae highly nonlinea in applie contol voltage u egaing IM oto flux of machine Ψ. he conventional contol metho of IM i bae in cae of FOC on implification of oto q flux component = = [,] Ψ,Ψ Ψ. he DC metho eplace the IM coupling with hyteei contol. In eal IM contol oto flux in q-axi will not be zeo an FOC metho i ue vaiation of motly paamete, inappopiate in enole ive application. he DC metho i in pinciple pee enole, but ue to ue of voltage tato moel of IM an appoximation of tato eitance R ~ in the flux moel, cuent an toque vaiation by low pee ae lightly highe then in cae of nominal pee [8],[9].. Contol Poceue he eign of liing moe ytem conit geneally of two poceue: eign of the witching uface an eign of the liing moe contolle [1]. he witching uface i eigne to obtain a eign pefomance fo the ytem output vaiable. In VSS contol, the goal i to keep the ytem motion on the manifol S, which i efine S = { y: σ ( y, t) = G y} = ; σ= y y, (7) whee y, y ae tate vaiable of eie an etimate value an σ i contol eo. he "chatteing fee" liing moe contol [11] houl be choen uch that the caniate Lyapunov function atifie the Lyapunov tability citeia. hi can be aue fo V = σ σ/ an V = σ σ (8) if the following inequality can be mae tue V = σ Dσ <, (9) whee D i poitive efinite matix. heefoe (8), (9) atify the Lyapunov conition. Fom (8) an (9) eaching conition ( σ = Dσ) can be got. With the electe Lyapunov function the tability of the whole contol ytem in the cae of the initial conition an paamete mimatch i guaantee. he contol function will atify eaching conition in the following fom 1 u() t = u() t ( GB) ( Dσ+ σ ); t = t +,. (1) In the icetize fom, which will be ue in contol algoithm, the continuou fit eivative of the contol eo can be eplace by it fit back tep appoximation. he contol input then i evaluate a 1 u( k + 1) = C( θ ) u( k) + ( GB) (( I + D) C( θ) σ( k) C ( θ) σ ( k 1) ). (11) Sytem i aymptotically table an theoetically will each the liing manifol S in infinite time, but ε= ( ) -vicinity of the manifol i eache in finite time. he otation matice C( θ), C( θ) ae ue in algoithm fo compenation of computational elay. 3 Popoe VSC oque an Flux Contol Scheme he main pupoe of thi eeach wok i to apply the nonlinea continuou liing moe contol combine with Lyapunov eign appoach to the toque an flux contol of IM to achieve that: the geneate toque become a linea output with epect of contol tate, egulating the oto flux amplitue can inceae the powe efficiency an make it poible to opeate in the flux-weakening egion,

4 employing the nonlinea continuou liing moe contol on the toque an flux poee the obutne to the matche an mimatche uncetaintie. heefoe, the following poblem tatement can be popoe: eign a flux / pee obeve to etimate the flux an pee imultaneouly bae on the meauement of the tato cuent an voltage an then eign a coeponing contolle to guaantee that the eal toque tack the eie one. Specially, bae on the tate equation fo toque (5) an oto flux vaiation (6), a coeponing liing moe toque contolle to guaantee the aymptotic tability of both the liing moe electomotive foce (EMF) flux obeve an the toque tacking contolle, i to be eigne. he aitional goal of contol of IM i to make the flux tack the efeence flux input. In thi eeach, the "phyical" coupling between obeve an contolle i ealize with the common ignal of EMF in nonlinea contol. Fom the above icuion an bae on the tate equation (5) an (6), liing moe uface fo toque an flux can be efine ˆ, ( ˆ σ ) ( ˆ = e e σψ = γ Ψ Ψ + Ψ Ψ ), (1) t whee e, Ψ ae efeence toque an oto flux, γ i a poitive contant paamete which etemine the convegence pee of the flux eo Ψ Ψ ˆ in the liing moe. he eign tak i euce to enfocing liing moe in the manifol σ =, σ =, ψ σ σ in -q plane with contol in tato fixe plane. Equation of the contolle motion pojection on the ubpace σ =, ψ σ σ can be a p L 1 σ, = f + Ψ u σ ψ = fψ + C Ψ u, (13) 3 σl Lm Ψ whee f, f ψ ae continuou tate function. Ieal contol input u eq coul be compute fom σ = an σ ψ = [1]. Howeve, u eq cannot be evaluate by (13), ince it contain unknown eal oto flux an will be eigne in oto flux obeve togethe with EMF. In popoe contol cheme the ieal equivalent contol voltage u eq i eplace with etimate EMF fom obeve ( e ˆ ). On thi way thee i etablihe connection with obeve an contolle a fee fowa contol of IM. he contol input voltage vecto (11) i evaluate a σ L u( k + 1) = C( θ ) ˆ ( ) e k + K (( I + D) C( θ) σ( k) C ( θ) σ( k 1) ), (14) whee σ =, ψ σ σ ae contol toque / flux eo an K = K, K ψ i toque / flux feeback gain. In popoe nonlinea VSC cheme liing moe can occu on manifol σ = an σ ψ =. he etimate toque an the magnitue of the oto flux convege to the efeence value: σ = mean ˆ e = e an σ ψ = mean Ψ ˆ = Ψ, both ten to zeo exponentially. oque / flux eo ( σ, σ ψ ) ae then tanfome fom -q to tato fixe a-b cooinate, whee tato voltage input vecto i compute in (14). σ co ˆ in ˆ a θ θ σ = b in ˆ co ˆ. (15) σ θ θ σ ψ

5 he popoe contol cheme i peente in Figue 1. Figue 1: Popoe contol cheme. Figue : Cloe-loop oto flux obeve. 4 Sliing Moe Flux an Spee Obeve Deign of an IM enole ive i till a challenge. he baic poblem i pee an flux etimation epecially at the low pee ange an une light loa conition. In thi ection the liing moe appoach to oto flux an pee etimation of an IM will be peente (Figue ). he oto flux of IM i in pinciple ecibe in tato efeence fame with voltage moel Ψ L i = u ir σ L (16) t L m t o cuent moel (). he IM tato cuent i 1 Lm i = Ψ Ψ. (17) σ L L Replacing tato cuent in () with (17) the eivative of oto flux will be ecibe with tate vaiable tato an oto flux a Ψ Lm R = Ψ +e, (18) t L σ L whee the electomotive foce EMF tem i expee with R e = I + pωj L Ψ. (19) σ he mot ignificant limitation of the oto flux obeve bae on voltage moel of IM in (16) i that it oe not wok at zeo pee. At zeo pee an low pee the amplitue of the electomotive foce e i too mall to accuately an eliably etemine the oto flux angle neceay fo both fiel oientation an pee etimation. At low pee the flux etimation given by voltage moel eteioate owing to the effect of an inaccuate value of the tato eitance R, which caue a eviation of the oto flux pace vecto lightly. he cuent moel of IM in (18) i neee infomation about pee, o in pee enole contol of IM oto flux an mechanical pee have to be etimate. In thi pape a novel metho have been popoe fo IM enole contol bae on etimation of electomotive foce ˆ e in which moto mechanical pee infomation i inclue (18), (19).

