Analysis and Simulation of Modified Adaptive Perturb and Observe MPPT Technique for PV Systems
|
|
- Madeleine Walsh
- 5 years ago
- Views:
Transcription
1 J. Suryakumari and G. Sahiti 9 Analysis and Simulatin f Mdifid Adaptiv Prturb and Obsrv MPPT Tchniqu fr P Systms J. Suryakumari and G. Sahiti Abstract: Slar nrgy is a clan and rnwabl nrgy rsurc fr pwr gnratin. Th pwr utput frm a slar phtvltaic systm mainly dpnds n th natur f th cnnctd lad bcaus f nn-linar I- charactristics. In th past yars, P pwr gnratin systm has attractd mr attntin du t th nrgy crisis and nvirnmnt pllutin. Phtvltaic (P pwr g nratin systms can mitigat ffctivly nvirnmntal issus such as th grn hus ffct and air pllutin. Phtvltaic (P ffrs an nvirnmntally frindly surc f lctricity, which is hwvr still rlativly cstly tday. P pwr gnratin systms hav n big prblm that th amunt f lctric pwr gnratd by P mdul is always changing with wathr cnditins i.., irradiatin and tmpratur.. Thrfr, a maximum pwr pint tracking (MPPT cntrl mthd t achiv maximum pwr (MP utput at ral tim bcms indispnsabl in P gnratin systms. Th maximum pwr pint tracking (MPPT f th P utput fr all sunshin cnditins is a ky t kp th utput pwr pr unit cst lw fr succssful P applicatins. Svral tchniqus hav bn prpsd fr maximum pwr tracking. Th mst cmmnly usd tchniqus fr MPPT, ar th Hill Climbing Tchniqus. Ths includ Prturb & Obsrv mthd Adaptiv P&O and mdifid adaptiv P&O tchniqus. It is knwn that th P&O mthd xhibits rratic bhavir undr rapidly changing irradianc lvl that causs incrrct r slw maximum pwr tracking. Th Mdifid P&O (MP&O mthd was prpsd t slv this prblm by dcupling th P pwr fluctuatins causd by hill-climbing prcss frm ths causd by irradianc changing. Kywrds: MPPT (Maximum Pwr Pint Trackr, P&O (Prturb and Obsrv, Phtvltaic systm, Bst Cnvrtr, Hill-Climbing, Adaptiv.. INTRODUCTION As fssil nrgy bcms mr xpnsiv and causs grwing nvirnmntal cncrns, nrgy frm natural rsurcs such as sunlight and wind ar glbally wlcmd t rplac th fssil ful. Amng mthds f gnrating lctric pwr by altrnativ rsurcs, phtvltaic (P has grwn stadily in rcnt dcads as a carbn-fr tchnlgy altrnativ P cnvrts sunlight dirctly int currnt lctricity by mans f th phtvltaic ffct. Sinc cmmn slar clls ar mad frm silicn-basd smicnductrs, th phtvltaic ffct is invlvd with th p-n junctin f th slar clls. First, sunlight prducs J. Suryakumari is wrking as Assciat Prfssr and G. Sahiti is a M. Tch Studnt, bth ar frm Dpartmnt Of Elctrical and Elctrnics Enginring, R.G.M.C.E.T, Nandyal, A.P., India, jdsk.@gmail.cm, sahithy.gmatham@gmail.cm lctrn-hl pairs (EHPs int th cll. Thn, th lctrns mv t th n-rgin and th hls mv t th p-rgin as a rsult f th lctric fild cratd by th junctin. Th lctric chargs cllctd in bth rgins finally flw as lctric currnt int a cnnctd lad. A P systm is a pwr systm that gnrats dirct currnt (DC frm sunlight and prcsss it rquiring DC r altrnating currnt (AC lctricity. Instad f slar clls, th P systm gnrally uss P panl-intrlinkd