Modeling and Field-Oriented Control of the Dual Stator Winding Induction Motor in the EMTP-Type Environment

Size: px
Start display at page:

Download "Modeling and Field-Oriented Control of the Dual Stator Winding Induction Motor in the EMTP-Type Environment"

Transcription

1 Modelng and Feld-Oented Contol of the Dual Stato Wndng Inducton Moto n the EMP-ype Envonent hban hbungu Abtact--he dual tato wndng nducton oto uppled by edundant Vaable Fequency Dve (VFD) fnd t applcaton n hp populon, locootve tacton, and aeopace. he edundancy of VFD lead to elablty and afety fo a contnuou avalablty of the yte even when one VFD ha faled. h pape popoe the odelng n an abtay efeence fae of dual tato wndng (wth an abtay dplaceent between the two thee-phae wndng et) nducton oto wth atuaton of the an flux fo the EMP-type oluton. he Indect Feld Oented Contol baed on the two ax d-q odel of the dual tato wndng nducton oto nvetgated and can be extended to any nube of phae, whch ae a ultple of thee. he contol can be pleented ung two VFD bult a an Actve Font End (AFE) Rectfe followed by Voltage-Souced Invete (VSI) baed nuodal PWM o cuent hytee contolle. he popoed odelng and contol wa ulated by ung the Engneeng Sute V6 oftwae and the ulaton eult how the plcty of the contol chee. Keywod: Dual Stato Inducton Moto (DSIM), Indect Feld Oented Contol (IFOC), Vaable Fequency Dve, AFE Rectfe. I. INRODUCION HE concept of ultphae (oe than thee-phae) achne odelng and dve not new. hee ae aleady lot of exaple n lteatue decbng ultphae achne [] [4], whch ae jut a epeentatve aple. Recently, oe attenton ha been gven to odelng and contol of a ultphae oto, epecally ultphae nducton oto. Geneally, a ultphae nducton oto dve ha any advantage ove the conventonal thee-phae dve uch a hgh powe capablty by dvdng powe between ultple phae, educed toque pulaton and hghe elablty. In patcula, wth the lo of one o oe tato wndng et, a ultphae nducton oto can contnue to opeate. he odelng and dve of a ultphae nducton oto can ue a vaety of tanfoaton. he yetcal coponent theoy and the atx theoy eve a theoetcal foundaton fo thee tanfoaton. A an advantage, by egentng equally the appled powe n ultphae nducton, t poble to upply hban hbungu wth Sat echnologe, Inc., Place du Coece, Boad (Québec), Canada, J4W 3B3. Engneeng Sute V6 a tadea of Sat echnologe, Inc. one o oe wndng unde balanced conon f fo any eaon oe of the cannot be uppled. he an focu of th pape to develop a dynac odel of the DSIM fo any abtay angle of dplaceent between the two wndng et fo the EMP-type oluton. he d-q odel n an abtay efeence fae odel ha been developed and can be ued to analyze the behavo of an nducton oto n any efeence fae. A ple IFOC chee contol fo an unatuated DSIM pleented ung two VFD bult a Actve Font End (AFE) Rectfe followed by VSI baed hytee cuent contolle. Snce the DSIM not avalable n tandad lbay of ot electcal oftwae, the valdaton and popoed contol of the Engneeng Sute V6 oftwae odel (ethe n teady tate o tanent) wee copaed wth the odel bult n the MALAB/SIMULINK envonent. Howeve, only the eult obtaned fo the Engneeng Sute V6 ae peented. A. Aupton II. MODELING OF DSIM he DSIM degned a an electoechancal yte copoed on the tato de by two wye thee-phae wndng, whch ae gounded though two epaate neutal pedance, efeed to a tato 1 and tato and on the oto de by a coon quel cage. he quel cage eplaced by an equvalent thee-phae wndng. he DSIM depcted n Fgue 1. he odelng of th oto ue the followng aupton: Stato wndng ae nuodally buted aound the a gap, he two et of tato wndng ae patally hfted by an electcal angle α, he yety of the wndng and only the atuaton of the an flux ae condeed, he agnetc couplng between tato wndng 1 and condeed though the an flux; the couplng of thee wndng though the leaage flux neglected, All the electoagnetc vaable and paaete of the oto ae efeed to the tato de. Pape ubtted to the Intenatonal Confeence on Powe Syte anent (IPS015) n Cavtat, Coata June 15-18, 015

2 unat unat d L d1 L d L d d (16) b b1 b a a α a1, d q d-q agnetzng flux coecton te R, L Neutal etance and nductance n n he echancal equaton gven a follow: c1 c Fg. 1. Wndng of DSIM B. DSIM equaton n dq0 Refeence Fae he odelng of the DSIM tat wth the clacal appoach of odelng the thee-phae nducton oto. he DSIM condeed a two ndependent thee-phae oto coupled though a coon oto wndng. he Pa tanfoaton tanfo abc efeence fae voltage and flux equaton nto an abtay dq0 efeence fae. ang nto account the an flux lnage atuaton by addng the d-q agnetzng flux coecton te [10] to the an flux, the voltage and flux equaton nto an abtay dq0 efeence fae ae a follow: dq1 vq1 Rq1 ωd1 (1) dd1 vd1 Rd1 ωq1 () d01 v01 ( R 3 Rn ) 01 (3) dq vq Rq ωd (4) dd vd Rd ωq (5) d0 v0 ( R 3 Rn ) 0 (6) dd vd Rd ( ω ω ) q (7) dq vq Rq ( ω ω ) d (8) unat unat q1 Lq1 L q L q q c (9) unat unat d1 Ld1 L d L d d (10) ( l 3 L ) (11) 01 σ n 01 unat unat q Lq L q1 L q q (1) unat unat d Ld L d1 L d d (13) ( l 3 L ) (14) 0 σ n 0 unat unat q L q1 L q Lq q (15) dω J e dω load (17) ( 1 ) ( 1 ) 3 p L e d q q q d d L (18) ω ω (19) p ω, ω p, d load, e Mechancal and electcal peed ad/ Nube of poleand dapng facto N /ad Load and electoagnetc toque C. anent Modelng Snce v d 0 and v q 0, equaton (15) and (16) nto (7) and (8) and applyng the tapezodal ule, the atx fo of oto d-q cuent n an abtay efeence fae a follow: d 1 d q1 htd ( t ) [ C] q ht ( ) d q t q ( ) ( ) ht t, ht t Roto d-q htoy te d q Saple te [ C ] -by-4 atx (0) Replacng (9) to (14) nto (1) to (6) and applyng the tapezodal ule, we have: d 1 vd 1 q1 htd 1 ( t ) vq1 ht q1 ( t d ) [ Z ] vd ( t ) q t htd ( t ) vq htq ( t d ) q (1)

