*<D]ÕúPDODUÕQ\DSÕODFD÷Õ\D]DU Sevcan $\WDo.RUNPD], sevcanaytackorkmaz@gmail.com, Tel: 05067927759
6RQOXHOHPDQODU\|QWHPLLOH asenkron motor analizi ve
motorXQIDUNOÕND\PDGH÷HUOHULQHJ|UH momentinin
matlab programlama dili ile hesaplanmasÕ
Sevcan AYTAÇ KORKMAZ1*
,
Hasan KÜRÜM21 )ÕUDWhQLYHUVLWHVLMaden MYO, (/$=,ö
2 )ÕUDWhQLYHrsitesi, 0KHQGLVOLN)DNOWHVL Elektrik-(OHNWURQLN0KHQGLVOL÷L%|OP(/$=,ö
Özet
Bu makalede, VRQOX HOHPDQODU \|QWHPL 6(< NXOODQÕODUDN DVHQNURQ PRWRUXQ matlab SURJUDPÕQGDQ \DUDUODQDUDN o|]P E|OJHVLQGH PDJQHWLN YHNW|U SRWDQVL\HO YH PDJQHWLN DNÕ \R÷XQOX÷XGH÷LúLPOHULLQFHOHQLSPDQ\HWLNE\NONOHUKHVDSODQPÕúWÕU Ek olarak, enerji ve moment GH÷HUOHUL KHVDSODQDUDN GHQH\VHO VRQXoODUOD NDUúÕODúWÕUÕOPÕúWÕU %XQXQ LoLQ 0DWODE SURJUDPODPD GLOLNXOODQÕODUDNELUSURJUDPJHOLúWLULOPLúWLU BXoDOÕúPDQÕQsonucunda GH÷LúLNND\PDGH÷HUOHULQH J|UHHOGHHGLOHQPRPHQWE\NONOHULQLQGHQH\VHOoDOÕúPDODUDoRN \DNÕQVRQXoODUYHUGL÷L, matlab SURJUDPÕ VD\HVLQGH J|UOPúWU <DSÕODQ OLWHUDWU WDUDPDVÕQGD QHVQHO WDEDQOÕ ELU SURJUDPODPD GLOL LOH \DSÕODQ DQDOL]OHULQ daha uzun NRPXW VDWÕUODUÕ\OD \DSÕOGÕ÷Õ J|UOS PDWODE LOH \DSÕODQ analizlerde daha NÕVDNRPXWVDWÕUODUÕNXOODQÕOPÕúWÕU.
Anahtar Kelimeler: Asenkron Motor, 6RQOX(OHPDQODU<|QWHPL Matlab
mühendislikdergisi
Cilt: 3-9
Dicle Üniversitesi Mühendislik Fakültesi .DV×P4, ,
Calculating momentum with matlab
programming language according to
values of different slip of motor and
induction motor analysis with finite
element method
Extended abstract
In this article, we will focus on the analysis of
an induction motor with finite element method. By using finite element method (FEM) calculation of energy and moment of induction motor is described. Aspects of being robust, requiring little maintenance, the low cost, not being affected by environmental conditions and their power per unit volume induction motors are superior to other motors and can be used in almost every field. Motor analyzed have 18 stator and 22 rotor. The air gap between stator and rotor is 0.5mm. Enameled copper conductors have diameter 2*0.55mm and winded as 47 windings. The finite element method generally can be explained from these stages: Giving node and element numbers, Division of the solution area, solution area is separated to areas and element numbers are given, Generation of coefficient matrix, Put known values of vector potential and excitations (current etc.) into problem, Solution of systems of equation and finding potential at nod points, Calculation of other quantities from calculated potential values. In finite element method initially solution area is divided small triangle
elements. In numerical calculation it is essential and expresses approximate solution. In this study, the magnetic vector potential and magnetic flux density changes have investigated in the solution of the induction motor using finite element method (FEM). Additionaly, calculated energy and momentum values , are compared with experimental results. For this, a program is developed using Matlab programming language. The induction motor (6A, 380V) is designed and constructed for this study has 7.45 Nm torque value is obtained from experimental studies.