packags with slar clls-r P arrays-cmbind assmblis f P panls-du t th lw vltag f a singl slar cll. Figur : Blck diagram f P systm As shwn in Figur, th P systm cnsists f thr stags: pwr gnratin, pwr cnvrsin & cnditining, and pwr distributin. In th pwr gnratin stag, th P array gnrats DC lctricity dirctly frm sunlight. Th gnratd DC must b cntrlld and cnductd in th pwr cnvrsin & cnditining stag t suit distributin rquirmnts. This stag uss pwr lctrnic dvics such as DC-DC cnvrtrs and/r DC-AC invrtrs fr prcssing DC frm th array. Th utput pwr f P mdul is nnlinar functin f tmpratur, islatin, and thus linar cntrl thry is nt suitabl fr MPPT. Thr ar a fw MPPT mthds prsntd. Th prturbatin and bsrvatin (P&O mthd with fixd prturbatin stp, which is wll knwn as th hill-climbing mthd, is widly applid. P&O algrithms hav drawbacks such as slw rspns and high scillatins arund MPP. Hwvr, pwr scillatins always appar in this mthd undr stady stat and rduc th fficincy f P mdul. Sm mthds fr aviding th prblms f th P&O mthd hav bn prpsd. This papr prpss a nw mthd fr th MPPT cntrl f P systms. Adaptiv P&O utilizs prturb as varying prturb. Evn thugh varying prturb is usd, but still thr xists scillatin arund MPP. Ths ar vrcm by mdifid adaptiv tchniqu in which autmatic tuning mchanism and cntrl md switching is usd. Owing t changs in th slar radiatin nrgy and th cll prating tmpratur, th utput pwr f a slar array Intrnatinal Jurnal f Emrging Trnds in Elctrical and Elctrnics (IJETEE ISSN: l. 9, Issu., Nv-.
2 J. Suryakumari and G. Sahiti is nt cnstant at all tims. Cnsquntly, during th dsign prcss a simulatin must b prfrmd fr systm analysis and paramtr sttings.. HOW A P CELL WORKS Slar cll cnsists f a p-n junctin fabricatd in a thin wafr r layr f a smicnductr matrial. Phtvltaic clls ar mad f svral typs f smicnductrs using diffrnt manufacturing prcsss.. Th cmmrcial slar cll is mad f wafr-basd tchnlgy f smicnductr matrials, such as Crystallin Si (C -Si and thin film. Diffrnt typs f silicn can b usd t fabricat th slar cll i.. mn-crystallin silicn, ply-crystallin silicn, and amrphus. Th variatin btwn ths typs is distinguishd by th cnvrsin fficincy f th P cll. Fig. rughly illustrats th rprsntd by a simplifid quivalnt circuit mdl such as th n givn in Fig. and/r by an quatin as in (. A phtvltaic cll is basically a smi-cnductr did whs p n junctin is xpsd t light [5], [6]. Mdling is basic tl f th ral systm simulatin. Fr mdling, it is ncssary t analyz th influnc f diffrnt factrs n th phtvltaic clls. Th mathmatical mdls fr phtvltaic clls ar basd n th thrtical quatins that dscrib th pratin f th phtvltaic clls and can b dvlpd using th quivalnt circuit f th phtvltaic clls. Th mst cmmn n is as fllws. Fig.. Equivalnt circuit f P cll Fig..Stuctur f a P cll physical structur f a P cll.. Whn phtns frm th slar nrgy hits th slar cll, with nrgy gratr than band gap nrgy f th smicnductr, lctrns ar knckd ls frm th atms in th matrial, crating lctrn-hl pairs. Ths