6 In obeve eign uitable fo the enole ive the obeve contol input houl be known function of moto pee o that, afte etablihing liing moe in toque tacking loop, the pee can be etemine a unique olution. hi lea to the following election of the feefowa/feeback tuctue of tato cuent obeve with combination of voltage (16) an cuent (18) moel: ˆ i 1 ˆ Lm ˆ R Lm ˆ = u Ri e + Ψ. () t σl L σl L ˆ ε = i i i etemine a: Etimation eo ( i ) ˆ εi ( i i ) 1 L m ( ˆ Lm Lm ) ( ˆ = = e e R + R ε i + R Ψ Ψ). (1) t t σ L L L L Sliing moe algoithm coul be ue to calculate contol, which ha meaning of EMF ˆ ( ) ˆ σl ( 1) L e k = e k + Ke m (( I + Di) εi( k) ε i( k 1) ). () L he poce of zeoing the cuent eo utilizing toque egulate PWM i the eence of liing moe obeve. Roto flux obeve coul be electe having the tuctue of oto moel (18) with aitional convegence tem ξ ψ an unknown tato flux Ψ will be eplace with eie one ˆ Ψ ˆ ˆ Lm R e = = e + Ψ + ξψ. (3) t L σ L Now flux etimation eo ( ε ˆ ψ = Ψ Ψ ) can be calculate a ε ( ˆ ψ Ψ Ψ) ˆ L m R ( ˆ = = e e + Ψ Ψ) ξ ψ. (4) t t L σl o enue convegence, ξ ψ coul be electe in the following fom ε ˆ i Ψ ξ ˆ ψ = KψI Ψ. (5) ˆ εi Ψ he metho of electing ε ˆ i Ψ an ε ˆ i Ψ i nothing but the conventional appoach to contol eign bae on equation in the fame otating with oto flux [13]. Deign paamete K ψ coul be electe fom (5) o that etimate oto flux ten to it eal value. he iea i to tack the tato cuent component by putting the coeponing cuent eo ( ˆ i i ) into the liing moe, an heeby, to impoe the aymptotic convegence of the flux obevation eo ε ψ epite paametic vaiation ' R R 1 Lm i i t ε + + = σl ε ε σl L t ψ. (6) he tato flux efeence Ψ i calculate fom the oto flux efeence Ψ an the toque efeence a L σ L e Ψ L 3 m plmψ Ψ Ψ = +. (7) Etimate ynchonou pee an the mechanical oto pee will be expee with co pouct ˆ 1 ˆ 1 1 ˆ, ˆ ˆ ˆ ω = Ψ ˆ t Ψ ω = e p Ψ. (8) ˆ Ψ Ψ

7 5 Flux Contol fo Efficiency Impovement Fo electic ive application, wie ange pee contol of moto ive i neceay. When the moto pee i lowe than the bae pee, the moto ive i equie to povie a contant output toque, alo calle contant toque opeation. On the othe han, when the pee i highe than the bae pee, the loa toque eceae with the pee. hu, intea of poviing a contant output toque, contant powe opeation i pefee becaue it can ignificantly euce the cot an ize of the moto ive. he popoe IM ive i a eiable caniate fo uch application becaue the fiel of the IM can be eaily weakene by eucing the oto flux component cuent a the oto pee inceae [14]. he maximum output toque evelope by the machine i epenent on the allowable cuent ating an the maximum voltage that the invete can apply to the machine [15]. heefoe, to ue the invete capacity fully, it i eiable to ue the contol cheme conieing the voltage an cuent limit conition, which can yiel the maximum toque pe ampee ove the entie pee ange. he cuent limit bounay i a cicle whoe aiu epen on only the cuent ating. he IM will opeate at the highet poible oto flux maintaine by the DC link voltage U DC in the entie pee ange. Opeation at the highet flux aue a maximum moto toque at the lowet lip fequency. A the moto loe ae popotional to the lip fequency we may expect the popoe contol metho to yiel a highly efficient electomechanical enegy conveion of the ive. he efficiency of IM ive i impove by ajuting the oto flux level automatically in accoance with the toque comman a hown with (9)-(31). hi will be epecially tue at light loa becaue of ue low flux level. he maximum allowe oto flux will epen on actual tato fequency an c-link voltage U ψ DC max = kv, kv < 1, (9) 3ω an toque epenent optimal oto flux m + L R L R ψ opt = e. (3) 3p R he effective comman will be ue a opt max ψ ψ. (31) 6 Stato Reitance Etimation Dynamic pefomance of the IM contolle tongly epen on moto paamete accuacy. A paamete mimatch pouce an eo in fiel oientation an uneiable coupling between the flux an toque contol. Although it i poible to etemine the moto paamete in avance, ignificant change occu uing the opeation. Among thee paamete epecially the exact knowlege of the tato eitance i an impotant iue. he poblem i peent in the cae of the ue of pee eno, but it i impotance inceae when in enole application. Hee, a new appoach to pee etimation with obut popety to tato eitance vaiation i popoe. Fit, we efine a new quantity q a a co pouct q= i ( u Ri ) = i u. (3) q epeent the intantaneou eactive powe maintaining the magnetizing cuent. Fom (3) it i evient that thi quantity i inepenent fom tato eitance ue popety of co pouct. he etimate electomotive foce EMF fom liing moe flux obeve i eitance R ˆ epenent q = i e ˆ. (33)

8 Uing (3) a the efeence moel an (33) the ajutable moel, epectively, an MRAS ytem can be ue, whee popotional an integal opeation ae utilize a the aaptation mechanim ˆ t R[ k + 1] = Kp( q qˆ) + Ki ( q qˆ) τ. (34) he etimate tato eitance value R ˆ fom (34) i then ue a an input ignal to the liing moe flux an pee obeve. 7 HIL Simulation of EV he IM ue fo tet i type N9L4, 38 V thee-phae, Y connection, 5 Hz, 1.5 kw, ix-pole, 9 RPM. Paamete in the pe phae teay-tate equivalent cicuit ae: tato eitance R =5.115 Ω, oto eitance R =5.8 Ω, tato an oto inuctance L =L =.167 H, an mutual inuctance L m =.196 H, moto. Lumpe inetia of the DM_LM mechanim i.45 kgm, an the vicou fiction coefficient i.6 Nm. he etup of the applie HIL metho (Dynamic Emulation of Mechanical Loa) i peente in Figue 3 an the expeimental hawae-in-the-loop ytem i hown in Figue 4. G i a ynamic of the teting mechanim, coniting of ive une tet (Dive Machine) an contolle ynamomete (Loa Machine), Dive Machine Loa Machine (DM-LM) mechanim, an G em i the ynamic of the emulate loa. ω i the oto pee of the DM-LM mechanim, ω em the pee of the emulate mechanim, e the applie electical toque of the Dive Machine, an L i the applie loa toque of the expeimental mechanim (Loa Machine). Nonlinea ynamic an toque etimation eo ae peente a input F. J m i the inetia an B m the vicou fiction coefficient of the DM-LM mechanim. Etimate value ae enote by ^, wheea eie value ae enote by. Feeback contolle G t i ue fo the compenation of unmoele ynamic, paamete vaiation, an numeical eo (Figue 3). ^ e G em () ω em ^ G -1 () + + L Contolle Loa Machine L e Contolle - Dive Machine e G t () F J 1 m - B m - ω DM-LM mechanim Figue 3: Dynamic emulation of mechanical loa Setup. Contolle-IM (SPACE) PC - efeence an paamete etting, ata acquiition, oftwae evelopment L out Invete-IM cuent meauement Contolle/ Invete-BLDC DC link -IM ω Dive Machine (IM) Loa Machine (BLDC) e L DM-LM mechnim DC link -BLDCM Figue 4: Expeimental ytem. Inuction moto (Dive Machine) contol i execute with the ue of the SPACE ytem containing DS113 PPC contolle boa, an the Danfo VL54 Invete. he ytem i pogamme with the ue of MALAB/Simulink. Meauement an computation of algoithm ae execute in µ. Buhle