Half of the motor according to the study of symmetry is discussed, so calculated value of moment multiplied by 2. In this case, the moment was 7.78 Nm. About 4.4% of error derived from negligence in the finite element method, experimental errors in measuring device is used in this study and etc. The momentum sizes that obtained from this study have a high degree of accuracy than literature examination. In addition, MATLAB software provides easy programming and advanced graphics features. Ready function takes many lines in programming languages, but it can be prepared in only a few lines by MATLAB program than literature examination (Polat ve Kürüm, 2011). Because of these advantages MATLAB programming language should be used during the analysis of an induction motor. As a conclusion, designing induction motor by using finite element method, gives better result.
Keywords: Induction Motor, Finite element
GLULú
Bu makalede, bir asenkron motorun sonlu elemanlar yöntemi ile analizi üzerinde GXUXODFDNWÕU$VHQNURQPRWRUXQVRQOXHOHPDQODU \|QWHPL 6(< NXOODQÕODUDN magnetik enerji ve PRPHQWKHVDEÕ DQODWÕOPÕúWÕU%XNRQXGD0DWODE programlama dilinde bir bilgLVD\DU SURJUDPÕ JHOLúWLULOPLúYHEXSURJUDPLOHPRWRUXQHQHUMLYH PRPHQW GH÷HUOHUL KHVDSODQDUDN ELU DVHQNURQ PRWRUXQSHUIRUPDQVDQDOL]L\DSÕOPÕúWÕU
Asenkron motor
$VHQNURQPRWRUODUVD÷ODPROPDVÕD]EDNÕP JHUHNWLUPHVLPDOL\HWLQLQGúNROPDVÕoHYUHVHO NRúXOODUGDQ HWNLOHQPHPHOHUL YH ELULP KDFLP EDúÕQD YHUGLNOHUL Jo EDNÕPÕQGDQ GL÷HU PRWRUODUD VWQON VD÷ODPDNWDGÕUODU YH KHPHQ KHPHQ KHU DODQGD NXOODQÕODELOPHNWHGLU. Analizi \DSÕODQ PRWRU ùHNLO ¶GH J|UOG÷ JLEL VWDWRUURWRUROX÷XQDVDKLSWLU6WDWor ile rotor DUDVÕQGDNLKDYDDUDOÕ÷ÕPP¶GLU
ùHNLO1. $QDOL]L\DSÕODQ motorXQ|QGHQ
J|UQú 6WDWRUVDUÕPúHPDVÕ
øQFHOHPHVL \DSÕODQ o ID]OÕ DVHQNURQ PRWRU \DUÕP NDOÕS RODUDN VDUÕOPÕú YH VDUÕP úHPDVÕ ùHNLO ¶GH YHULOPLúWLU 0RWRU <ÕOGÕ] ED÷ODQPÕúWÕU .XOODQÕODQ HPD\H NDSOÕ EDNÕU LOHWNHQOHULQ oDSÕ PP ROXS VDUÕP RODUDNVDUÕOPÕúWÕU
ùHNLO2. 6WDWRUVDUÕPúHPDVÕ
0RWRUGD.XOODQÕODQ0DWHU\DOOHULQ 7DQÕPODQPDVÕ
Motorun analizinde 5 materyal modeli NXOODQÕOPÕúWÕU 1-Hava 2-Silisyumlu sDoVWDWRUYHURWRU 3-6WDWRUEDNÕUVDUJÕ 4-5RWRUDOPLQ\XPVDUJÕ 5-Rotor mili ùHNLO 0DWHU\DOWUOHULQHJ|UHPRWRU geometrisi
6RQOXHOHPDQODU\|QWHPL
6RQOX HOHPDQODU \|QWHPLQGH LON DúDPD RODUDN o|]P E|OJHVL NoN oJHQ HOHPDQODUD E|OQU 1PHULN KHVDSODPDODUGD EX úDUW ROXS \DNODúÕNo|]PLIDGHHGHUhoJHQOHUHE|OQHQ EX HOHPDQODUÕQ LNL ER\XWOX DQDOL]LQLQ \DSÕOPDVÕ HVQDVÕQGD DODQODUÕQÕQ o ER\XWOX DQDOL]LQLQ \DSÕOPDVÕ HVQDVÕQGD LVH KDFLPOHULQLQ
KHVDSODPDODUD NDWÕOPDVÕQGDQ GROD\Õ DODQ YH hacim hHVDSODPDODUÕQÕQNROD\ \DSÕODELOHFH÷L YH o|]P E|OJHVLQLQ VÕQÕUODUÕQÕ ER]PD\DFDN HOHPDQODUD E|OQPHVL HVDV DOÕQÕU (÷ULVHO VÕQÕUODUÕVD÷OD\DELOPHVLQHGHQL\OHHQoRNoJHQ YH WHWUDKHGURQ HOHPDQODU WHUFLK HGLOLU d|]P E|OJHVLQLQ PPNQ ROGX÷X NDGDU NoN elePDQODUD E|OQPHVL YH YHNW|U SRWDQVL\HO GH÷LúLPOHULQLQ ID]OD ROGX÷X NÕVÕPODUÕQ GDKD NoN HOHPDQODUD E|OQPHVL o|]PQ GR÷UXOX÷XQX DUWÕUPDNWDGÕU (Chari ve Silvester, 1970).