carrirs ar swpt apart undr th influnc f th intrnal lctric filds f th p-n junctin and crat a currnt prprtinal t th incidnt radiatin. Whn th cll is shrt circuitd, this currnt flws in th xtrnal circuit; whn pn circuitd, this currnt is shuntd intrnally by th intrinsic p-n junctin did. Th rat f gnratin f lctric carrirs dpnds n th flux f incidnt light and th capacity f absrptin f th smicnductr. Th capacity f absrptin dpnds mainly n th smicnductr band gap, n th rflctanc f th cll surfac (that dpnds n th shap and tratmnt f th surfac, n th intrinsic cncntratin f carrirs f th smicnductr, n th lctrnic mbility. Th slar radiatin is cmpsd f phtns f diffrnt nrgis. Phtns with nrgis lwr than th band gap f th P cll ar uslss and gnrat n vltag r lctric currnt. Phtns with nrgy suprir t th band gap gnrat lctricity, but nly th nrgy crrspnding t th band gap is usd th rmaindr f nrgy is dissipatd as hat in th bdy f th P cll. Smicnductrs with lwr band gaps may tak advantag r a largr radiatin spctrum, but th gnratd vltags ar lwr. Slar cll gnratd currnt dpnds n th charactristic f matrial, ag f slar cll, irradiatin and cll tmpratur. A dubl xpnntial quatin may b usd fr th plycrystallin silicn clls. = ph s.(.. ( ( Equatin ( rprsnts utput vltag f a P cll = Output currnt f a P cll Whr, = = ( ( ( = [ + ( 98] ( (5 Th P array pwr can b calculatd using th fllwing quatin = (6. MODELLING OF P ARRAY = ( (7 P arrays ar built up with cmbind sris r paralll cmbinatins f P slar clls, which ar usually Whr, Intrnatinal Jurnal f Emrging Trnds in Elctrical and Elctrnics (IJETEE ISSN: l. 9, Issu., Nv-.
3 J. Suryakumari and G. Sahiti is utput vltag f a P cll ( is utput currnt f a P cll (A is th numbr f mduls cnnctd in sris is th numbr f mduls cnnctd in paralll is th light gnratd currnt in a P cll (A is th P cll saturatin currnt (A is th sris rsistanc f a P cll (Ω A=B is an idality factr =.6 K is Bltzmann cnstant =.85-Nm/K T is th cll tmpratur in Klvin =98K Q is lctrn charg =.6-9 Culmbs is th rfrnc tmpratur =.8K is th P cll shrt circuit currnt N = N f clls is shunt rsistanc f a P cll is th P cll illuminatin (MW/cm is th saturatin currnt at T r E g is th nrgy band gap (v Bth k and T shuld hav th sam tmpratur unit, ithr Klvin r Clsius. Th curv fitting factr A is usd t adjust th I- charactristics f th cll btaind frm th actual charactristics btaind by tsting. Eq. ( givs th vltag f a singl slar cll which is thn multiplid by th numbr f th clls cnnctd in sris t calculat th full array vltag. Sinc th array currnt is th sum f th currnts flwing thrugh th clls in paralll branchs, th cll currnt IC is btaind by dividing th array currnt by th numbr f th clls cnnctd in paralll bfr bing usd in (, which is nly valid fr a crtain cll prating tmpratur T with its crrspnding slar irradiatin lvl Sc. If th tmpratur and slar irradiatin lvls chang, th vltag and currnt utputs f th P array will fllw this chang. Hnc, th ffcts f th changs in tmpratur and slar irradiatin lvls shuld als