3 ( ) ( ) v0 1 t R t ht0 1 t v0 t 0 R 0 0 t ht0 t ( lσ 3 Ln ) R0 ( R 3 Rn ) Z 4-by-6 etance atx [ ] ( ) ht t () Stato dq0 htoy te fo d1, d, q1, q,01,0 he eleent n atce [ C] and [ Z ] ae a functon of the oto paaete and the peed devaton. Snce the peed change lowly, n copaon wth the electcal quantte, and peed at te t unnown, the equaton (0) and (1) ae lneazed by ung the pedcto coecto ethod [8]. he followng pedcton ued: ( t ) ( t ) ω ω ω (3) he tato and oto d-q htoy te ae not only dependent on pevou d-q cuent and peed devaton but alo on pevou and actual d-q agnetzng flux coecton te. Snce d-q agnetzng flux coecton te at te t ae unnown, the thee-pont pedcto foula wll be ued (ee atuaton odelng). Replacng (0) nto (1), we have: vd 1 t d 1 t ed1( t ) v t t e ( t ) q1 q1 q1 R dq v e d ( t ) d t d t v t t eq ( t ) q q R dq 4-by-4 etance atx (4) Applyng Pa nvee tanfoaton (ee appendx), the voltage equaton n abc efeence fae ae a follow: vabc1 t Zabcabc1 t Zabc1 abc t eabc1 (5) vabc t Zabc1abc1 t Zabc abc t eabc (6) conductance equaton fo a follow: abc 1 t vabc 1 t h 1 t [ G] abc t vabc t h t 1 [ ] Gabc Gabc1 Zabc Zabc1 G Gabc1 Gabc Zabc1 Zabc 6-by-6 conductance atx (7) h 1 t eabc 1 t h [ G] 6-by-1 cuent htoy h t eabc t he odelng n a oto, fo a ynchonou and tatonay efeence fae, ae obtaned epectvely by ettng: ω ω, ω ω, ω 0 Gven a powe yte netwo decbed by the followng nodal equaton: t G v t hn n abcn (8) Hee, ouce, hn n epeent the netwo htoy cuent G denote the oveall conductance atx wthout ncopoatng the DSIM conductance atx and vabcn epeent the nodal voltage. A ngle DSIM ntefaced wth the above powe yte netwo by olvng (7) fo the tato cuent and then ubttutng the nto (8). he fnal lnea yte of equaton n te of nodal voltage ha the followng tandad fo: h t Geq vabcn t (9) Fgue llutate the foulaton of (9) whee t hown that G n and hn t ae odfed by ncludng the 6-by-6 h 6-by-1 oto cuent htoy te to the coepondng oto node. oto equvalent conductance [ G ] and [ Zabc ] [ Z ] [ Z ] e abc1 abc1 abc1 abc Self-etance atx, Mutual etance atce, e Voltage behnd etance D. Intefacng DSIM wth EMP-type netwo oluton he coplete odel of the DSIM fo the EMP-type oluton obtaned afte cobnng (5) and (6) n the Fg.. Contbuton of the DSIM to the netwo nodal equaton.

4 E. Satuaton Modelng he chaactetc of nonlnea nductance cuent dependent can be epeented a a ult pecewe lnea nductance wth oe lope. Let aue that the flux veu agnetzng cuent povded (Fg. 3.), whch only the ft quadant hown, and uppoed to be yetcal. unat L unat L unat d d (36) unat q q (37) 3. Detene the appopate pece of atuated lne ung and calculate the agnetzng flux coecton te: unat t L b (38) 4. Calculate d-q agnetzng flux coecton te a follow: he agnetzng flux gven a follow: Fg. 3. Magnetzng Flux v cuent of the DSIM unat L at fo a gven agnetzng cuent (30) < 0 the agnetzng flux coecton te. unat d d (39) at unat q q (40) at III. INDIREC FIELD ORIENED CONROL Neglectng atuaton and f we chooe a new d-q ax otatng at a ynchonou peed and algned wth the oto feld, that ean q 0, and the electoagnetc toque wll be: Snce the agnetzng flux veu cuent can be appoxated at t L t a a ult pecewe lnea cuve a, whee the nee pont flux, the teatve algoth fo calculatng the d-q flux atuaton effect a follow: e 3 p L L dq q q1 q (41) 1. Calculate the agnetzng cuent ung the thee-pont pedcto foula: ( t ) ( t ) ( t 3 ) (31) 4 4 t t t t (3) 1 d d d d t t t t (33) q q1 q q t d t q t, Repeent d-q agnetzng cu ent d q May be,,,,, d1 d q1 q d q (34). Calculate the unatuated flux (a gap taght lne), d and q utual flux ung the pedcted d-q cuent: unat L unat (35) If contant, whch ple that 0, the d electoagnetc toque wll depend only on q equaton (8), (15) and (16) gve: Rq ω Ld d. Hence, ω (4) d d L (43) d d1 d If the agntude d ha to be changed, (7), (16) and nowng that q 0, we have: L d d (44) 1 τ L τ R

5 A. VSI Baed Hytee Cuent Contolle Snce the nvete contolled by a hytee cuent contolle, only the peed and flux contolle hould be degned. 1) Flux PI Contolle Degn he followng contolle wll output the d ax cuent (efeence) d gven a follow: L and pf pf ( 1 τ ). Ung (44), the open loop tanfe functon ( 1 ) (45) ae epectvely the te contant and popotonal gan of the flux contolle. Fo a gven α, te contant of the flux cloed loop tanfe functon, the flux contolle paaete ae calculated ung the Intenal Model Contol (IMC) and the tanfe functon gven a follow: G c ( ) τ 1 L α L α (46) Snce both tato ut have equal d ax cuent, d ax cuent (efeence) fo each tato obtaned a follow: d1 d d (47) ) Speed PI Contolle Degn he followng contolle wll output a efeence toque e. Ung (17) and (41), the open loop tanfe functon gven a: p ( 1 ) ( ) (48) 1 τ an d p ae epectvely te contant and popotonal gan of the peed contolle. 3 p L t J,, τ L t d d d By ung the pole placeent ethod, one can place pole at p 1 and p, and t wll be aued that p1 the donant pole. hu, the peed contolle paaete ae calculated a follow: p ( p p ) τ 1 1 p τ p p 1 he u of tato q ax cuent obtaned by ung (41), whee toque and flux ae epectvely the output of peed and flux contolle. Fo both tato havng equal q ax cuent, we have: q1 q q (49) B. Vaable Fequency Dve and Contol Fgue 3, 4 and 5 uaze the pleentaton of the two VFD dve DSIM. Paaete of the DSIM and load odel ae gven n the appendx. VFD have been degned n Engneeng Sute V6 wth unty powe facto AFE ectfe. DC voltage contol ae baed on hytee cuent contolle and voltage contolle ae degned ung abc Refeence Fae ethod. vabc d abc 0 q θ abc Fg. 4. Daga bloc of an AFE ectfe DC voltage contol IV. SIMULAION PARAMEERS A. AFE Rectfe Contolle and Degn fo Unty Powe Facto wo epaate 3-phae voltage ouce 460 V, 60 Hz, R 0.15 Ω,L 8 H upply two AFE ectfe that feed the nvete. he DC efeence voltage et to 1000 Volt. he IGB (odeled by deal wtch n paallel wth a dode) tggeed by a hytee contol whch et to h ±0.1 A. he dode nubbe RC ae C n 0.1 µf and R n 500 Ω.he capacto ntally chaged at 1000 Volt and C 5000 µf. pv ABLE I AFE RECIFIER VOLAGE CONROLLER PARAMEER pv v Voltage contolle and v ae epectvely the popotonal and ntegal of the ectfe voltage contolle.