9 AC evomoto of type 14UMD4CACAA pouce by UNIMOOR iven by 7.5kW Digital AC Dive UNI4 (Uniive, Contol echnique) wa ue a the Loa Machine. Shaft of the ive an loa machine ae mechanically connecte with the clutch, which in ieal conition woul eult in both having a common haft. he ynamic of the implifie moel of an electical vehicle wa choen. It moel exhibit a complex nonlinea ynamic, peente in (35): ω e Rb R( CaR ωem + Bωem + mginα) em =, (35) t Je + R ( Jw + m ) whee J e i engine inetia an J M i the lumpe inetia of wheel an axle. R i the gea atio, the aiu of the wheel, m the ma of the vehicle, g the gavity acceleation contant, B the vicou fiction coefficient, an C a the ai eitance coefficient. ω em i the otational pee of the populion ytem an α the teet inclination angle, wheea e i the applie populion ytem toque an b the toque geneate fom the bake. PI contolle wa ue a feeback contolle G t (). Expeimental eult ae hown fo the potion of the ECE-15 tet cycle (Economic Commiion fo Euope, [16]). Fit movement phae (ECE-15 (1)) i peente in Figue 5 - Figue 8, an the econ movement phae (ECE-15 ()) in Figue 9 - Figue 1. Within the movement phae the EV fit acceleate, then fo ome potion of time ive with the contant pee, an finally it eceleate until it i toppe completely. Duing the movement, the tanmiion gea ae ometime witche, witching i coniee to occu momentaily. he ynamic of clutch i not moele. Fo the fit phae of movement it i aume, that the gea atio emain unchange (tanmiion i kept in the lowet gea). Etimate an eie value of applie toque ae peente in Figue 5. he oto haft otation pee ω i peente in Figue 6, togethe with the emulate mechanim (EV) moel pee ω em. Figue 7 featue the calculate loa toque L of EV, applie by the Loa Machine, wheea the pee of vehicle i peente in Figue oque (Nm) 1 Spee (a/) t() Figue 5: ECE-15 (1) - applie toque etimate (otte line, e ) an eie value (oli line, e ) t() Figue 6: ECE-15 (1) - emulate (otte line, ω em ) an actual (oli line, ω ) oto pee. Fo the econ phae of movement the gea atio i changing (the tanmiion gea i witche to the highe one when the vehicle pee uing the acceleation eache 15km/h, an back to the lowe one, when the vehicle pee pae 15 km/h uing the eceleation phae). Etimate an eie value of

10 applie toque ae peente in Figue 9. he oto haft otation pee ω i peente in Figue 1, togethe with the emulate mechanim (EV) moel pee ω em. Figue 11 featue the calculate loa toque L of EV, applie by the Loa Machine, wheea the pee of vehicle i peente in Figue 1. Loa toque (Nm) Spee (km/h) t() Figue 7: ECE-15 (1) Applie loa toque ( L ) t() Figue 8: ECE-15 (1) Deie (otte line) an actual (oli line) pee of EV in km/h. 1 8 oque (Nm) Spee (a/) t() Figue 9: ECE-15 () - applie toque etimate (otte line, e ) an eie value (oli line, e ) t() Figue 1: ECE-15 () - emulate (otte line, ω em ) an actual (oli line, ω ) oto pee. 8 Concluion In thi pape we have peente an avance icete time chatteing fee cheme of IM ue an tete in EV' application. he itinctive featue of the cheme i it obutne to iffeent initial conition value an paamete mimatch. A unifom ynamic IM moel ha been eive to facilitate the toque/flux contol tak. he avantage of the popoe IM vecto contol cheme pevail ove thoe of conventional contol cheme ince no pecie knowlege of moel i neceay. Anothe avantage of the popoe contol i it imple micopoceo implementation.

11 Dynamic emulation of mechanical loa wa peente a a api pototyping eign an teting technique. he emulation i limite to the cetain banwith, epecially in the cae when the paamete of the teting mechanim (DM-LM mechanim) ae not well known. In the peente cae the banwith of the EV i within the banwith of the ynamic emulation poceue. Loa toque (Nm) t() Figue 11: ECE-15 () Applie loa toque ( L ). Spee (km/h) t() Figue 1: ECE-15 () Deie (otte line) an actual (oli line) pee of EV in km/h. he electic ive ytem ae in an avance technological level ue to the contuction of appopiate moto an the fat evelopment of the powe electonic a well a the micoelectonic technology. Batteie have not yet evelope to the equie level a they have a elatively mall powe enity an they ae heavy. So the EV a city ca can not be oubte an thei wie pea ue in the futue i expecte. EV' povie a clean, enegy efficient uban tanpotation altenative. High peciion of the toque contol i alo ueful in the hybi vehicle. Refeence [1] V.I. Utkin, Sliing moe in contol an optimization, Spinge Velag, Belin, 199. [] Z.H. Akpolat, G.M. Ahe, J.C. Clae, "Dynamic Emulation of Mechanical Loa Uing a Vecto Contolle Inuction Moto-Geneato Set", IEEE an. on Inutial Electonic, vol. 46, no., 1999, pp [3] Z.H.Akpolat, G.M. Ahe, J.C.Clae, "A Pactical Appoach to the Deign of Robut Spee Contolle fo Machine Dive", IEEE an. on Inutial Electonic, vol. 47, no.,, pp [4] M. Roič, K. Jezenik, M. lep, "A Feefowa Appoach to the Dynamic Emulation of Mechanical Loa", Poceeing of the 35th Annual IEEE Powe Electonic Specialit Confeence (PESC'4), pp , 4. [5] M. Roič, K. Jezenik, M. lep, "Feefowa an Feeback Appoach fo the Dynamic Emulation of Mechanical Loa". Poceeing of Sympoium on Powe Electonic, Electical Dive, Automation & Motion : SPEEDAM 4, Capi (Italy). pp , 4. [6] R.W. Newton, R.E. Betz, H.B. Penfol, "Emulating Dynamic Loa Chaacteitic Uing a Dynamic Dynamomete", in Poceeing of the IEEE Powe Electonic an Dive Sytem (PEDS), Singapoe, 1995, vol. 1, pp