Sonlu elemanlar yöntemi teorisi
Sonlu elemanODU \|QWHPL /DSODFH GHQNOHP (1) ve Poission denklem (2) WLSL NÕVPÕ WUHYOL GLIHUDQVL\HO GHQNOHPOHULQ o|]POHrinde NXOODQÕODQELU\|QWHPGLU6HOoXN 0 2 2 2 2 w w w w y x I I (1) ) , ( 2 2 2 2 y x f y x w w w wI I (2) Sonlu elemanlar ve rayleigh-ritz yöntemi 6RQOX HOHPDQODU \|QWHPLQLQ HVDVÕ NDUPDúÕN VÕQÕUNRúXOODUÕQHGHQL\OHWPo|]PE|OJHVLLoLQ ELU SRWDQVL\HO IRQNVL\RQX EXOPDQÕQ PPNQ ROPDGÕ÷Õ GXUXPODUGD o|]PQ VRQOX NoN HOHPDQODU LoLQGH DUDQPDVÕQD GD\DQÕU d|]P LoLQ HOHPDQODUÕQ JHRPHWULN \DSÕVÕ D\QÕ NDOPDN NRúXOX LOH WP o|]P E|OJHVL D\QÕ JHRPHWULN HOHPDQODUD E|OQU %X oDOÕúPDGD oJHQ HOHPDQODUNXOODQÕOPÕúWÕU
ùHNLO 4. %LUoJHQHOHPDQÕ
%X \|QWHPOHo|]P \DSDUNHQLONRODUDNELU GHQHPH IRQNVL\RQX VHoLOLr. Bu fonksiyon alan GH÷LúLPLQLLIDGHHGHU(Silvester vd., 1973).
Bu deneme fonksiyonunun birinci dereceden SROLQRP NÕVPÕ denklem (3) oR÷X SUREOHPGH \HWHUOLKDVVDVL\HWLVD÷ODU y x y x, ) 0 1 2 ( D D D I (3) Bu deneme fonksiyonunda I[YH\\HJ|UH GR÷UXVDO ELU úHNLOGH GH÷LúPHNWHGLU (÷HU oJHQLQ N|úHOHULQGHNL SRWDQVL\HOOHU Ii ,Ij ,Im LVHGHQHPHIRQNVL\RQXEXN|úHQRNWDODUÕQGDEX GH÷HUOHUL VD÷ODPDN ]RUXQGDGÕU %X QHGHQOH DúD÷ÕGDNLLIDGHOHU\D]ÕODELOLU i i i D0 D1x D2y I j j j D0 D1x D2y I m m m D0 D1x D2y I (4) (OH DOÕQDQ GHQHPH IRQNVL\RQXQX oJHQOHULQ N|úH Ii ,Ij ,Im GH÷HUOHUL LOH GHQNOHP 4)¶GH YHULOGL÷L úHNLOGH LIDGH HWPHN LoLQ Ni ,Nj ,Nm úHNLOYH\DHQWHUSRODV\RQIRQNVL\RQODUÕNXOODQÕOÕU (Chari, 1973).