b includd in th final P array mdl. Th cmplt bhavir f P clls ar dscribd by fiv mdl paramtrs (I ph, N, Is, Rs, R sh which is rprsntativ f th physical bhavir f P cll/mdul. Ths fiv paramtrs f P cll/mdul ar in fact rlatd t tw nvirnmntal cnditins f slar islatin & tmpratur. Th dtrminatin f ths mdl paramtrs is nt straightfrward wing t nn-linar natur f quatin. Fig.. Maximum Pwr Pint ( mp, I mp Charactristic I curv f a practical P dvic and th thr rmarkabl pints: shrt circuit (, I sc, MPP ( mp, I mp, and pn circuit ( c,. Th shrt circuit currnt slightly incrass with cll tmpratur. Fr practical us, P clls can b ampr curv lctrical cnnctd in diffrnt ways: sris r paralll. P clls ar first cnnctd in sris in mst manufacturing mthds t frm P mdul. Mduls can b cnnctd in diffrnt ways t frm P array. This is dn fr th sak f vltag/currnt rquirmnt f th pwr cnditining units (PCU s f th P systm. IRRADIANCE (A Simulatin mdl f P cll Basd n Matlab / Simulink Irradianc P MODEL Ppv pv Ipv Rsistr Fig.5. Simulatin mdl f P cll Th utput charactristic f a phtvltaic (P array is nnlinar and is influncd by slar irradianc lvl, ambint tmpratur, wind spd, humidity, prssur, tc. Th irradiatin and ambint tmpratur is tw primary factrs. T study th utput charactristics f P cll, sm xprimnts basd n simulatin f P cll hav bn dn. Fr cnstant tmpratur (5 C and diffrnt intnsity (- W/m Th P array currnt cnstant up t sm vltag lvl and thn it will b dcrasd. Th P array currnt always incrass with intnsity -.6 OLTAGE.7656 CURRENT.5 POWER Intrnatinal Jurnal f Emrging Trnds in Elctrical and Elctrnics (IJETEE ISSN: l. 9, Issu., Nv-.
4 J. Suryakumari and G. Sahiti W/m 8W/m 5 C 5 C 65 C 6W/m 85 C Currnt(A W/m Currnt(A Fig6(a. I- charactristics f Slar array fr varius irradianc at a cnstant tmpratur f 5 C. Fr cnstant tmpratur (5 C and diffrnt intnsity (- W/m Th P array pwr incrass up t sm vltag lvl and thn it will b dcrasd. Th P array pwr always incrass with lw t high intnsity. 8 Pwr(W ltag( W/m 8W/m 6W/m W/m Fig7(a. I- charactristics f Slar array fr varius tmpratur at cnstant irradianc f W/m. 8 Pwr(W 6 ltag( ltag( 5 C 5 C 65 C 85 C Fig7(b. P- charactristics f Slar array fr varius tmpratur at a cnstant irradianc f W/m. ltag(. BOOST CONERTER Fig 6(b. P- charactristics f Sla array fr varius irradianc at a cnstant tmpratur f 5 C. Frm figur.7 (a I- charactristics fr diffrnt tmpratur and cnstant irradianc th gnratd pwr is gradually dcrasd and maximum pwr availabl mr at lw tmpratur. Th utput vltag can b gratr than th input vltag in (slar array vltag.th switch S prats at high frquncis t prduc a chppd utput vltag []. Th pwr flw is cntrlld by adjusting th n/ff duty cycl f th switching. Th avrag utput vltag is dtrmind by th quatin, Frm figur.7 (b P- charactristics fr diffrnt tmpratur and cnstant irradianc th currnt is cnstant up t sm vltag and thn it will dcras gradually. in T T ff D (8 Intrnatinal Jurnal f Emrging Trnds in Elctrical and Elctrnics (IJETEE ISSN: l. 9, Issu., Nv-.