12 [7] P. Sanholt, E. Ritchie, J.K. Peeen, R.E. Betz, "A Dynamomete Pefoming Dynamical Emulation of Loa with Non-linea Fiction", in Poceeing of the IEEE Intenational Sympoium on Inutial Electonic (ISIE'96), Waaw, Polan, 1996, Pat, pp [8] G.S. Buja, an M.P. Kazmiekowki, Diect oque oque Contol of PWM Invete-Fe AC Moto-A Suvey. In: IEEE anaction on Inutial Electonic, vol. 51, no. 4, 4, pp., [9] W. Leonha, Contol of Electic Dive, Spinge Velag, Belin, Gemany, 3 eition, 1. [1] V.I. Utkin, Sliing Moe Contol Deign Pinciple an Application to Electic Dive, IEEE anaction on Inutial Electonic, vol. 4, 1993, pp [11] A. Šabanović, K. Jezenik, N. Šabanović, an K. Waa, Chatteing Fee Sliing Moe, in: Poc. Wokhop on the Robut Contol via Lyapunov echnique. Benevento, Italy, pp , [1] V.I. Utkin, Sliing Moe Contol in Dicete ime an Diffeence Sytem. Vaiable Stuctue an Lyapunov Contol (A.S. Zinobe, E.). Spinge Velag, Lonon, [13] D.W. Novotny, an.a. Lipo, Vecto Contol an Dynamic of AC Dive, Oxfo Univeity Pe, Lonon. [14] S.H. Kim, S.K. Sul, "Maximum oque Contol of an Inuction Machine in the Fiel Weakening Region", IEEE an. In. App., vol.31, no.4, 1995, pp [15] P. Va, Vecto Contol of AC Machine, Claenon pe, Oxfo, 199. [16] Autho Pof.. Kael Jezenik, Univeity of Maibo, Faculty of Electical Engineeing an Compute Science, Smetanova 17, SI- Maibo, Slovenia el.: , fax: , kael.jezenik@uni-mb.i He eceive B.S. (1968), M.S. (1974) an D.Eng. (1976) egee in electical engineeing fom the Univeity of Ljubljana. In 1976 he joine the Univeity of Maibo an in 1985 he became a Full Pofeo an Hea of the Intitute of Robotic. Hi eeach an teaching inteet inclue automatic contol, obotic, powe electonic an electical ive. Cuent poject in thee aea ae high peciion tacking contol in machine tool an DD obot an obut toque contol in EV'. D. Mian Roič, Univeity of Maibo, Faculty of Electical Engineeing an Compute Science, Smetanova 17, SI- Maibo, Slovenia el.: , fax: , mian.oic@uni-mb.i He eceive B.S. (1994), M.S. (1996) an Ph.D. () egee in electical engineeing fom the Univeity of Maibo. In 1994 he joine the Univeity of Maibo an in 4 he became an Aitant Pofeo. Cuently he wok a Reeache. Hi eeach an teaching inteet inclue automatic contol, obotic, powe electonic an electical ive. Cuent poject in thee aea ae in the fiel of contol of electical ive (with an without pee eno) an mechatonic application (ynamic emulation of mechanical loa).

LOW SPEED SENSORLESS VARIABLE STRUCTURE CONTROL OF INDUCTION MOTOR

LOW SPEED SENSORLESS VARIABLE STRUCTURE CONTROL OF INDUCTION MOTOR LOW SPEED SENSORLESS VARIABLE SRUCURE CONROL OF INDUCION MOOR Kael Jezenik Gego Eelbahe Aif Šabanović Univeity of Maibo Faculty of Electical Engineeing an Copute Science Setanova ul. 7 SI-000 Maibo Slovenia

More information

A Novel Discrete-Time Predictive Current Control for PMSM

A Novel Discrete-Time Predictive Current Control for PMSM A Novel Dicete-Time Peictive Cuent Contol fo SM Jung-Won Sun, Jin-Woo Lee, Jin-Ho Suh, Young-Jin Lee, an Kwon-Soon Lee Depatment of Electical Engineeing, Dong-A Univeity 840, Haan-ong, Saha-gu, Buan, 604-714,

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

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

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

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

MRAS Based Speed Sensor-less Vector Controlled Induction Motor Using Modified Adaptive Mechanism

MRAS Based Speed Sensor-less Vector Controlled Induction Motor Using Modified Adaptive Mechanism Seno & Tanduce, Vol. 55, Iue 8, Augut 23, pp. 8-85 Seno & Tanduce 23 by IFSA http://www.enopotal.com MRAS Baed Speed Seno-le Vecto Contolled Induction Moto Uing Modified Adaptive Mechanim ALIYU Eneji Iah,

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

Passivity-Based Control of Saturated Induction Motors

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

More information

Sensorless Control of Surface Permanent Magnet Synchronous Motor with A Self-Adaptive Flux Obserber

Sensorless Control of Surface Permanent Magnet Synchronous Motor with A Self-Adaptive Flux Obserber 7th WSEAS Int. Conf. on MATHEMATICAL METHODS an COMPUTATIONAL TECHNIQUES IN ELECTRICAL ENGINEERING, Sofia, 27-29/10/05 (pp63-68) Senole Contol of Suface Pemanent Magnet Synchonou Moto with A Self-Aaptive

More information

VECTOR CONTROL OF INDUCTION MOTOR DRIVE BY USING THE CONSTANT SWITCHING FREQUENCY CURRENT CONTROLLER FOR REDUCED RIPPLE

VECTOR CONTROL OF INDUCTION MOTOR DRIVE BY USING THE CONSTANT SWITCHING FREQUENCY CURRENT CONTROLLER FOR REDUCED RIPPLE Acta Electotechnica et Infomatica, Vol. 3, No. 3, 203, 27 33, DOI: 0.2478/aeei-203-0036 27 VECTOR CONTROL OF INDUCTION MOTOR DRIVE BY USING THE CONSTANT SWITCHING FREQUENCY CURRENT CONTROLLER FOR REDUCED

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

Sensorless Speed and Position Control of Induction Motor Drives

Sensorless Speed and Position Control of Induction Motor Drives IECON Roanoke VA, 3 Senole Spee an Poition Contol of Inuction oto Dive aaa Joachim Holtz, Fellow, IEEE Electical achine an Dive Goup, Univeity of Wuppetal 497 Wuppetal Gemany Abtact Contolle inuction moto

More information

Fuzzy Speed Regulator for Induction Motor Direct Torque Control Scheme

Fuzzy Speed Regulator for Induction Motor Direct Torque Control Scheme ACEEE Int. J. on Electical and Powe Engineeing, ol., No., Dec Fuzzy peed Regulato fo Induction Moto Diect Toque Contol cheme Jagadih H. Puja,. F. Kodad Reeach chola JNTU, Anantapu & Faculty Depatment of

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

Accounting for magnetic saturation in induction machines modelling

Accounting for magnetic saturation in induction machines modelling Accounting fo magnetic atuation in inuction machine moelling Hami Ouai, Foua Gii, Luc Duga To cite thi veion: Hami Ouai, Foua Gii, Luc Duga. Accounting fo magnetic atuation in inuction machine moelling.