6 Fg. 5. Daga of VFD dve DSIM e q q abc d 3 p L L abc L 1 τ d d d q1 d1 abc1 abc d α abc1 abc1 q Fg. 6. Daga bloc of the DSIM peed contol wth IFOC B. DSIM Contolle and Degn he two nvete that contol the DSIM ae contolled by a hytee cuent contolle. he hytee contol et to h ± 0.5 A. Ung the foula developed fo peed and flux contolle, the followng table uaze the PI Contolle paaete. p and ABLE II DSIM FLUX AND SPEED CONROLLER PARAMEERS Flux contolle Speed contolle ae epectvely the popotonal and ntegal of the flux o peed contolle. V. SIMULAION RESULS he ft cenao wa caed out to copae onlne tatup of the atuated (blac colo) and unatuated (blue colo) p oto dvng load odel 1. Fgue 7 and 8 how the peed (ad/) and electoagnetc toque (N) of the atuated and unatuated oto ung the odel pleented n the Engneeng Sute V6. Fgue 9 and 10 how the tato cuent (A) of both tato (cae of unatuated oto). he econd cenao wa caed out ung VFD to dve the DSIM connected to the load odel. A efeence peed of 10 ad/ and -10 ad/ ae appled epectvely at t 0 and t 1.6. Fgue 11 and 1 how contol of electoagnetc toque and peed. oque lted to 500 N a equeted. Fgue 13 and 14 how tanent and teady tate of both tato cuent (A). Both cuent ae equal n agntude nce d-q cuent contol ae equally haed between both tato. Fgue 15 how contol of the flux (Wb) veu t efeence. he thd cenao tude the behavo of long one of the nvete when the yte connected to load odel. A efeence peed of 10 ad/ appled and nvete lot at t 1.4. Fgue 16 and 17 how peed (ad/) and electoagnetc toque (N). A expected at t 1.4 when nvete dconnected, peed and toque dop. he toque fall to half of the teady tate value befoe nceang to the deed value equeted by the peed contolle n ode to

7 eet the efeence peed. A a conequence, Fgue 18 and 19 how tanent and teady tate of both tato cuent (A), whee tato 1 cuent double the teady tate value. Fgue 0 how the tanent of flux (Wb). Fg. 7. Speed fo unatuated v atuated oto Fg. 8. oque fo unatuated v atuated oto Fg. 9. Stato 1 cuent fo unatuated oto Fg. 10. Stato cuent fo unatuated oto Fg. 11. Electoagnetc v Load toque Fg. 1. Speed v efeence Fg. 13. anent-dsim tato 1 cuent Fg. 14. anent-dsim tato cuent Fg. 15. Magnetzng flux v efeence Fg. 16. Speed v efeence Fg. 17. Electoagnetc v Load toque Fg. 18. anent-dsim tato 1 cuent

8 Fg. 19. anent-dsim tato cuent Fg. 0. Magnetzng flux v efeence VI. CONCLUSIONS he odelng of the DSIM fo the EMP-type oluton and a ple appoach to the IFOC ha been peented. he valy of the odel and contol wa vefed by eveal nfoatve ulaton. he odelng and contol of the DSIM ae baed on a two axe d-q odel, and can be ealy extended to any nube of phae, whch ae a ultple of thee. he DSIM can be odeled n any efeence fae and any abtay angle dplaceent between the two thee-phae wndng et. he edundancy of the VFD pove elablty and avalablty of the yte even when one VFD ha faled. Wthn the acceptable lt fo the DSIM cuent, the ple IFOC peented allow contol of the DSIM unde balanced conon and equed toque even when one of the nvete out of evce. VII. APPENDIX Load Model 0.5 ω, gn ω ω load1 load Pa nvee tanfoaton nγ coγ 1 f n ( π ) co( π abc γ γ ) 1 f 3 3 dq0 n ( γ π ) co ( γ π ) Fo the oto γ θ θ, fo the tato 1 γ θ and the tato γ θ α. f : Voltage o cuent θ : Angle between tato and oto dentcal phae θ : Angle between q ax and tato phae A he DSIM a 460 V, 60 Hz, 4 pole and α 30. he axu toque allow 500 N and the oto ungounded though an pedance R 1e5 Ω, L 0 H. he DSIM paaete ae gven n table III. Stato etance Roto etance ABLE III n DSIM PARAMEERS Roto leaage nductance Stato leaage nductance Magnetzng nductance R R n Ω 0.8 Ω l σ 0.8 H l σ 0.8 H L 34.7 H Moent of Ineta J 1.66 g Rated flux 1 Wb d Satuaton cuve ( Wb) Fo 8.9A ( Wb) Fo > 8.9A 0 VIII. REFERENCES [1] Alf Kae Adnae, Mate Electcal Intallaton and Deel Electc Populon, ABB AS Mane, Olo, Apl 003. [] Sngh G. K., Na K. and L S. K., A ple ndect feld-oented contol chee fo ultphae nducton oto, IEEE an. Ind. Elec., vol.5, Aug [3] A. Munoz and. A. Lpo, Dual tato wndng nducton achne dve, IEEE an. Ind. Appl., vol.36, Sept/Oct [4]. A. Lpo, A d-q odel fo x phae nducton achne, Poc. Int. Conf. Electc Machne, Athen, Geece, [5] D. W. Novotny and. A. Lpo, Vecto Contol and Dynac of AC Dve. Oxfod, U.K. Claendon, [6] Zhao Y. and. A. Lpo, Space Vecto PWM Contol of Dual hee- Phae Inducton Machne Ung Vecto Space Decopoton, IEEE an. Ind. Appl., vol.31, [7] G.K. Sngh, Mult-phae nducton achne dve eeach- A uvey, Elect. Powe Syt. Re., vol. 6, 00. [8] Doel, H. W., EMP heoy boo, Mcotan Powe Syte Analy Copoaton, Vancouve, [9] Hubet Raz, Handboo of Aynchonou Machne wth Vaable Speed. 1 t Eon, Wley, 011. [10] P. C. Kaue, O. Waynczu, S.D. Sudhoff, Analy of Electc Machney and Dve Syte. nd Eon, IEEE Pe, Wley- Intecence, 00. [11] M. P. Kazeow, F. Blaabjeg, R. Khnan, Contol In Powe Electonc. Selected Poble. Acadec Pe, 00. [1] Gaha C. Goodwn, Stefan F. Gaebe, Mao E. Salgado, Contol Syte Degn. 1 t Eon, Pentce Hall, 000.

Dynamic Modeling and Simulation of a 3-HP Asynchronous Motor Driving a Mechanical Load.

Dynamic Modeling and Simulation of a 3-HP Asynchronous Motor Driving a Mechanical Load. Dynac Modelng and Sulaton of a 3-HP Aynchonou Moto Dvng a Mechancal Load. C.U. Oguka, M.Eng. Depatent of Electcal Engneeng, Unvety of Ngea, Nukka, Ngea. E-al: ucoguka@yahoo.co ABSTRACT The qd0 tanfoaton

More information

Sensorless Control of Induction Motor using Simulink by Direct Synthesis Technique

Sensorless Control of Induction Motor using Simulink by Direct Synthesis Technique Intenatonal Jounal of Electcal Engneeng. ISSN 0974-258 olue 4, Nube (20), pp.23-32 Intenatonal Reeach Publcaton Houe http://www.phoue.co Senole Contol of Inducton Moto ung Sulnk by Dect Synthe Technque

More information

Modeling, Simulation & Control of Induction Generators Used in Wind Energy Conversion

Modeling, Simulation & Control of Induction Generators Used in Wind Energy Conversion Modelng, Sulaton & Contol of nducton Geneato Ued n Wnd Enegy Conveon Chapte-4 Equvalent Ccut and Matheatcal Model of nducton Geneato 4. ntoducton: n peent-day pactce, two type of geneato uually fnd applcaton

More information

ASSESSMENT OF STRESSES ON INDUCTION MOTOR UNDER DIFFERENT FAULT CONDITIONS

ASSESSMENT OF STRESSES ON INDUCTION MOTOR UNDER DIFFERENT FAULT CONDITIONS Jounal of Theoetcal and Appled Infoaton Technology 2005-2009 JATIT. All ght eeved. www.jatt.og ASSESSMENT OF STESSES ON INDUCTION MOTO UNDE DIFFEENT FAUT CONDITIONS 1 B.AUNA KUMAI, 2 K.NAGA SUJATHA, 3

More information

Stability Analysis of Simultaneous Estimation of Speed and Stator Resistance for Sensorless Induction Motor Drives

Stability Analysis of Simultaneous Estimation of Speed and Stator Resistance for Sensorless Induction Motor Drives Poceedng of the 4 th Intenatonal Mddle Eat Powe yte Confeence (MEPCON 0), Cao Unvety, Egypt, Decebe 9-, 00, Pape ID 80. tablty Analy of ultaneou Etaton of peed and tato Retance fo enole Inducton Moto Dve