xy Nixy Ii Nj
xy Ij Nm
xy Im
I , , , , (5)
+HU ELU oJHQ HOHPDQ LoLQGH SRWDQVL\HO fonksiyonunun Laplace diferansiyel denklemini VD÷ODGÕ÷Õ YDUVD\ÕOGÕ÷ÕQGDQ KRPRMHQ VÕQÕU NRúXOODUÕQGD /DSODFH GHQNOHPLQH NDUúÕOÕN JHOHQ fonksiyonel dy 2 2 dx y x F ³³ w w w w » » ¼ º « « ¬ ª ¸¸ ¹ · ¨¨ © § ¸ ¹ · ¨ © § I I (6) úHNOLQGHLIDGHHGLOHELOLU » » » ¼ º « « « ¬ ª » » » ¼ º « « « ¬ ª » » » ¼ º « « « ¬ ª 0 0 0 2 m j i mm mj mi jm jj ji im ij ii S S S S S S S S S I I I (7) HOGH HGLOLU ùHNLOGH YHULOGL÷L KDOL\OH Ii gi VÕQÕUNRúXOXPDWULVLQLONVDWÕUÕQD\HUOHúWLULOLUVH » » » ¼ º « « « ¬ ª » » » ¼ º « « « ¬ ª » » » ¼ º « « « ¬ ª 0 0 0 0 1 i m j i mm mj mi jm jj ji g S S S S S S I I I (8)
ve bu matrisi düzenlersek » ¼ º « ¬ ª » ¼ º « ¬ ª » ¼ º « ¬ ª mi i ji i m j mm mj jm jj S g S g S S S S I I (9) elde edilir (Demirchian vd., 1976).
(OHPDQODUÕQ%LUOHúWLULOPHVL
d|]P DUDQDQ SRWDQVL\HO LúOHYLQLQ WP E|OJH LoLQGH HOHPDQODU DUDVÕQGDNL VÕQÕUODUGD VUHNOL ROPDVÕ JHUHNLU %LU oJHQ HOHPDQÕQ LoLQGH YH NHQDUODUÕQGD SRWDQVL\HO GR÷UXVDO RODUDNGH÷LúLUBoldea, 2002).
ùHNLO. øNLoJHQHOHPDQÕQELUOHúLPL
3UREOHPLQ WDELDWÕ JHUH÷L ED]Õ G÷POHUGH DNÕP RODELOLU %X GXUXPGD GHQNOHP VLVWHPL úX úHNLOGHG]HQOHQLU ' » » » » ¼ º « « « « ¬ ª » » » » ¼ º « « « « ¬ ª » » » » » ¼ º « « « « « ¬ ª 3 / 0 3 / 0 0 0 4 2 4 3 2 1 )2 ( 44 )2 ( 43 )2 ( 41 )2 ( 34 )2 ( 33 )1 ( 33 )1 ( 32 )2 ( 31 )1 ( 31 )1 ( 23 )1 ( 22 )1 ( 21 )2 ( 14 )2 ( 13 )1 ( 13 )2 ( 12 )2 ( 11 )1 ( 11 J J S S S S S S S S S S S S S S S S S S I I I I (10) '÷POHUGHNLDNÕP\R÷XQOXNODUÕGHQNOHPLQ GLUHN RODUDN VD÷ WDUDIÕQD \D]ÕOÕU Denklem VLVWHPL o|]OG÷QGH KHU G÷P LoLQ SRWDQVL\HOGH÷HUOHULEHOOLROXU
Poisson Denklemlerinin Elde Edilmesi Manyetik alan problemlerinde Maxwell GHQNOHPOHULNXOODQÕOÕU o o u H J (11) o o H B P (12) 0 oB (13) P Q 1 (14) +0DQ\HWLNDODQúLGGHWL$WP %0DQ\HWLNLQGNVL\RQ7 μ=Manyetik permabilite, v= Manyetik rezistivitedir. o o u A B (15) %XUDGD $ 9HNW|U SRWDQVL\HO ROXS ELULPL Wb/m'dir. Denklem (11)’de H yerine denklem o (¶GHNL HúLWOLN NRQXOGX÷XQGD GHQNOHP (13) elde edilir. Bu denklemde B yerine denklem (15¶GHNL HúLWOLN NRQXOGX÷XQGD GHQN 17) elde edilir. Bu denklem, denklem (18)’de G]HQOHQGL÷LQGH GHQNOHP 11) Poisson denklemi elde edilir.