More information

Transient Stability Analysis of Distributed Generation Connected with Distribution Network

Transient Stability Analysis of Distributed Generation Connected with Distribution Network Intenational Jounal o Electical Enegy Vol. 3 No. 4 Decembe 2015 Tanient Stability Analyi o Ditibute Geneation Connecte with Ditibution Netwok Wei Huang1 Zhipeng Li1 Zehu Zhang2 an Lei Feng3 1 School o

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

Inference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo

Inference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo Infeence fo A One Way Factoial Expeiment By Ed Stanek and Elaine Puleo. Intoduction We develop etimating equation fo Facto Level mean in a completely andomized one way factoial expeiment. Thi development

More information

Performance of a Sensorless Speed Control for Induction Motor Using DTFC strategy and Intelligent Techniques

Performance of a Sensorless Speed Control for Induction Motor Using DTFC strategy and Intelligent Techniques A. ABBOU H. MAHMOUDI J. Electical Sytem 3-5.6(29): 64-8 Regula pape Pefomance of a Senole Speed Contol fo Induction Moto Uing DFC tategy and Intelligent echnique In hi pape, the autho popoe a Senole Diect

More information

Expression of the radiative heat exchange for the human body and its application to modifying the original WBGT for outdoor environment

Expression of the radiative heat exchange for the human body and its application to modifying the original WBGT for outdoor environment Poceeing of Clima 27 WellBeing Inoo Expeion of the aiative heat exchange fo the human boy an it application to moifying the oiginal WBGT fo outoo envionment Kouhei Kuwabaa, Katunoi Nagano, Tohu Mochia

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

CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS

CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS 17 CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS 2.1 DESCRIPTION The development of wind enegy ytem and advance in powe electonic have enabled an efficient futue fo wind enegy. Ou imulation tudy

More information

FUZZY-SLIDING MODE CONTROLLER FOR LINEAR INDUCTION MOTOR CONTROL

FUZZY-SLIDING MODE CONTROLLER FOR LINEAR INDUCTION MOTOR CONTROL FUZZY-SIDING MODE CONTROER FOR INEAR INDUCTION MOTOR CONTRO ABDEKRIM BOUCHETA, ISMAI KHAI BOUSSERHANE,, ABDEDJEBAR HAZZAB, BENYOUNES MAZARI, MOHAMMED KARIM FEAH 3 Key wod: inea induction moto (IM), Vecto

More information

2.3. SLIDING MODE BASED OUTER CONTROL LOOP FOR INDUCTION MOTOR DRIVES WITH FORCED DYNAMICS

2.3. SLIDING MODE BASED OUTER CONTROL LOOP FOR INDUCTION MOTOR DRIVES WITH FORCED DYNAMICS 2.3. SLIDING MODE BASED OUTER CONTROL LOOP FOR INDUCTION MOTOR DRIVES WITH FORCED DYNAMICS Abstact: Though the loa toque estimation, the basic FDC base IM ive contol system pesente in the last two sections

More information

Induction machines (IMs) are widely used in industry applications,

Induction machines (IMs) are widely used in industry applications, Geneic machine ientification an maximum efficiency opeation of inuction machine Julian Kullick an Chitoph M. Hackl axiv:1812.02431v1 [c.sy] 6 Dec 2018 Abtact Thi pape popoe an avance machine ientification

More information

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

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

More information

Symmetry of Lagrangians of holonomic systems in terms of quasi-coordinates

Symmetry of Lagrangians of holonomic systems in terms of quasi-coordinates Vol 18 No 8, Augut 009 c 009 Chin. Phy. Soc. 1674-1056/009/1808/3145-05 Chinee Phyic B an IOP Publihing Lt Symmety of Lagangian of holonomic ytem in tem of quai-cooinate Wu Hui-Bin an Mei Feng-Xiang School

More information

Speed Control of a Doubly Fed Induction Motor using Fuzzy Logic Techniques

Speed Control of a Doubly Fed Induction Motor using Fuzzy Logic Techniques Intenational Jounal on Electical Engineeing and Infomatic - Volume 2, Numbe 3, 2010 Speed Contol of a Doubly Fed Induction Moto uing Fuzzy Logic Technique D. Ben Attou and Y. Bekaka Depatment of Electical

More information

SIMPLE LOW-ORDER AND INTEGRAL-ACTION CONTROLLER SYNTHESIS FOR MIMO SYSTEMS WITH TIME DELAYS

SIMPLE LOW-ORDER AND INTEGRAL-ACTION CONTROLLER SYNTHESIS FOR MIMO SYSTEMS WITH TIME DELAYS Appl. Comput. Math., V.10, N.2, 2011, pp.242-249 SIMPLE LOW-ORDER AND INTEGRAL-ACTION CONTROLLER SYNTHESIS FOR MIMO SYSTEMS WITH TIME DELAYS A.N. GÜNDEŞ1, A.N. METE 2 Abtact. A imple finite-dimenional

More information

Solutions Practice Test PHYS 211 Exam 2

Solutions Practice Test PHYS 211 Exam 2 Solution Pactice Tet PHYS 11 Exam 1A We can plit thi poblem up into two pat, each one dealing with a epaate axi. Fo both the x- and y- axe, we have two foce (one given, one unknown) and we get the following

More information

Optimizing Voltage-Frequency Control Strategy for Single-Phase Induction Motor Drives

Optimizing Voltage-Frequency Control Strategy for Single-Phase Induction Motor Drives Poceeing of the 5th WSEAS Intenational Confeence on Application of Electical Engineeing, Pague, Czech Republic, Mach 12-14, 26 (pp84-89) Optiizing Voltage-Fequency Contol Stategy fo Single-Phae Inuction

More information

CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES

CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES 44 CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES 3.1 INTRODUCTION The contolle equied fo AC dive can be divided into two majo type: cala contol and vecto contol (Boe 1976). In cala contol, which

More information

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection

More information

A Robust Sensorless Direct Torque Control of Induction Motor Based on MRAS and Extended Kalman Filter

A Robust Sensorless Direct Torque Control of Induction Motor Based on MRAS and Extended Kalman Filter Leonado Jounal of Science ISSN 1583-33 Iue 1, Januay-June 8 p. 35-56 A Robut Senole Diect Toque Contol of Induction Moto Baed on MRAS and Extended Kalman Filte Mutapha MESSAOUDI, Habib KRAIEM, Mouna BEN

More information

Model Predictive Control of Induction Motor with Delay Time Compensation: An Experimental Assessment

Model Predictive Control of Induction Motor with Delay Time Compensation: An Experimental Assessment Model Pedictive Contol of Induction Moto with Delay Time Compenation: An Expeimental Aement Mulem Uddin, Saad Mekhilef, Mutuo Nakaoka Powe Electonic and Renewable Enegy Reeach aboatoy (PEAR), Depatment

More information

Simulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements

Simulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model Paamete fom PER ZETTERBERG Stockholm Septembe 8 TRITA EE 8:49 Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model

More information

Development of Model Reduction using Stability Equation and Cauer Continued Fraction Method

Development of Model Reduction using Stability Equation and Cauer Continued Fraction Method Intenational Jounal of Electical and Compute Engineeing. ISSN 0974-90 Volume 5, Numbe (03), pp. -7 Intenational Reeach Publication Houe http://www.iphoue.com Development of Model Reduction uing Stability

More information

Chapter 19 Webassign Help Problems

Chapter 19 Webassign Help Problems Chapte 9 Webaign Help Poblem 4 5 6 7 8 9 0 Poblem 4: The pictue fo thi poblem i a bit mileading. They eally jut give you the pictue fo Pat b. So let fix that. Hee i the pictue fo Pat (a): Pat (a) imply

More information

SIMULATION OF PERMANENT MAGNET SYNCHRONOUS MOTOR CONTROL SYSTEM WITH EXTENTED KALMAN FILTER

SIMULATION OF PERMANENT MAGNET SYNCHRONOUS MOTOR CONTROL SYSTEM WITH EXTENTED KALMAN FILTER 2005-2013 JAI & LLS. All ight eeved. SIMULAION OF PERMANEN MAGNE SYNCHRONOUS MOOR CONROL SYSEM WIH EXENED KALMAN FILER 1 AO XU, 2 ZHENGBIN ZHANG 1 Aoc. Pof., Depatment of Automation, Shenyang Aeopace Univeity,