More information

Mechanical design of IM. Torque Control of. Induction Machines... Slip ring rotor. Mathematical model. r r. Stator same as PMSM Rotor:

Mechanical design of IM. Torque Control of. Induction Machines... Slip ring rotor. Mathematical model. r r. Stator same as PMSM Rotor: Toqe ontol of Incton Machne... a copae to PMSM Intal Electcal Engneeng an Atoaton Mechancal egn of IM Stato ae a PMSM oto: at aln Won coppe /Slp ng Intal Electcal Engneeng an Atoaton n Unvety, Sween Nan

More information

Magnetic Flux Density Feedback Control for Permanent Magnetic- Electromagnetic Hybrid Suspension System

Magnetic Flux Density Feedback Control for Permanent Magnetic- Electromagnetic Hybrid Suspension System MATEC Web of Confeence 95, 5 (7 DOI:.5/ atecconf/7955 ICMME 6 Magnetc Flux Denty Feedback Contol fo Peanent Magnetc- Electoagnetc Hybd Supenon Syte Qang CHEN, Je LI, Guanchun LI, Syang ZHOU College of

More information

Effects of Rotor Air-gap Eccentricity on the Power Factor of Squirrel Cage Induction Machines

Effects of Rotor Air-gap Eccentricity on the Power Factor of Squirrel Cage Induction Machines Effect of Roto A-gap Eccentcty on the Powe Facto of Squel Cage Inducton Machne H. Mehgn-Kelk, J. Mlmonfaed Electc Machne and Dve Laboatoy Depament of Electcal Engneeng Amkab Unvety of echnology ehan 594,

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

SOME SUBJECTS OF COMPENSATION OF THE INDUCTION GENERATORS REACTIVE POWER IN WIND-POWER AND SMALL HYDROELECTRIC POWER PLANTS

SOME SUBJECTS OF COMPENSATION OF THE INDUCTION GENERATORS REACTIVE POWER IN WIND-POWER AND SMALL HYDROELECTRIC POWER PLANTS R.I. Mutafayev, L.H. Haanova, M.M. Muayev THE PAPER NAME SOME SUBJECTS OF COMPENSATION OF THE INDUCTION (Vol.8) 0, Decebe SOME SUBJECTS OF COMPENSATION OF THE INDUCTION GENERATORS REACTIVE POWER IN WIND-POWER

More information

ISSN International Journal of Advanced Research (2014), Volume 2, Issue 4, RESEARCH ARTICLE

ISSN International Journal of Advanced Research (2014), Volume 2, Issue 4, RESEARCH ARTICLE ISSN 3-547 Intenatonal Jounal of Advanced Reeach (14), Volume, Iue 4, 474-483 Jounal homepage: http://www.jounalja.com INTERNATIONA JOURNA OF ADVANCED RESEARCH RESEARCH ARTICE Effcency Impovement of Thee

More information

RX Model-Based Newton Raphson Load Flow for Distribution Power System Considering Wind Farm with Asynchronous Generators

RX Model-Based Newton Raphson Load Flow for Distribution Power System Considering Wind Farm with Asynchronous Generators T. T. han and. L. Nguyen / GMSARN Intenatonal Jounal 0 (06-8 R Model-Baed Newton Raphon Load Flow fo Dtbuton owe Syte Condeng Wnd Fa wth Aynchonou Geneato Tong Tuan han and an Le Nguyen Abtact Th pape

More information

Observer Based Parallel IM Speed and Parameter Estimation

Observer Based Parallel IM Speed and Parameter Estimation SERBIAN JOURNAL OF ELECTRICAL ENGINEERING Vol. 11, No. 3, Octobe 2014, 501-521 UDC: 621.313.333-253:519.853 DOI: 10.2298/SJEE1403501S Obeve Baed Paallel IM Speed and Paamete Etmaton Saša Skoko 1, Dako

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

Predictive Vector Control Based Induction Motor Drive using Fuzzy Controller

Predictive Vector Control Based Induction Motor Drive using Fuzzy Controller Intenatonal Jounal of Scence, Engneeng and Technology Reeach (IJSETR, Volume 4, Iue 11, Novembe 2015 Pedctve Vecto Contol Baed Inducton Moto Dve ung Fuzzy Contolle G. Vcto Raj 1, K.Venkataamana 2, V.Chatanya

More information

Generalized State-Space Modeling of Three Phase Self-Excited Induction Generator For Dynamic Characteristics and Analysis

Generalized State-Space Modeling of Three Phase Self-Excited Induction Generator For Dynamic Characteristics and Analysis 48 Jounal of Electcal Engneeng & Technology, ol., No. 4,. 48~489, 6 Genealzed State-Sace Modelng of Thee Phae Self-Excted Inducton Geneato Fo Dynac haactetc and Analy Galaat Sath Kua* and Anah Khoe** Abtact

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

Direct Torque Control Scheme For Dual-Three-Phase Induction Motor

Direct Torque Control Scheme For Dual-Three-Phase Induction Motor The Intenatonal Powe Electonc Confeence Dect Toque Contol Scheme Fo Dual-Thee-Phae Inducton Moto R. Zameddne, T. Undeland Depatment of Electc Powe Engneeng Enegy Coneon Reeach Goup Nowegan Unety of Scence

More information

Modelling and Simulation of Multiple Single - Phase Induction Motors in Parallel Operation

Modelling and Simulation of Multiple Single - Phase Induction Motors in Parallel Operation Poceedn of the 8th WSEAS Int. Confeence on Automatc Contol Modeln and Smulaton Paue Czech Republc Mach -4 6 (pp95-) Modelln and Smulaton of Multple Snle - Phae Inducton Moto n Paallel Opeaton SAKRAWEE

More information

The Fuzzy Tracking Control of Output vector of Double Fed Induction Generator DFIG via T S Fuzzy Model

The Fuzzy Tracking Control of Output vector of Double Fed Induction Generator DFIG via T S Fuzzy Model Receved: Augut 25, 2017 113 he Fuzzy ackng Contol of Output vecto of Double Fed Inducton Geneato DFIG va S Fuzzy Model Fouad Abdelmalk 1 * Najat Ouaalne 1 1 aboatoy of Engneeng, Indutal Management and

More information

Three-axis dynamic modeling of induction motor

Three-axis dynamic modeling of induction motor INERNAIONA JOURNA OF MAHEMAICA MODES AND MEHODS IN APPIED SCIENCES Vole 9, 05 hee-ax dynac odelng of ndcton oto Ya. Dojen,. enbaya and J. evegd Abtact h pape peent a new odelng and laton ethod fo the thee

More information

Modelling Starting Regime Work of the Induction Generators of Wind Turbine and Small Hydroplaning

Modelling Starting Regime Work of the Induction Generators of Wind Turbine and Small Hydroplaning Intenatonal Jounal o Recent Developent n Engneeng and Technology Webte: www.jdet.co (ISSN 47-645(Onlne), Volue, Iue, Decebe 0) Modellng Statng Rege Wok o the Inducton Geneato o Wnd Tubne and Sall Hydoplanng

More information

Chapter 8. Linear Momentum, Impulse, and Collisions

Chapter 8. Linear Momentum, Impulse, and Collisions Chapte 8 Lnea oentu, Ipulse, and Collsons 8. Lnea oentu and Ipulse The lnea oentu p of a patcle of ass ovng wth velocty v s defned as: p " v ote that p s a vecto that ponts n the sae decton as the velocty