5 J. Suryakumari and G. Sahiti Fig.8. Bst Tplgy Bst cnvrtr which bsts th vltag t maintain th maximum utput vltag cnstant fr all th cnditins f tmpratur and slar irradianc variatins. A simpl bst cnvrtr is as shwn in Figur9.. MPPT TECHNIQUES.. Opn Circuit ltag mthd This mthd uss OC t calculat MP. Onc th systm btains th OC valu, MP is calculatd by th quatin 9. MP = k x OC (9 Th k valu is typically varis frm.7 t.8. It is ncssary t updat OC ccasinally t cmpnsat fr any tmpratur changs. It uss fractin f pn circuit vltag t dtrmin th mduls vltag at th maximum pwr pint. Th pn circuit vltag algrithm is basd n th bsrvatin frm -I curvs that th rati f th array s maximum pwr vltag ( mp t its pn circuit vltag ( c is apprximatly cnstant. Hr th factr is always <.Th slar array is tmprarily islatd frm th MPPT and a c masurmnt is takn.. Shrt Circuit Currnt mthd Th shrt circuit currnt mthd uss a valu f ISC t stimat IMP. I MP = k x I SC ( This mthd uss a shrt lad puls t gnrat a shrt circuit cnditin. During th shrt circuit puls, th input vltag will g t zr, s th pwr cnvrsin circuit must b pwrd frm sm thr surc. On advantag f this systm is th tlranc fr input capacitanc cmpard t th OC mthd. Th k valus ar typically cls t.9 t.98 Fig.9. Blck diagram f P&O MPPT If th pwr incrasd, th prturbatin is cntinuus in th sam dirctin in th nxt prturbatin cycl, thrwis th prturbatin dirctin is rvrsd. This way, th prating pint f th systm gradually mvs twards th MPP and scillats arund it in stady-stat cnditins. Larg prturbatin stp sizs yild fast tracking f th MPP undr varying atmsphric cnditins but rsult in rducd avrag pwr cnvrsin in stady stat du t larg scillatins arund th MPP. It was prvd that th P&O MPPT cntrl systm smtims dviats frm th maximum prating pint in cas f rapidly changing atmsphric cnditins, such as brkn cluds. Anthr disadvantag is that this simpl tracking mthd has difficulty in prviding gd prfrmanc in bth dynamic and stady-stat rspnss. Hnc th famus tradff prblm btwn fastr rspns and stady-stat scillatins is inhrnt. Mrvr, th prturbatin is nt gnric. In rdr t vrcm all this, high prfrmanc P&O tchniqu is prpsd.. Prturb and Obsrv (P&O mthd A P&O mthd is th mst simpl, which mvs th prating pint tward th maximum pwr pint pridically incrasing r dcrasing th P array vltag by cmparing pwr quantitis btwn in th prsnt and past. Th blck diagram f P&O mthd is illustratd in Fig. 9. Intrnatinal Jurnal f Emrging Trnds in Elctrical and Elctrnics (IJETEE ISSN: l. 9, Issu., Nv-.
6 J. Suryakumari and G. Sahiti r(w w P 5 t(a n r u C.5.5 Fig.Flw chart diagram f P&O MPPT mthd Tim(sc Fig(c. P array utput pwr fr P&O MPPT tchniqu Th rspns with prturbatin and bsrvatin (P&O MPPT Tchniqu wavfrms ar (a P array utput currnt (b P array utput vltag (c P array utput pwr at tmpratur=5 c and slar irradiatin =W/m.. Adaptiv Prturbatin and Obsrvatin mthd (AP&O Th main ida bhind this tchniqu is that at th start f any hill climbing tchniqu, larg prturb stps ar ndd t quickly rach th MPP, and as th MPP is apprachd, th prturb valu nds t b dcrasd t avid larg scillatins arund this maximum utput pwr prating pint. This adaptiv tchniqu utilizs th rrr btwn tw succssiv array pwr signals calculatd frm th masurd array vltag and currnt signals t crat an adaptiv prturb Tim(sc Fig(a. P array utput currnt fr P&O MPPT tchniqu 5 ( g lta Tim(sc Fig(b. P array utput vltag fr P&O MPPT tchniqu Fig.. Blck diagram f Adaptiv P&O MPPT Basically, at th start f th hill climbing prcss, this rrr is larg and dcrass as th maximum pwr prating pint is apprachd at stady stat. Thrfr, this rrr can Intrnatinal Jurnal f Emrging Trnds in Elctrical and Elctrnics (IJETEE ISSN: l. 9, Issu., Nv-.