More information

Determination of Excitation Capacitance of a Three Phase Self Excited Induction Generator

Determination of Excitation Capacitance of a Three Phase Self Excited Induction Generator ISSN (Online): 78 8875 (An ISO 397: 007 Cetified Oganization) Detemination of Excitation Capacitance of a Thee Phae Self Excited Induction Geneato Anamika Kumai, D. A. G. Thoa, S. S. Mopai 3 PG Student

More information

Near-Optimal Relay Station Placement for Power Minimization in WiMAX Networks

Near-Optimal Relay Station Placement for Power Minimization in WiMAX Networks Nea-Optimal elay Station lacement fo owe Minimization in WiMAX Netwok Dejun Yang, Xi Fang an Guoliang Xue Abtact In the IEEE 80.16j tana, the elay tation ha been intouce to inceae the coveage an the thoughput

More information

rad rev 60sec p sec 2 rad min 2 2

rad rev 60sec p sec 2 rad min 2 2 NAME: EE 459/559, Exa 1, Fall 2016, D. McCalley, 75 inute allowed (unle othewie diected) Cloed Book, Cloed Note, Calculato Peitted, No Counication Device. The following infoation ay o ay not be ueful fo

More information

Theorem 2: Proof: Note 1: Proof: Note 2:

Theorem 2: Proof: Note 1: Proof: Note 2: A New 3-Dimenional Polynomial Intepolation Method: An Algoithmic Appoach Amitava Chattejee* and Rupak Bhattachayya** A new 3-dimenional intepolation method i intoduced in thi pape. Coeponding to the method

More information

Sensorless Control of Induction Motor Drives

Sensorless Control of Induction Motor Drives Poceeding of the IEEE, Vol. 9, No. 8, Aug., pp. 359-394 Senole Contol of Induction Moto Dive Joachim Holtz, Fellow, IEEE Electical Machine and Dive Goup, Univeity of Wuppetal 497 Wuppetal Gemany Abtact

More information

The Research of Sensorless Vector Control for Permanent Magnet Linear Synchronous Motor

The Research of Sensorless Vector Control for Permanent Magnet Linear Synchronous Motor 1184 JOURNAL OF COMPUTERS, VOL. 8, NO. 5, MAY 2013 The Reeach of Senole Vecto Contol fo Pemanent Magnet Linea Synchonou Moto Jun Zhu School of Electical Engineeing an Automation, Henan polytechnic Univeity,

More information

DQ Modeling Of Induction Motor With Broken Rotor Bars In MATLAB Simulink

DQ Modeling Of Induction Motor With Broken Rotor Bars In MATLAB Simulink DQ Moeling Of Inuction Moto With Boken Roto Bas In MATLAB Simulink Pincy P 1 an Gayathi Vijayachanan 2 1,2 Depatment. Of Electical an Electonics, See Buha College of Engineeing, Keala Abstact To analyze

More information

Induction Machine Shaft Speed Estimation using Imaginary Power

Induction Machine Shaft Speed Estimation using Imaginary Power Induction Machine Shaft Speed Etimation uing Imaginay Powe Teence Summe, Robet Eic Betz, Bendan McGath, Gaham Cliffod Goodwin School of Electical Engineeing and Compute Science Univeity of Newcatle, Callaghan,

More information

Influences of Interfacial Shear in Turbulent Film Boiling on a Horizontal Tube with External Flowing Liquid

Influences of Interfacial Shear in Turbulent Film Boiling on a Horizontal Tube with External Flowing Liquid Engineeing, 05, 7, 754-764 Publihe Online Novembe 05 in SciRe. http://www.cip.og/jounal/eng http://x.oi.og/0.46/eng.05.7066 Influence of Intefacial Shea in Tubulent Film Boiling on a Hoizontal Tube with

More information

PH126 Exam I Solutions

PH126 Exam I Solutions PH6 Exam I Solutions q Q Q q. Fou positively chage boies, two with chage Q an two with chage q, ae connecte by fou unstetchable stings of equal length. In the absence of extenal foces they assume the equilibium

More information

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

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

More information

AC DRIVES. There are two type of AC motor Drives : 1. Induction Motor Drives 2. Synchronous Motor Drives

AC DRIVES. There are two type of AC motor Drives : 1. Induction Motor Drives 2. Synchronous Motor Drives AC DRIVES AC moto Dive ae ued in many indutial and dometic application, uch a in conveye, lift, mixe, ecalato etc. The AC moto have a numbe of advantage : Lightweight (0% to 40% lighte than equivalent

More information

Advanced energy management strategies for vehicle power nets

Advanced energy management strategies for vehicle power nets Advanced enegy management tategie fo vehicle powe net E.H.J.A. Nuijten, M.W.T. Koot, J.T.B.A. Keel, Bam de Jage, W..M.H. Heemel, W.H.A. Hendix,..J. van den Boch Abtact In the nea futue a ignificant inceae

More information

Speed Sensorless Variable Structure Torque Control of Induction Motor

Speed Sensorless Variable Structure Torque Control of Induction Motor ISSN 0005-1144 ATKAFF 51(1), 33 40(2010) Kael Jezenik, Asif Šabanović, Mian Roič Spee Sensoless Vaiable Stuctue Toque Contol of Inuction Moto UDK IFAC 621.313.333.072.1 5.5.4; 4.0.1 Oiginal scientific

More information

one primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems

one primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems CHAPTER 3: One-Dimenional Steady-State Conduction one pimay diection in which heat tanfe (geneally the mallet dimenion) imple model good epeentation fo olving engineeing poblem 3. Plane Wall 3.. hot fluid

More information

Precision Spectrophotometry

Precision Spectrophotometry Peciion Spectophotomety Pupoe The pinciple of peciion pectophotomety ae illutated in thi expeiment by the detemination of chomium (III). ppaatu Spectophotomete (B&L Spec 20 D) Cuvette (minimum 2) Pipet:

More information

Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic fields. Chapter 28: Magnetic fields

Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic fields. Chapter 28: Magnetic fields Chapte 8: Magnetic fiels Histoically, people iscoe a stone (e 3 O 4 ) that attact pieces of ion these stone was calle magnets. two ba magnets can attact o epel epening on thei oientation this is ue to

More information

Position Control of Linear Induction Motor using an Adaptive Fuzzy Integral - Backstepping Controller

Position Control of Linear Induction Motor using an Adaptive Fuzzy Integral - Backstepping Controller SERBIAN JOURNA OF EECTRICA ENGINEERING Vol. 3, No., June 006, - 7 Poition Contol of inea Induction Moto uing an Adaptive Fuzzy Integal - Backtepping Contolle I. K. Bouehane, A. Hazzab, M. Rahli 3, B. Mazai

More information

The Analysis of the Influence of the Independent Suspension on the Comfort for a Mine Truck

The Analysis of the Influence of the Independent Suspension on the Comfort for a Mine Truck 16 3 d Intenational Confeence on Vehicle, Mechanical and Electical Engineeing (ICVMEE 16 ISBN: 978-1-6595-37- The Analyi of the Influence of the Independent Supenion on the Comfot fo a Mine Tuck JINGMING

More information

Gravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003

Gravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003 avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive

More information

Equilibria of a cylindrical plasma

Equilibria of a cylindrical plasma // Miscellaneous Execises Cylinical equilibia Equilibia of a cylinical plasma Consie a infinitely long cyline of plasma with a stong axial magnetic fiel (a geat fusion evice) Plasma pessue will cause the