More information

Field-oriented Vector Control of Induction Motor for Electric Vehicles

Field-oriented Vector Control of Induction Motor for Electric Vehicles Feld-oented Vecto Contol o Inducton Moto o Electc Vehcle Wang Y Shenzhen Gaduate School Habn Inttute o Technology Shenzhen, Chna Wangy60@yahoo.com.cn Zhao Kaq Automaton College Habn Engneeng Unvety Habn,

More information

DYNAMIC ANALYSIS OF HYSTERESIS MOTOR USING MATLAB/SIMULINK

DYNAMIC ANALYSIS OF HYSTERESIS MOTOR USING MATLAB/SIMULINK DYNAMC ANALYSS OF HYSTSS MOTO USNG MATLAB/SMULNK Moulwaaao eddy P G Scola GM nttute of Tecnology LVSue Atant Pofeo GM nttute of Tecnology Atact-Hytee moto ae elf tatng ule ynconou moto wc ae eng ued wdely

More information

Physics 1501 Lecture 19

Physics 1501 Lecture 19 Physcs 1501 ectue 19 Physcs 1501: ectue 19 Today s Agenda Announceents HW#7: due Oct. 1 Mdte 1: aveage 45 % Topcs otatonal Kneatcs otatonal Enegy Moents of Ineta Physcs 1501: ectue 19, Pg 1 Suay (wth copason

More information

The Suitable Power Control of Wind Energy Conversion System based doubly Fed Induction Generator

The Suitable Power Control of Wind Energy Conversion System based doubly Fed Induction Generator Intenatonal Jounal of Compute Applcaton (975 8887) Volume 87 No.3, Febuay 4 The Sutable Powe Contol of Wnd Enegy Conveon Sytem baed doubly Fed Inducton Geneato D E. eouche Depatment of Electcal Engneeng,

More information

PERFORMANCE ANALYSIS OF DOUBLY- FED INDUCTION GENERATOR FOR WIND ENERGY CONVERSION SYSTEM

PERFORMANCE ANALYSIS OF DOUBLY- FED INDUCTION GENERATOR FOR WIND ENERGY CONVERSION SYSTEM The 5 th PSU-UNS Intenatonal Confeence on Engneeng an 53 Technology (ICET-11), Phuket, May -3, 11 Pnce of Songkla Unety, Faculty of Engneeng Hat Ya, Songkhla, Thalan 911 PEFOMANCE ANALYSIS OF OUBLY- FE

More information

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles /4/04 Chapte 7 Lnea oentu Lnea oentu of a Sngle Patcle Lnea oentu: p υ It s a easue of the patcle s oton It s a vecto, sla to the veloct p υ p υ p υ z z p It also depends on the ass of the object, sla

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

A Generalized Dynamic Model of Induction Motor using Simulink

A Generalized Dynamic Model of Induction Motor using Simulink A Generalzed Dynac Model of Inducton Motor ung Sulnk P. M. Palpankar, R. U. Ghanare & *N. Makade D.B.A.C.E.R, Nagpur *Y.C.C.E, Nagpur E-al : prach_bd@yahoo.co, ghanare.rahul@gal.co, nluakde@gal.co Abtract

More information

(8) Gain Stage and Simple Output Stage

(8) Gain Stage and Simple Output Stage EEEB23 Electoncs Analyss & Desgn (8) Gan Stage and Smple Output Stage Leanng Outcome Able to: Analyze an example of a gan stage and output stage of a multstage amplfe. efeence: Neamen, Chapte 11 8.0) ntoducton

More information

PMSM. Mechanical Design

PMSM. Mechanical Design PMSM Indutial Electical Engineeing and Autoation Lund Univeity, Sweden Mechanical Deign Indutial Electical Engineeing and Autoation 1 Indutial Electical Engineeing and Autoation y i b i β Matheatical Model

More information

gravity r2,1 r2 r1 by m 2,1

gravity r2,1 r2 r1 by m 2,1 Gavtaton Many of the foundatons of classcal echancs wee fst dscoveed when phlosophes (ealy scentsts and atheatcans) ted to explan the oton of planets and stas. Newton s ost faous fo unfyng the oton of

More information

Steady-State Analysis of DFIG for Wind Power Generation System Drive

Steady-State Analysis of DFIG for Wind Power Generation System Drive INTERNATIONAL JOURNAL OF ENERGY, Iue, Vol., SteadyState Analy of DFIG fo Wnd owe Geneaton Syte De Jhène Ben Alaya, Adel Khedhe and Mohaed Faouz Moun Abtact Wnd enegy ha a key ole to play n poducng of clean

More information

EE595S: Class Lecture Notes Chapter 2* / QD Models for Permanent Magnet Synchronous Machines

EE595S: Class Lecture Notes Chapter 2* / QD Models for Permanent Magnet Synchronous Machines EE595S: Class ectue Notes Chapte * / QD Models fo Peanent Magnet Synchonous Machines S.D. Sudhoff Fall 5 *Analysis and Design of Peanent Magnet Synchonous Machines S.D. Sudhoff, S.P. Pekaek B. Fahii .1

More information

CHAPTER 6 VECTOR CONTROL ON DOUBLE OUTPUT INDUCTION GENERATOR FOR VARIABLE SPEED WIND ENERGY CONVERSION SYSTEMS

CHAPTER 6 VECTOR CONTROL ON DOUBLE OUTPUT INDUCTION GENERATOR FOR VARIABLE SPEED WIND ENERGY CONVERSION SYSTEMS CHAPTER 6 VECTOR CONTROL ON DOUBLE OUTPUT INDUCTION GENERATOR FOR VARIABLE SPEED WIND ENERGY CONVERSION SYSTEMS 6.1 Intoucton Woun oto nucton machne ue n vaable pee WECS a hown n fgue 1.4 an 3.6 known

More information

Off-Line Parameter Estimation of Induction Motor Based on a Multitime Scale Approach

Off-Line Parameter Estimation of Induction Motor Based on a Multitime Scale Approach Off-ne Paaete Etaton of Indcton Moto Baed on a Mltte Scale ppoach EXNDU ONE VSIE HOG MIE DIONESU ONEIU BOŢN Depatent of toatc ontol and Indtal Infoatc Depatent of Electc Dve "Gh. ach" echncal Unvety of

More information

Queuing Network Approximation Technique for Evaluating Performance of Computer Systems with Input to Terminals

Queuing Network Approximation Technique for Evaluating Performance of Computer Systems with Input to Terminals 6th Intenatonal Confeence on Chemcal Agcultual Envonmental and Bologcal cence CAEB-7 Dec. 7-8 07 Pa Fance ueung Netwo Appoxmaton Technque fo Evaluatng Pefomance of Compute ytem wth Input to Temnal Ha Yoh

More information

THE EQUIVALENCE OF GRAM-SCHMIDT AND QR FACTORIZATION (page 227) Gram-Schmidt provides another way to compute a QR decomposition: n

THE EQUIVALENCE OF GRAM-SCHMIDT AND QR FACTORIZATION (page 227) Gram-Schmidt provides another way to compute a QR decomposition: n HE EQUIVAENCE OF GRA-SCHID AND QR FACORIZAION (page 7 Ga-Schdt podes anothe way to copute a QR decoposton: n gen ectos,, K, R, Ga-Schdt detenes scalas j such that o + + + [ ] [ ] hs s a QR factozaton of

More information

Recurrence Relations for Single and Product Moments of Generalized Order Statistics from Extreme Value Distribution

Recurrence Relations for Single and Product Moments of Generalized Order Statistics from Extreme Value Distribution Aecan Jonal o Appled Matheatc and Stattc, 204, Vol. 2, No. 2, 77-82 Avalable onlne at http://pb.cepb.co/aa/2/2/5 Scence and Edcaton Pblhng DOI:0.269/aa-2-2-5 Recence Relaton o Sngle and Podct Moent o Genealzed