o o u B J P (16) o o u u A J P (17) o ¸¸ ¹ · ¨¨ © § w w w w J y A x A 2 2 2 2 Q (18) øNL ER\XWOXVRQOXHOHPDQODU \|QWHPL DQDOL]L \DSÕOÕUNHQGHQNOHP18)’deNL-DNÕP\R÷XQOX÷X ] HNVHQLQGH ROGX÷X LoLn, manyetik vektör potansiyel A(x,y)=Az(x,y) olur.
0DQ\HWLNøQGNVL\RQXQ+HVDEÕ
'R\PDGDQ GROD\Õ HOGH HGLOHQ 3RLVVRQ GHQNOHPLQGHNL PDQ\HWLN SHUPDELOLWH $ YHNW|U potansiyelin bir fonksiyonudur. Bu durum SRLVVRQ GHQNOHPLQLQ QRQOLQHHU ROPDVÕQD \RO DoDU d|]P \DSÕOÕUNHQ $ YHNW|U SRWDQVL\HO GH÷HUOHUL EXOXQGXNWDQ VRQUD %x ve By GH÷HUOHUL
denklem (20)’de ve (22¶GH verilen GHQNOHPOHUOHKHVDSODQÕU
x,y rotA
x,y
HúLWOL÷LQLDoWÕ÷ÕPÕ]]DPDQ
»»» » » ¼ º « « « « « ¬ ª w w w w w w o o o y x A z y x k j i y x B , 0 0 , (19)
y y x A B z x w w , i i j j m m x c A c A c A B ' 2 1 (20)
x y x A B z y w w , (21) i i j j m m y b A b A b A B ' 2 1 (22)
ROXU 7RSODP DNÕ \R÷XQOX÷X LVH GHQNOHP (23)¶GHNLJLELEXOXQXU.
, 2 2 y x B B y x B (23) d|]P VRQXFXQGD HOGH HGLOHQ % GH÷HUOHUL YH\D $ GH÷HUOHUL ELU |QFHNL KHVDSODQDQ GH÷HUOHUOH NDUúÕODúWÕUÕOÕU $UDODUÕQGD NDEXO edilebiOLU ELU IDUN ROXQFD\D NDGDU EX LúOHPH devam edilir.
0DQ\HWLN$NÕ<ROXdL]LPL
0DQ\HWLN\DSÕQÕQDNÕ\ROXúHPDVÕPDQ\HWLN
E|OJHQLQ VRQOX HOHPDQODU \|QWHPL\OH \DSÕODQ o|]POHULQ VRQXFXQGD HOGH HGLOHQ G÷POHULQ YHNW|Upotansiyel GH÷HUOHULQHJ|UHoL]LOHEilmektedir.