7 J. Suryakumari and G. Sahiti 5 b tratd lik an rrr signal in a clsd-lp systm that nds t b minimizd at stady stat, prvntd frm vrsht at startup, and fr frm stady-stat scillatins. Th simplst clu t achiv all ths targts is t trat this rrr signal using a cnvntinal PI cntrllr, which is th main cr f this tchniqu. Evn thugh prturb is adaptiv, still thr xists scillatins arund MPP and givs slw rspns. Th flwchart f Adaptiv P&O is shwn in fig ( ( g lta Tim(sc Fig(b. P array utput vltag fr AP&O MPPT tchniqu 8 6 r(w w P.5 Fig.Flw chart diagram f AP&O MPPT mthd Tim(sc Fig(c. P array utput pwr fr AP&O MPPT tchniqu.5 Mdifid Adaptiv Prturbatin and Obsrvatin mthd (AP&O A mdifid adaptiv hill climbing (MAHC MPPT cntrl mthd is intrducd basd n th prvius rsarch and dtaild analysis f th charactristics f P pwr systms. Th mdificatins t th traditinal hill climbing mthd includ autmatic paramtr tuning and Cntrl md switching..5. Prpsd MPPT Tchniqu t(a n r u C Tim(sc Fig(a. P array utput currnt fr AP&O MPPT tchniqu Thr is a tradff btwn dynamic rspns and stady stat prfrmanc du t th slctin f th incrmntal stp f switching duty cycl. Thrugh analysis, it is idal t mak larg switching duty cycl during transint stag and small in stady stat. In th prpsd MAHC mthd, this prblm is slvd by th autmatic tuning f paramtr nlin. Whn th pwr changs in a larg rang primarily du t nvirnmntal variatin, this tunr will chang th switching duty cycl t a larg valu t satisfy th fast rspns rquirmnt during th transint stag. Whn th pwr chang is small, th cntrllr assums that th systm ntrs th stady-stat stag and th valu f "a" bcms small t kp cntrl signal chang smth. With this tuning mchanism, bth dynamic and stady-stat rquirmnts can b cnsidrd in th cntrllr dsign, bcaus th critical paramtr is updatd and adjustd Intrnatinal Jurnal f Emrging Trnds in Elctrical and Elctrnics (IJETEE ISSN: l. 9, Issu., Nv-.
8 J. Suryakumari and G. Sahiti 6 adaptivly.. In sm spcific cass, it was shwn that th P&O mthd culd caus th prating pint t dviat frm th ptimal pint during th prid f rapid islatin changs. This prblm culd b avidd by switching th cntrl md. Th cntrl algrithm can b dmnstratd in flw chart frmat shwn in Fig.8, whr "P" and "D" rprsnt th P pwr lvl and th duty cycl valu rspctivly. n t(a r u C Tim(sc Fig7(a. P array utput currnt fr MAP&O MPPT tchniqu Fig5. Blck diagram f MAP&O MPPT 5 ( g lta Tim(sc Fig7(b. P array utput vltag fr MAP&O MPPT tchniqu 8 6 r(w w P Tim(sc Fig6.Flw chart diagram f MAP& &O MPPT mthd Fig7(b. P array utput vltag fr MAP&O MPPT tchniqu Intrnatinal Jurnal f Emrging Trnds in Elctrical and Elctrnics (IJETEE ISSN: l. 9, Issu., Nv-.