More information

Fault-Current Study of the Wind-Turbine-Driven Doubly-Fed Induction Generator with the Crowbar Protection

Fault-Current Study of the Wind-Turbine-Driven Doubly-Fed Induction Generator with the Crowbar Protection ELEKTROTEHNIŠKI VESTNIK 8(-): 57-6 ORIGINAL SIENTIFI PAPER Fault-uent Study of the Wnd-Tubne-Dven Doubly-Fed Inducton Geneato wth the owba Potecton Xangpng Kong Zhe Zhang State Key Laboatoy of Advanced

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

Initialization of DFIG based wind generating system

Initialization of DFIG based wind generating system Intalzaton of DFIG bae wn geneatng ytem N.Amutha an B. Kalyan Kuma, membe, IEEE Electcal Engneeng epatment Inan Inttute of Technology Maa Chenna, Ina 636 Emal: namutha@gmal.com, balyan@ee.tm.ac.n Abtact

More information

Physics 207 Lecture 16

Physics 207 Lecture 16 Physcs 07 Lectue 6 Goals: Lectue 6 Chapte Extend the patcle odel to gd-bodes Undestand the equlbu of an extended object. Analyze ollng oton Undestand otaton about a fxed axs. Eploy consevaton of angula

More information

Solving the Dirac Equation: Using Fourier Transform

Solving the Dirac Equation: Using Fourier Transform McNa Schola Reeach Jounal Volume Atcle Solvng the ac quaton: Ung oue Tanfom Vncent P. Bell mby-rddle Aeonautcal Unvety, Vncent.Bell@my.eau.edu ollow th and addtonal wok at: http://common.eau.edu/na Recommended

More information

RISK ANALYSIS ON THE BASIS OF PARTIAL INFORMATION ABOUT QUANTILES

RISK ANALYSIS ON THE BASIS OF PARTIAL INFORMATION ABOUT QUANTILES L Utkn Augutn RISK ANALYSIS ON HE BASIS OF PARIAL INFORAION ABOU QUANILES (Vol) 2008 Decembe RISK ANALYSIS ON HE BASIS OF PARIAL INFORAION ABOU QUANILES Lev V Utkn Depatment of Compute Scence St Petebug

More information

Speed Tracking of a Linear Induction Motor- Enumerative Nonlinear Model Predictive Control

Speed Tracking of a Linear Induction Motor- Enumerative Nonlinear Model Predictive Control Speed Tackng of a nea Inducton Moto- Enumeatve Nonlnea Model Pedctve Contol Jean Thoma and Ande Hanon nköpng Unvety Pot Pnt N.B.: When ctng th wok, cte the ognal atcle. 3 IEEE. Peonal ue of th mateal pemtted.

More information

The Backpropagation Algorithm

The Backpropagation Algorithm The Backpopagaton Algothm Achtectue of Feedfowad Netwok Sgmodal Thehold Functon Contuctng an Obectve Functon Tanng a one-laye netwok by teepet decent Tanng a two-laye netwok by teepet decent Copyght Robet

More information

Numerical Study of Large-area Anti-Resonant Reflecting Optical Waveguide (ARROW) Vertical-Cavity Semiconductor Optical Amplifiers (VCSOAs)

Numerical Study of Large-area Anti-Resonant Reflecting Optical Waveguide (ARROW) Vertical-Cavity Semiconductor Optical Amplifiers (VCSOAs) USOD 005 uecal Sudy of Lage-aea An-Reonan Reflecng Opcal Wavegude (ARROW Vecal-Cavy Seconduco Opcal Aplfe (VCSOA anhu Chen Su Fung Yu School of Eleccal and Eleconc Engneeng Conen Inoducon Vecal Cavy Seconduco

More information

Exam 1. Sept. 22, 8:00-9:30 PM EE 129. Material: Chapters 1-8 Labs 1-3

Exam 1. Sept. 22, 8:00-9:30 PM EE 129. Material: Chapters 1-8 Labs 1-3 Eam ept., 8:00-9:30 PM EE 9 Mateal: Chapte -8 Lab -3 tandadzaton and Calbaton: Ttaton: ue of tandadzed oluton to detemne the concentaton of an unknown. Rele on a eacton of known tochomet, a oluton wth

More information

Small signal analysis

Small signal analysis Small gnal analy. ntroducton Let u conder the crcut hown n Fg., where the nonlnear retor decrbed by the equaton g v havng graphcal repreentaton hown n Fg.. ( G (t G v(t v Fg. Fg. a D current ource wherea

More information

Influence of the rotor resistance change to control performance of an induction machine

Influence of the rotor resistance change to control performance of an induction machine POSTE 2017, PAGUE MAY 23 1 Influence of the oto esstance change to contol pefomance of an nducton machne Tomáš KOŠŤÁ Dept. of Electc Dves and Tacton, Czech Techncal Unvesty, Techncká 2, 166 27 Paha, Czech

More information

Maximum Torque Control of Induction Traction Motor Based on DQ Axis Voltage Regulation

Maximum Torque Control of Induction Traction Motor Based on DQ Axis Voltage Regulation 6th Intenational Confeence on Machiney, Mateials, Envionent, Biotechnology and Copute (MMEBC 016) Maxiu Toque Contol of Induction Taction Moto Based on DQ Axis Voltage Regulation Guo-Bin SUN1,a, Shu-Jia

More information

POWER RATINGS AND LOSSES ESTIMATION OF A SWITCHED RELUCTANCE MOTOR FOR ELECTRIFIED RAILWAY APPLICATIONS

POWER RATINGS AND LOSSES ESTIMATION OF A SWITCHED RELUCTANCE MOTOR FOR ELECTRIFIED RAILWAY APPLICATIONS POER RATIGS AD LOSSES ESTIMATIO OF A SITCHED RELUCTACE MOTOR FOR ELECTRIFIED RAILAY APPLICATIOS Mohammad Shafan Fahad Shahna hafan@tabzuac fahadhahna@yahoocom Cente of Excellence fo Mechatonc, Unvety of

More information

Direct Torque Control of Saturated Doubly-Fed Induction Generator using High Order Sliding Mode Controllers

Direct Torque Control of Saturated Doubly-Fed Induction Generator using High Order Sliding Mode Controllers (IJACSA) Intenatonal Jounal of Avance Compute Scence an Applcaton, Vol. 7, No. 7, 6 Dect Toque Contol of Satuate Doubly-Fe Inucton Geneato ung Hgh Oe Slng Moe Contolle Elhaj BOUNADJA Depatment of Automatc

More information

Lecture Set 6 Brushless DC Machines

Lecture Set 6 Brushless DC Machines Lectue Set 6 Bushless DC Machines S.D. Sudhoff Sping 2018 Reading Chapte 8, Electomechanical Motion Devices, 2 nd Edition 2 A Bushless DC Machine 3 Sample Applications Low Powe: Disk dive motos Medium

More information

24-2: Electric Potential Energy. 24-1: What is physics

24-2: Electric Potential Energy. 24-1: What is physics D. Iyad SAADEDDIN Chapte 4: Electc Potental Electc potental Enegy and Electc potental Calculatng the E-potental fom E-feld fo dffeent chage dstbutons Calculatng the E-feld fom E-potental Potental of a

More information

Root Locus Techniques

Root Locus Techniques Root Locu Technque ELEC 32 Cloed-Loop Control The control nput u t ynthezed baed on the a pror knowledge of the ytem plant, the reference nput r t, and the error gnal, e t The control ytem meaure the output,

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

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints. Mathematcal Foundatons -1- Constaned Optmzaton Constaned Optmzaton Ma{ f ( ) X} whee X {, h ( ), 1,, m} Necessay condtons fo to be a soluton to ths mamzaton poblem Mathematcally, f ag Ma{ f ( ) X}, then

More information

Simulation of the Performance of Induction Machine under Unbalanced Source Voltage Conditions.