xy x y
A , D0D1 D2 (24)
ùHNLO. Av QRNWDVÕQÕQYHNW|USRWDQVL\HOLQLQ
EXOXQPDVÕ
ùHNLO ¶GD oL]LOHFHN YHNW|U SRWDQVL\HO GH÷HULQLQ$i ve Am GH÷HUOHULDUDVÕQGDROGX÷XQX
kabul edersek Av YHNW|U SRWDQVL\HO GH÷HULQin
yerini Denklem (25¶GHQEXODELOLUL]
m i v i m i v i A A A A x x x x (25) %X HúLWOLNWH x GÕúÕQGD EWQ GH÷HUOHUv
ELOLQGL÷LQH J|UH x ¶\L oHNHUVHN GHQNOHPv
(26)¶\Õ HOGHHWPLúROXUX]
m i v i m i i v A A A A x x x x ( ) (26)Denklem (26)¶GDNL EX HúLWOLN D\QÕ ]DPDQGD
v y LoLQGHJHoHUOLGLU
m i v i m i i v A A A A y y y y ( ) (27) 0DJQHWLN(QHUMLYHøQGNWDQVÕQ+HVDEÕ 0DJQHWLN HQHUMLQLQ KHVDSODQDELOPHVL LoLQ|QFH KHU ELU oJHQ HOHPDQÕQ PDQ\HWLN LQGNVL\RQ GH÷HUL DODQÕ YH PDQ\HWLN SHUPDELOLWHVL KHVDSODQPDOÕGÕU øODYHWHQ PRWRUXPX]XQ \NVHNOL÷L GH JHUHNLU 3URJUDPÕPÕ]GD HQHUMLQLQ EDúODQJÕo GH÷HUL VÕIÕU DOÕQPÕúWÕU +HU ELU oJHQ HOHPDQÕQ HQHUMLVL denklem (¶GHn teker teker hesaplanarak ELUELUOHUL LOH WRSODQPÕú YH WRSODP HQHUML EXOXQPXúWXU
P * 2 * * 2 Alan Yükseklik B Enerji Magnetik (28)Denklem (¶GHNL HúLWOLNWHQ ID\GDODQDUDN \DSÕODQ KHVDSODPDODUD J|UH WRSODP PDJQHWLN eneUMLEHOOLROGXNWDQVRQUDPRWRUGDQJHoHQDNÕP GH÷HULQH J|UH LQGNWDQV GH÷HUL 'HQNOHP (29)¶GDn kolayca hesaplanabilir. 2 * 2 I Enerji Magnetik L (29)
0RPHQW+HVDEÕ
Asenkron motorlarda moment biri stator ]HULQGH GL÷HUL GH URWRU ]HULQGH ROXúDQ LNL HOHNWULNDODQÕQÕQHWNLOHúLPLVRQXFXRUWD\DoÕNDU 6DELW ELU PRPHQWLQ UHWLOHELOPHVL LoLQ EX LNL DODQÕQ PRWRUXQ KDYD DUDOÕ÷ÕQGD Hú ]DPDQOÕ ELU GXUXPGDROPDVÕJHUHNLU%XoDOÕúPDGD0D[ZHOO VWUHVV PHWRGX NXOODQÕODUDN PRPHQW hesaplanPÕúWÕU (KüUP, 2002).
¨¨ © §¦
0 Pn t B B rdl T (30) UGDLUHVHO\ROXQ\DUÕoDSÕG\ROXQX]XQOX÷XO PDNLQHQLQ X]XQOX÷X B DNÕ \R÷XQOX÷XQXQn QRUPDO ELOHúHQL B DNÕ \R÷XQOX÷XQXQ WH÷HWt ELOHúHQidir.Sonuçlar
<DSÕODQ progrDP DGÕP DGÕP DúD÷ÕGDNL gibidir.
DGÕP ProgramGD LON DGÕP RODUDN oJHQ HOHPDQODUÕQ NRRUGLQDWODUÕQÕQ YH KHU ELU oJHQ HOHPDQÕ ROXúWXUDQ G÷P QXPDUDODUÕQÕQ JLULOPHVLJHUHNPHNWHGLU%XYHULOHULQJLULúLWHNHU WHNHU \DSÕODELOHFH÷i gibi dosyalardan da okutulabilir.