More information

About Stability of Mechatronic Systems Driven by Asynchronous Motors

About Stability of Mechatronic Systems Driven by Asynchronous Motors Monica Adela Enache Soin Enache Micea Dobiceanu About Stability of Mechatonic Sytem Diven by Aynchonou Moto MONICA ADEA ENACHE SORIN ENACHE MIRCEA DOBRICEANU Electomechanical Faculty Univeity of Caiova

More information

Speed Control of Matrix Converter-Fed Five-Phase Permanent Magnet Synchronous Motors under Unbalanced Voltages

Speed Control of Matrix Converter-Fed Five-Phase Permanent Magnet Synchronous Motors under Unbalanced Voltages enegie Aticle Speed Contol of Matix Convete-Fed Five-Phae Pemanent Magnet Synchonou Moto unde Unbalanced Voltage Bozou Youefi 1 ID, Soodabeh Soleymani 1, *, Babak Mozafai 1 and Seid Agha Gholamian 2 1

More information

Rotational Kinetic Energy

Rotational Kinetic Energy Add Impotant Rotational Kinetic Enegy Page: 353 NGSS Standad: N/A Rotational Kinetic Enegy MA Cuiculum Famewok (006):.1,.,.3 AP Phyic 1 Leaning Objective: N/A, but olling poblem have appeaed on peviou

More information

PHY 213. General Physics II Test 2.

PHY 213. General Physics II Test 2. Univesity of Kentucky Depatment of Physics an Astonomy PHY 3. Geneal Physics Test. Date: July, 6 Time: 9:-: Answe all questions. Name: Signatue: Section: Do not flip this page until you ae tol to o so.

More information

Comparative Study of Sensorless Control Methods of PMSM Drives

Comparative Study of Sensorless Control Methods of PMSM Drives Compaative Study of Senole Contol Method of PMSM Dive Aafa S. Mohamed, Mohamed S. Zaky, Ahaf S. Zein El Din and Huain A. Yain Electical Engineeing Dept., Faculty of Engineeing, Minoufiya Univeity, Shebin

More information

Jerk and Hyperjerk in a Rotating Frame of Reference

Jerk and Hyperjerk in a Rotating Frame of Reference Jek an Hypejek in a Rotating Fame of Refeence Amelia Caolina Spaavigna Depatment of Applie Science an Technology, Politecnico i Toino, Italy. Abstact: Jek is the eivative of acceleation with espect to

More information

This lecture. Transformations in 2D. Where are we at? Why do we need transformations?

This lecture. Transformations in 2D. Where are we at? Why do we need transformations? Thi lectue Tanfomation in 2D Thoma Sheme Richa (Hao) Zhang Geomet baic Affine pace an affine tanfomation Ue of homogeneou cooinate Concatenation of tanfomation Intouction to Compute Gaphic CMT 36 Lectue

More information

A Nonlinear Controller for Photovoltaic Water Pumping System

A Nonlinear Controller for Photovoltaic Water Pumping System Intenational Jounal of Engineeing Tens an Technology (IJETT) - Volume4Issue5- ay 013 A Nonlinea Contolle fo Photovoltaic Wate Pumping System Hai Kishnan P 1, Ashokkuma K, Bhaathkuma S 3 1 Assistant pofesso,

More information

Intelligent Control for Torque Ripple Minimization in Combined Vector and Direct Controls for High Performance of IM Drive

Intelligent Control for Torque Ripple Minimization in Combined Vector and Direct Controls for High Performance of IM Drive Jounal of Electical Engineeing & Technology Vol. 7, No., pp. ~7, http://dx.doi.og/.7/jeet..7.. Intelligent Contol fo Toque Ripple inimization in Combined Vecto and Diect Contol fo High Pefomance of I Dive

More information

Introduction of a Mathematical Storage Function Model Based on lumping Process of Infiltration Theory

Introduction of a Mathematical Storage Function Model Based on lumping Process of Infiltration Theory Manucipt eceive Oct. 8, 7; evie Ma., 8 Siamak Boaghpou, See Ahma Mibaghei an See Aman Hahemi Monfae Intouction of a Mathematical Stoage Function Moel Bae on lumping Poce of Infiltation Theo SIAMAK BODAGHPOUR,

More information

Rotor Flux Estimation of Induction Motors Using Sliding-Mode Observer

Rotor Flux Estimation of Induction Motors Using Sliding-Mode Observer 5th Intenational Confeence on Sustainable Enegy and Envionment Engineeing (ICSEEE 2016) Roto Flux Estimation of Induction Motos Using Sliding-Mode Obseve Yong Feng1,a, Minghao Zhou1,b and Fengling Han2,c

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

Theory. Single Soil Layer. ProShake User s Manual

Theory. Single Soil Layer. ProShake User s Manual PoShake Ue Manual Theoy PoShake ue a fequency domain appoach to olve the gound epone poblem. In imple tem, the input motion i epeented a the um of a eie of ine wave of diffeent amplitude, fequencie, and

More information

Static Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E.

Static Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E. Coulomb Law Ε Gau Law Electic Potential E Electical Popetie of Mateial Conducto J σe ielectic Capacitance Rˆ V q 4πε R ρ v 2 Static Electic Field εe E.1 Intoduction Example: Electic field due to a chage

More information

Sensors and Actuators Introduction to sensors

Sensors and Actuators Introduction to sensors Sensos an ctuatos Intouction to sensos Sane Stuijk (s.stuijk@tue.nl) Depatment of Electical Engineeing Electonic Systems PITIE SENSORS (hapte 3., 7., 9.,.6, 3., 3.) 3 Senso classification type / quantity

More information

THE INFLUENCE OF THE ROTOR ARCHITECTURE OF A ROTATING WORKING MACHINE ON THE DRIVING POWER

THE INFLUENCE OF THE ROTOR ARCHITECTURE OF A ROTATING WORKING MACHINE ON THE DRIVING POWER U.P.B. Sci. Bull., Seie D, Vol. 77, I. 1, 015 ISSN 1454-358 THE INFLUENCE OF THE ROTOR ARCHITECTURE OF A ROTATING WORKING MACHINE ON THE DRIVING POWER Antonio DETZORTZIS 1, Nicolae BĂRAN, Malik N. HAWAS

More information

6. The Squirrel-Cage Induction Machine . (6.2)

6. The Squirrel-Cage Induction Machine . (6.2) Electical Machine and Dive 6/1 Squiel-Cage nduction Machine Electical Machine and Dive 6/ Squiel-Cage nduction Machine 6. The Squiel-Cage nduction Machine Sliping-induction machine do not only have advantage

More information

Speed Sensorless Control of a Doubly Fed Induction Motor Drives using MRAS Estimator

Speed Sensorless Control of a Doubly Fed Induction Motor Drives using MRAS Estimator Intenational Jounal of Electical Component and Enegy Conveion 018; 4(1): 1-1 http://www.ciencepublihinggoup.com/j/ijecec doi: 10.11648/j.ijecec.0180401.11 ISSN: 469-8040 (Pint); ISSN: 469-8059 (Online)