Simulation of the Performance of Induction Machine under Unbalanced Source Voltage Conditions. Sulaton of the efoance of Inducton Machne unde Unalanced Souce oltage Condton. E.J. Akaa, M.Eng. 1 ; O.I. Okoo, h.d. 2 ; and E. Chkun, h.d. 3 1 Deatent of Electcal/Electonc Engneeng, Co ve Unvety of Technology,

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

Summary 7. ELECTROMAGNETIC JOINT. ROTATING MAGNETIC FIELD. SPACE-PHASOR THEORY... 2

Summary 7. ELECTROMAGNETIC JOINT. ROTATING MAGNETIC FIELD. SPACE-PHASOR THEORY... 2 uay 7. ELECTROMAGETIC JOIT. ROTATIG MAGETIC FIELD. PACE-PHAOR THEORY... 7.1 ELECTROMAGETIC JOIT... 7. UMER OF POLE... 4 7. DITRIUTED WIDIG... 5 7.4 TORQUE EXPREIO... 6 7.5 PACE PHAOR... 7 7.6 THREE-PHAE

More information

CHAPTER 5 DESIGN OF SPEED CONTROLLER FOR CONVERTER FED PERMANENT MAGNET SYNCHRONOUS MOTOR DRIVE

CHAPTER 5 DESIGN OF SPEED CONTROLLER FOR CONVERTER FED PERMANENT MAGNET SYNCHRONOUS MOTOR DRIVE 8 CHAPER 5 DESIN OF SPEED CONROLLER FOR CONVERER FED PERMANEN MANE SYNCHRONOUS MOOR DRIVE 5. INRODUCION he Penent Mgnet Synchonou Moto PMSM develop nuodl bck ef Pfff et l 98 etblhng telf eou copetto to

More information

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems Engneeng echancs oce esultants, Toques, Scala oducts, Equvalent oce sstems Tata cgaw-hll Companes, 008 Resultant of Two oces foce: acton of one bod on anothe; chaacteed b ts pont of applcaton, magntude,

More information

CHAPTER 4 TWO-COMMODITY CONTINUOUS REVIEW INVENTORY SYSTEM WITH BULK DEMAND FOR ONE COMMODITY

CHAPTER 4 TWO-COMMODITY CONTINUOUS REVIEW INVENTORY SYSTEM WITH BULK DEMAND FOR ONE COMMODITY Unvety of Petoa etd Van choo C de Wet 6 CHAPTER 4 TWO-COMMODITY CONTINUOU REVIEW INVENTORY YTEM WITH BULK DEMAND FOR ONE COMMODITY A modfed veon of th chapte ha been accepted n Aa-Pacfc Jounal of Opeatonal

More information

9/12/2013. Microelectronics Circuit Analysis and Design. Modes of Operation. Cross Section of Integrated Circuit npn Transistor

9/12/2013. Microelectronics Circuit Analysis and Design. Modes of Operation. Cross Section of Integrated Circuit npn Transistor Mcoelectoncs Ccut Analyss and Desgn Donald A. Neamen Chapte 5 The pola Juncton Tanssto In ths chapte, we wll: Dscuss the physcal stuctue and opeaton of the bpola juncton tanssto. Undestand the dc analyss

More information

Physics Exam II Chapters 25-29

Physics Exam II Chapters 25-29 Physcs 114 1 Exam II Chaptes 5-9 Answe 8 of the followng 9 questons o poblems. Each one s weghted equally. Clealy mak on you blue book whch numbe you do not want gaded. If you ae not sue whch one you do

More information

Chapter Fifiteen. Surfaces Revisited

Chapter Fifiteen. Surfaces Revisited Chapte Ffteen ufaces Revsted 15.1 Vecto Descpton of ufaces We look now at the vey specal case of functons : D R 3, whee D R s a nce subset of the plane. We suppose s a nce functon. As the pont ( s, t)

More information

LECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12

LECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12 CTU 4 ] NWTON W O GVITY -The gavity law i foulated fo two point paticle with ae and at a ditance between the. Hee ae the fou tep that bing to univeal law of gavitation dicoveed by NWTON. a Baed on expeiental

More information

ECEN474/704: (Analog) VLSI Circuit Design Spring 2018

ECEN474/704: (Analog) VLSI Circuit Design Spring 2018 EEN474/704: (Anal) LSI cut De S 08 Lectue 8: Fequency ene Sa Pale Anal & Mxed-Sal ente Texa A&M Unety Annunceent & Aenda HW Due Ma 6 ead aza hate 3 & 6 Annunceent & Aenda n-suce A Fequency ene Oen-cut

More information

PARAMETER OPTIMIZATION IN THE DESIGN OF A GRID-SIDE CONVERTER CONTROLLER IN THE LIGHT OF GRID FAULTS

PARAMETER OPTIMIZATION IN THE DESIGN OF A GRID-SIDE CONVERTER CONTROLLER IN THE LIGHT OF GRID FAULTS IJRRAS 9 () Octobe www.apape.com/volume/vol9iue/ijrras_9 8.pdf PARAMETER OPTIMIZATION IN THE DESIGN OF A GRIDSIDE CONVERTER CONTROLLER IN THE LIGHT OF GRID FAULTS C.A. Nwou & C.U. Ogbua Depatment of Electcal

More information

Quick Visit to Bernoulli Land

Quick Visit to Bernoulli Land Although we have een the Bernoull equaton and een t derved before, th next note how t dervaton for an uncopreble & nvcd flow. The dervaton follow that of Kuethe &Chow ot cloely (I lke t better than Anderon).

More information

A Novel Method for Modeling Magnetic Saturation in the Main Flux of Induction Machine

A Novel Method for Modeling Magnetic Saturation in the Main Flux of Induction Machine Poceeding of the 5th WSEAS Int. Conf. on Syte Science and Siulation in Engineeing, Teneife, Canay Ilan, Spain, Decebe 16-18, 2006 150 A Novel Method fo Modeling Magnetic Satuation in the Main Flux of Induction

More information

HYSTERESIS BASED ON ARTIFICIAL INTELLIGENCE TECHNIQUES OF SIX SECTORS DTC WITH VOLTAGE ZERO FOR INDUCTION MACHINE

HYSTERESIS BASED ON ARTIFICIAL INTELLIGENCE TECHNIQUES OF SIX SECTORS DTC WITH VOLTAGE ZERO FOR INDUCTION MACHINE Algean Jounal of Reeach and echnology (AJR) Volume 2 Iue (Decembe 27) Algean Jounal of Reeach and echnology AJRDZ@gmalcom http://wwwunv-utodz/ajr/ ISSN (Pnt):2543-3946, ISSN (onlne):2543-3954 AJR Volume

More information

Dynamics and Control of Electrical Drives

Dynamics and Control of Electrical Drives Dnac and Contol of Electcal Dve Pot Wach Dnac and Contol of Electcal Dve ABC Autho Pof. Pot Wach Poltechna Opola Inttute of Electoechancal Ste and Appled Infoatc Mołajcza 5 t. 45-7 Opole Poland E-al: p.wach@po.opole.pl

More information

Dynamics and Control of Electrical Drives

Dynamics and Control of Electrical Drives Dnac and Contol of Electcal Dve Pot Wach Dnac and Contol of Electcal Dve ABC Autho Pof. Pot Wach Poltechna Opola Inttute of Electoechancal Ste and Appled Infoatc Mołajcza 5 t. 45-7 Opole Poland E-al:

More information

The Dynamic Modelling and Electrical Profiles of Three Phase Induction Motor Using MATLAB Program