DGÕP Gerekli olan verilerin belirtilen GRV\DODUGDQ RNXWXOPDVÕ LúOHPLQGHQ sonra 2. DGÕPRODUDNPRWRUXQ KHVDSDODQODUÕQÕQoL]GLUPH DGÕPÕQDJHoLOLU ùHNLO. MotorXQHOOHE|OPHOHQGLULOPLúGXUXPX 0RWRUXPX]XQHOOHE|OPHOHQGLULOPLúGH÷HUOHUL '÷P6D\ÕVÕ hoJHQ(OHPDQ6D\ÕVÕ 6ÕQÕU'÷P6D\ÕVÕ ¶GLU
DGÕP Asenkron motorun elle yapÕOPÕúROXQDQ E|OPHOHQGLUPHLúOHPLQLQoL]GLULOPHVLQGHn sonra EX DGÕPGD o|]P E|OJHVLQLQ Sonlu Elemanlar <|QWHPLQHJ|UHRWRPDWLNE|OPHOHQGLUPHLúOHPL \DSWÕUÕOPDNWDGÕU 6RQOX HOHPDQODU \|QWHPLQGH o|]PQ GR÷UXOX÷XQX DUWWÕUPDN LoLQ YHNW|U SRWDQVL\HO GH÷HULQH DLW GH÷LúLPLQ ID]OD ROGX÷X E|OJHOHUGH EDNÕU GHPLUYE oJHQ HOHPDQODUÕQÕQVD\ÕVÕoR÷DOWÕOÕU
ùHNLO. Motorun otoPDWLNE|OPHOHQGLULOPLú
durumu
2WRPDWLN E|OPHOHQGLUPH SURJUDPÕ LOH ELU GHID E|OPHOHQGLUPH LúOHPL VRQXFXQGD DúD÷ÕGDNL VRQXoODUHOGHHGLOGL '÷P6D\ÕVÕ hoJHQ(OHPDQ6D\ÕVÕ 6ÕQÕU'÷P6D\ÕVÕ ¶GLU 4DGÕP %X DGÕPGD RWRPDWLN E|OPHOHQdirme LúOHPLQGHQ VRQUD HOGH HGLOHQ \HQL oJHQ HOHPDQODU YH G÷POHUH J|UH PRWRUXQ o|]PQHJHoLOLU d|]PLoLQ|QFHOLNOH A, B, C YH 1 úHNLO IRQNVL\RQODUÕ KHVDSODQÕU $\QÕ zamanda her bir oJHQ HOHPDQÕQ DODQÕ KHVDSODQÕU
ϱ͘ĂĚŦŵ͗%XDGÕPD kadar sonlu elemanlar analizi
\DSPDN LoLQ JHUHNOL RODQ KHVDS DODQODUÕ ROXúWXUXOPXúWXU $NÕP \R÷XQOX÷X 4000000 A/m2 RODUDN DOÕQPÕúWÕU Motorun analizinde 5
PDWHU\DO PRGHOL NXOODQÕOPÕúWÕU %D÷ÕO PDQ\HWLN JHoLUJHQOLN r KDYD LoLQ VLOLV\XP VDo LoLQ
RODUDN DOÕQPÕúWÕU 'LUHQo (Ohm.m) ise stator EDNÕU VDUJÕVÕ LoLQ 1.588e- URWRU DOPLQ\XP VDUJÕVÕLoLQH-DOÕQPÕúWÕU
6RQ DGÕPGD LVH ROXúWXUXODQ EX YHULOHU o|]GUOSJHUHNOLRODQE\NONOHUPDQ\HWLN LQGNVL\RQ YHNW|U SRWDQVL\HO PRPHQW JLEL EXOXQGXNWDQVRQUDLVWHQLOHQVD\ÕGDHúpotansiyel H÷ULleri PDJQHWLNDNÕ\ROX H÷ULOHUL) oL]LOLU
ùHNLO9. .D\PD ROGX÷u durumda magnetik
DNÕ\ROX H÷ULOHULH÷UL
ùHNLO0. Kayma ROGX÷XGXUXPGDPDJQHWLN
DNÕ\ROX H÷ULOHUL H÷UL
ùHNLO1. Kayma=0ROGX÷XGXUXPGD
PDJQHWLNDNÕ\ROX H÷ULOHUL H÷UL
ùHNLO2. Kayma=0ROGX÷XGXUXPGD
PDJQHWLNDNÕ\ROX H÷ULOHUL H÷UL
ùHNLO3. Kayma=0ROGX÷XGXUXPGD
magnHWLNDNÕ\ROX H÷ULOHULH÷UL
ùHNLO4. .D\PD ROGX÷XGXrumda
PDJQHWLNDNÕ\ROXH÷UOHUL H÷UL %X oDOÕúPDGD \DSÕODn analizler sonucunda motorun IDUNOÕ ND\PD GH÷HUOHULQGH KHVDSODQDQ PRPHQWGH÷HUOHULDúD÷ÕGDYHULOPLúWLU
Kayma=0.03 iken; Moment=3.8930 Nm Kayma=0.049 iken;