More information

ANALYSIS AND DESIGN OF ONE-BIT NOISE-SHAPING QUANTIZER USING VARIABLE STRUCTURE CONTROL APPROACH

ANALYSIS AND DESIGN OF ONE-BIT NOISE-SHAPING QUANTIZER USING VARIABLE STRUCTURE CONTROL APPROACH 266 Aian Jounal of Contol, Vol. 7, No. 3, pp. 266-274, Septembe 2005 ANALYSIS AND DESIGN OF ONE-BI NOISE-SHAPING QUANIZER USING VARIABLE SRUCURE CONROL APPROACH Jwuheng Hu and Shiang-Hwua Yu ABSRAC hi

More information

15. SIMPLE MHD EQUILIBRIA

15. SIMPLE MHD EQUILIBRIA 15. SIMPLE MHD EQUILIBRIA In this Section we will examine some simple examples of MHD equilibium configuations. These will all be in cylinical geomety. They fom the basis fo moe the complicate equilibium

More information

GRAVITATION. Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., New Delhi -18 PG 1

GRAVITATION. Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., New Delhi -18 PG 1 Einstein Classes, Unit No. 0, 0, Vahman Ring Roa Plaza, Vikas Pui Extn., New Delhi -8 Ph. : 96905, 857, E-mail einsteinclasses00@gmail.com, PG GRAVITATION Einstein Classes, Unit No. 0, 0, Vahman Ring Roa

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

Performance and Power Factor Improvement of Indirect Vector Controlled Cage Induction Generator in Wind Power Application

Performance and Power Factor Improvement of Indirect Vector Controlled Cage Induction Generator in Wind Power Application Pefomance and Powe Facto Impovement of Indiect Vecto Contolled Cage Induction Geneato in Wind Powe Application DEPARTMENT OF EECTRICA ENGINEERING NATIONA INSTITUTE OF TECHNOOGY, ROURKEA Pefomance and Powe

More information

University of East London Institutional Repository:

University of East London Institutional Repository: Univeity of Eat London Intitutional Repoitoy: http://oa.uel.ac.uk hi pape i made available online in accodance with publihe policie. Pleae coll down to view the document itelf. Pleae efe to the epoitoy

More information

A Crash Course in (2 2) Matrices

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

More information

FRACTIONAL ORDER SYSTEM IDENTIFICATION BASED ON GENETIC ALGORITHMS

FRACTIONAL ORDER SYSTEM IDENTIFICATION BASED ON GENETIC ALGORITHMS Jounal of Engineeing Science and Technology Vol. 8, No. 6 (2013) 713-722 School of Engineeing, Taylo niveity FRACTIONAL ORDER SSTEM IDENTIFICATION BASED ON GENETIC ALGORITHMS MAZIN Z. OTHMAN*, EMAD A.

More information

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer. Kiangsu-Chekiang College (Shatin) F:EasteHolidaysAssignmentAns.doc Easte Holidays Assignment Answe Fom 6B Subject: Physics. (a) State the conditions fo a body to undego simple hamonic motion. ( mak) (a)

More information

Original Method for Stability Analysis of Mechatronic Systems with Asynchronous Machines

Original Method for Stability Analysis of Mechatronic Systems with Asynchronous Machines Soin Enache, Auel Campeanu, Oiginal Method fo Stability Analyi of Mechatonic Sytem with Aynchonou Machine SORIN ENACHE, AUREL CAMPEANU, ION VLAD, MONICA ADELA ENACHE Electomechanical Faculty Univeity of

More information

PHY132 Lecture 6 02/05/2010. Lecture 6 1

PHY132 Lecture 6 02/05/2010. Lecture 6 1 Claical Phyic II PHY3 Lectue 6 The lectic Potential ti - II /5/ Lectue 6 Wok by a Vaying Foce Wok i a cala quantity, an we can thu a little piece of wok togethe, i.e. um a eie of ot-pouct of the foce F(

More information

Determining the Best Linear Unbiased Predictor of PSU Means with the Data. included with the Random Variables. Ed Stanek

Determining the Best Linear Unbiased Predictor of PSU Means with the Data. included with the Random Variables. Ed Stanek Detemining te Bet Linea Unbiaed Pedicto of PSU ean wit te Data included wit te andom Vaiable Ed Stanek Intoduction We develop te equation fo te bet linea unbiaed pedicto of PSU mean in a two tage andom

More information

Electric Potential and Gauss s Law, Configuration Energy Challenge Problem Solutions

Electric Potential and Gauss s Law, Configuration Energy Challenge Problem Solutions Poblem 1: Electic Potential an Gauss s Law, Configuation Enegy Challenge Poblem Solutions Consie a vey long o, aius an chage to a unifom linea chage ensity λ a) Calculate the electic fiel eveywhee outsie

More information

Mathematical Model of the Three-Phase Induction Machine for the Study of Steady-State and Transient Duty Under Balanced and Unbalanced States

Mathematical Model of the Three-Phase Induction Machine for the Study of Steady-State and Transient Duty Under Balanced and Unbalanced States Chapte 1 Mathematical Model of the Thee-Phae Induction Machine fo the Study of Steady-State and Tanient Duty Unde Balanced and Unbalanced State Alecandu Simion, Leonad Livadau and Adian Munteanu Additional

More information

Integral Control via Bias Estimation

Integral Control via Bias Estimation 1 Integal Contol via Bias stimation Consie the sstem ẋ = A + B +, R n, R p, R m = C +, R q whee is an nknown constant vecto. It is possible to view as a step istbance: (t) = 0 1(t). (If in fact (t) vaies

More information

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

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

More information

Then the number of elements of S of weight n is exactly the number of compositions of n into k parts.

Then the number of elements of S of weight n is exactly the number of compositions of n into k parts. Geneating Function In a geneal combinatoial poblem, we have a univee S of object, and we want to count the numbe of object with a cetain popety. Fo example, if S i the et of all gaph, we might want to

More information

Physics C: Electricity and Magnetism

Physics C: Electricity and Magnetism Physics C: Electicity an Magnetism TABLE OF INFORMATION FOR CONSTANTS AND CONVERSION FACTORS - unifie atomic mass unit, u =. 66 7 kg = 93 MeV/ c Poton mass, m p = 67. 7 kg Neuton mass, m n = 67. 7 kg Electon

More information

Nonlinear Control of an Induction Motor Using a Reduced-Order Extended Sliding Mode Observer for Rotor Flux and Speed Sensorless Estimation

Nonlinear Control of an Induction Motor Using a Reduced-Order Extended Sliding Mode Observer for Rotor Flux and Speed Sensorless Estimation Engineeing, 00,, 83-89 doi:0.436/eng.00.004 Publihed Online Octobe 00 (http://www.scirp.og/jounal/eng) Nonlinea Contol of an Induction Moto Uing a Reduced-Ode Extended Sliding Mode Obeve fo Roto Flux and

More information

Mathematical Models of High-Speed Trains Movement

Mathematical Models of High-Speed Trains Movement Mathematical Model of High-Speed Tain Movement CISMARU CRISTIAN DANIEL NICOLA DORU ADRIAN MANOLEA GHEORGHE DRIGHICIU MIRCEA ADRIAN BULUCEA CORNELIA AIDA Faculty of Electomechanical Engineeing Univeity

More information

AE 423 Space Technology I Chapter 2 Satellite Dynamics

AE 423 Space Technology I Chapter 2 Satellite Dynamics AE 43 Space Technology I Chapte Satellite Dynamic.1 Intoduction In thi chapte we eview ome dynamic elevant to atellite dynamic and we etablih ome of the baic popetie of atellite dynamic.. Dynamic of a

More information