The Dynamic Modelling and Electrical Profiles of Three Phase Induction Motor Using MATLAB Program nnovatve Sytem Degn an Engneeng SSN -177 ape SSN -871 Onlne ol.6 No.1 15 www.te.og he Dynamc oellng an Electcal ofle of hee hae nucton oto Ung AAB ogam E.S. Oluwaogo 1* O.D. Oune A.K. Babane.K. Okakwu

More information

Bayesian and Frequentist Prediction Using Progressive Type-II Censored with Binomial Removals

Bayesian and Frequentist Prediction Using Progressive Type-II Censored with Binomial Removals Intellgent Infoaton Manageent 3 5 6-7 http://dxdoog/436/3557 Publhed Onlne eptebe 3 (http://wwwcpog/jounal/) Bayean Fequentt Pedcton Ung Pogeve Type-II Cenoed w Bnoal Reoval Ahed A olan Ahed H Abd Ellah

More information

CSE-571 Robotics. Ball Tracking in RoboCup. Tracking Techniques. Rao-Blackwelized Particle Filters for State Estimation

CSE-571 Robotics. Ball Tracking in RoboCup. Tracking Techniques. Rao-Blackwelized Particle Filters for State Estimation CSE-571 Rootcs Rao-Blacwelzed Patcle Fltes fo State Estaton Ball Tacng n RooCup Exteely nosy nonlnea oton of oseve Inaccuate sensng lted pocessng powe Inteactons etween taget and Goal: envonent Unfed faewo

More information

GENERALIZATION OF AN IDENTITY INVOLVING THE GENERALIZED FIBONACCI NUMBERS AND ITS APPLICATIONS

GENERALIZATION OF AN IDENTITY INVOLVING THE GENERALIZED FIBONACCI NUMBERS AND ITS APPLICATIONS #A39 INTEGERS 9 (009), 497-513 GENERALIZATION OF AN IDENTITY INVOLVING THE GENERALIZED FIBONACCI NUMBERS AND ITS APPLICATIONS Mohaad Faokh D. G. Depatent of Matheatcs, Fedows Unvesty of Mashhad, Mashhad,

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

A high performance svm-dtc scheme for induction machine as integrated starter generator in hybrid electric vehicles

A high performance svm-dtc scheme for induction machine as integrated starter generator in hybrid electric vehicles 41 Natue & echnology A hgh pefomance m-c che fo nducton machne a ntegated tate geneato n hybd electc ehcle Mohamed Bounadja, a Ahmed Wahd Belab, b Bach Belmadan a a Depatment of Electotechnc, Unety Haba

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

Chapter 5: Root Locus

Chapter 5: Root Locus Chater 5: Root Locu ey condton for Plottng Root Locu g n G Gven oen-loo tranfer functon G Charactertc equaton n g,,.., n Magntude Condton and Arguent Condton 5-3 Rule for Plottng Root Locu 5.3. Rule Rule

More information

Characterizations of Slant Helices. According to Quaternionic Frame

Characterizations of Slant Helices. According to Quaternionic Frame Appled Mathematcal Scence, Vol. 7, 0, no. 75, 79-78 HIKARI Ltd, www.m-hka.com http://dx.do.og/0.988/am.0.557 Chaactezaton of Slant Helce Accodng to Quatenonc Fame Hüeyn KOCAYİĞİT and Beyza Betül PEKACAR

More information

Sensorless Speed Control of Induction Motor Using MRAS

Sensorless Speed Control of Induction Motor Using MRAS Intenatonal Jounal of Recent Technology and Engneeng (IJRTE) ISSN: 2277-3878, Volume-1, Iue-5, Noembe 2012 Senole Speed Contol of Inducton Moto Ung MRAS G. Pydaju, M. Daaaadam Abtact : In ode to mplement

More information

Addition of Angular Momentum

Addition of Angular Momentum Addition of Angula Moentu We ve leaned tat angula oentu i ipotant in quantu ecanic Obital angula oentu L Spin angula oentu S Fo ultielecton ato, we need to lean to add angula oentu Multiple electon, eac

More information

Detection and Estimation Theory

Detection and Estimation Theory ESE 54 Detecton and Etmaton Theoy Joeph A. O Sullvan Samuel C. Sach Pofeo Electonc Sytem and Sgnal Reeach Laboatoy Electcal and Sytem Engneeng Wahngton Unvety 411 Jolley Hall 314-935-4173 (Lnda anwe) jao@wutl.edu

More information

SLIDING MODE APPLICATION IN SPEED SENSORLESS TORQUE CONTROL OF AN INDUCTION MOTOR

SLIDING MODE APPLICATION IN SPEED SENSORLESS TORQUE CONTROL OF AN INDUCTION MOTOR Copyght IFAC 15th ennal Wol Conge, Bacelona, Span SLIDING MODE APPLICAION IN SPEED SENSORLESS ORQUE CONROL OF AN INDUCION MOOR Kael Jezenk 1, Man Roč 1, Af Šabanovć 1 Unvety of Mabo, Faculty of Electcal

More information

AGC Introduction

AGC Introduction . Introducton AGC 3 The prmary controller response to a load/generaton mbalance results n generaton adjustment so as to mantan load/generaton balance. However, due to droop, t also results n a non-zero

More information

19 The Born-Oppenheimer Approximation

19 The Born-Oppenheimer Approximation 9 The Bon-Oppenheme Appoxmaton The full nonelatvstc Hamltonan fo a molecule s gven by (n a.u.) Ĥ = A M A A A, Z A + A + >j j (883) Lets ewte the Hamltonan to emphasze the goal as Ĥ = + A A A, >j j M A

More information

Rigid Bodies: Equivalent Systems of Forces

Rigid Bodies: Equivalent Systems of Forces Engneeng Statcs, ENGR 2301 Chapte 3 Rgd Bodes: Equvalent Sstems of oces Intoducton Teatment of a bod as a sngle patcle s not alwas possble. In geneal, the se of the bod and the specfc ponts of applcaton

More information

XII.3 The EM (Expectation-Maximization) Algorithm

XII.3 The EM (Expectation-Maximization) Algorithm XII.3 The EM (Expectaton-Maxzaton) Algorth Toshnor Munaata 3/7/06 The EM algorth s a technque to deal wth varous types of ncoplete data or hdden varables. It can be appled to a wde range of learnng probles

More information

Energy in Closed Systems

Energy in Closed Systems Enegy n Closed Systems Anamta Palt palt.anamta@gmal.com Abstact The wtng ndcates a beakdown of the classcal laws. We consde consevaton of enegy wth a many body system n elaton to the nvese squae law and

More information

Sensorless A.C. Drive with Vector Controlled Synchronous Motor

Sensorless A.C. Drive with Vector Controlled Synchronous Motor Seole A.C. Dve wth Vecto Cotolle Sychoo Moto Ořej Fše VŠB-echcal Uvety of Otava, Faclty of Electcal Egeeg a Ifomatc, Deatmet of Powe Electoc a Electcal Dve, 17.ltoa 15, 78 33 Otava-Poba, Czech eblc oej.fe@vb.cz

More information

1 cos. where v v sin. Range Equations: for an object that lands at the same height at which it starts. v sin 2 i. t g. and. sin g

1 cos. where v v sin. Range Equations: for an object that lands at the same height at which it starts. v sin 2 i. t g. and. sin g SPH3UW Unt.5 Projectle Moton Pae 1 of 10 Note Phc Inventor Parabolc Moton curved oton n the hape of a parabola. In the drecton, the equaton of oton ha a t ter Projectle Moton the parabolc oton of an object,

More information

Section Induction motor drives

Section Induction motor drives Section 5.1 - nduction motor drive Electric Drive Sytem 5.1.1. ntroduction he AC induction motor i by far the mot widely ued motor in the indutry. raditionally, it ha been ued in contant and lowly variable-peed

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