Moment=4.8076 Nm olarak KHVDSODQPÕúWÕU %X oDOÕúPD LoLQ WDVDUODQPÕú YH LPDO HGLOPLú asenkron motorun (6A,380V) deneysel oDOÕúPDODU sonucu elde edilen momenW GH÷HUL úHEHNHGHQ $ oHNLOGL÷LQGH 7.45 Nm dir. <DSÕODQ oDOÕúPDGD VLPHWUL GXUXPXQD J|UH
PRWRUXQ \DUÕVÕ HOH DOÕQPÕú ROGX÷XQGDQ KHVDSODQDQPRPHQWGH÷HULLOHoDUSÕOPÕúWÕU%X durumda momentin 7.78 1P ROGX÷X J|UOPúWU $UDGDNL \DNODúÕN % 4.4¶Ok hata PLNWDUÕ GD VRQOX HOHPDQODU \|QWHPLQGH NXOODQÕODQ PRGHOOHUGH \DSÕODQ LKmaller, GHQH\VHO oDOÕúPDGD NXOODQÕODQ |OoPH FLKD]Õ hatDODUÕQGDQ YE ND\QDNODQPDNWDGÕU $\UÕFD MATLAB NROD\ SURJUDP \D]ÕOÕPÕ YH LOHUL VHYL\HGH JUDILN |]HOOLNOHU GH VD÷ODPDNWDGÕU
(Freeman ve Lawther, 1973). +D]ÕU IRQNVL\RQ GRV\DODUÕ \DUGÕPÕ LOH GL÷HU SURJUDPlama GLOOHUL\OHVDWÕUODUFDWXWDQSURJUDPODU0$7/$% SURJUDPFÕOÕ÷Õ \ROX LOH VDGHFH ELUNDo VDWÕUOD KD]ÕUODQDELOLU %X DYDQWDMODUÕQGDQ GROD\Õ ELU asenkron motor analizini yaparken Matlab ProJUDPODPD'LOLNXOODQÕOPÕúWÕU
6RQXo RODUDN VRQOX HOHPDQODU \|QWHPinin ve matlab SURJUDPÕQÕQ NXOODQÕPÕQÕQ asenkron motor tasarlamada L\L QHWLFHOHU YHUHFH÷L HOGH HGLOHQVRQXoODUGDQDQODúÕOPDNWDGÕU
Kaynaklar
Chari,M.V.K.,Silvester,P., (1970). Finite Element Solution of Saturable Magnetic Field Problems, IEEE Transactions on Power Apparatus and Systems, Vol pas-89, No:7 (1642-1650)
6HOoXN $ +., (2003). Lineer Asenkron 0RWRUODUGD 8o (WNLOHULQLQ 6RQOX (lemanlar <|QWHPL\OH øQFHOHQPHVL, Doktora Tezi )ÕUDW hQLYHUVLWHVL(OD]Õ÷
Silvester, P., Cabayan, H.S., Browne, B.T., (1973). Efficient Techniques For Finite Element Analysis Of Electric Machines, IEEE PES Winter Meeting, New York.
Chari, M.V.K., (1973). Finite Element Solution Of The Eddy Current Problem In Magnetic Structures IEEE PES Summer Meeting And EHV/UHV Conference, Vancouver, B.C. Canada.
Demirchian, K. S., Chechurin, V., Sarma, I., S., Boldea, A., (2002). Nasar, The Induction Machine Handbook, CRC Pres LLC, Washington D.C., 133 159.
Cathey, J., J., (2001). Electric machines analysis and design applying matlab, Mc Graw Hill, Singapore, 317-420.
3RODW 0 .UP + 6RQOX (OHPDQODU <|QWHPLQLQ 1HVQHO 7DEDQOÕ %LU 3URJUDPODPD 'LOL øOH d|]POHQPHVL YH 7UDQVIRUPDW|UQ 0DQ\HWLN %\NONOHULQLQ +HVDEODQPDVÕ H-Journal of New World Sciences Academy. .Um H., (2002). Bir Lineer Asenkron Motorun
dHOLN 6HNRQGHULQLQ 0DQ\HWLN g]HOOLNOHULQLQ Matematiksel Olarak Modellenmesi, F.Ü. Fen ve 0K%LOLPOHUL'HUJLVL(OD]Õ÷.