9 J. Suryakumari and G. Sahiti 7 S. N MPPT Tchniqu ltag ( Currnt (A Pwr (W Efficincy (% P & O AP&O MAP&O Tabl5. Cmparisn f MPPT Tchniqus at a tmpratur f 5 C and irradianc f W/m 6. CONCLUSION This papr prpss dsign and mdling f pht vltaic systm, simpl bst cnvrtr and Mdifid Adaptiv P&O MPPT Tchniqu. Th P cll utput vltag varis with atmsphric paramtrs such as tmpratur and irradiatin. In rdr t prat P array at MPP, w nd an intrfac systm btwn P array and lad calld MPPT. Th OC, SC and P&O mthds ar simpl and mstly usd mthds, but d nt accuratly track th MPP. In rdr t vrcm th drawback f abv mthds Mdifid Adaptiv P&O MPPT mthd is prpsd, in which switching duty cycl is usd as cntrl paramtr. Rfrncs []. Dunlp JP, Natinal Jint Apprnticship and Training Cmmitt fr th Elctrical Industry. Pht-vltaic systms. Orland Park, Ill.: Amrican Tchnical Publishrs, Inc.;. [] F.Z. Png, L. M. Tlbrt:Multilvl Cnvrtrs fr Larg Elctric drivs, IEEE Transactins n Industry Applicatins, Jan/Fb 999, vl. 5. [] J. Applbaum: Starting and stady-stat charactristics f DC mtrs pwrd by slar cll gnratrs, IEEE Trans., EC-I ( [] J. A. Rgr: Thry f th dirct cupling btwn DC mtrs and phtvltaic slar arrays, Slar Enrgy, ( [5] J.Surya Kumari, Ch. Sai Babu and J. Yugandhar Dsign and Invstigatin f Shrt Circuit Currnt Basd Maximum Pwr Pint Tracking fr Phtvltaic Systm,Intrnatinal Jurnal f Rsarch and Rviws in Elctrical and Cmputr Enginring (IJRRECE l., N., Jun. [6]. K.E. Yagr, "Elctric hicls and Slar Pwr: Enhancing th Advantags f Elctricity", IEEE Pwr Enginring Rviw, l., N., Octbr 99. [7] K. R and S. Rahman: Tw Lp Cntrllr fr maximizing prfrmanc f a grid-cnnctd phtvltaic ful cll hybrid pwr plant, IEEE Transactins n Industry Applicatins Sptmbr 998. [8] Lai, J., and Png, F.: Multilvl Cnvrtrs- A nw Brd f Pwr Cnvrtrs, IEEE Transactins n Industry Applicatins, May/Jun 996, vl.. [9] L. M. Tlbrt, F. Z. Png: Multilvl Cnvrtrs as a Utility Intrfacfr Rnwabl Enrgy Systms, IEEE Pwr Enginring Scity Summr Mting, July 5-,. Sattl, Washingtn, pp [] Macrci Mnds Casarr, Dnizar Cruz Martins Grid cnnctd PSystm: Intrductin t Bhavir Matching IEEE Transactins n Industrial Elctrnics 8 [] M. Bursch: Phtvltaic Enrgy Systms Dsign and Installatin, McGraw-Hill, Nw Yrk, 98 [ M. Calais,.G. Aglidis, M. Minhardt: Multilvl Cnvrtrs fr Singl-phas Grid Cnnctd Phtvltaic Systms: An Ovrviw. Slar Enrgy. l. 66, N 5. [] Nguyn, D y Lhman, B.:A Rcnfigurabl Slar Phtvltaic Array Undr Shadw Cnditins, Applid Pwr Elctrnics Cnfrnc and Expsitin, pp , 8. [] Srgi Dahr, Jurgn Schmid and Frnand L.M Antuns, Multilvl Invrtr Tplgis fr Stand-Aln P Systms IEEE Transactins n Industrial Elctrnics.l.55, N.7, July 8. [5] Tchnlgy radmap slar phtvltaic nrgy. [Intrnt] Paris: OECD/IEA;. [6] W. Z. Far and M. K. Balahandr: Dynamic prfrmanc f a DC shunt mtr cnnctd t a phtvltaic array, IEEE Trans., EC-( Authrs Prfil: J. Surya Kumari was brn in Kurnl, India in 98. Sh rcivd th B.Tch (Elctrical and Elctrnics Enginring dgr frm S.K Univrsity, India in and th M.Tch (High vltag Enginring frm J.N.T Univrsity, Kakinada in 6. In 5 sh jind th Dpt. Elctrical and Elctrnics Enginring, R.G.M. Cllg f Enginring and Tchnlgy, Nandyal, as an Assistant Prfssr. Sh has publishd svral Natinal and Intrnatinal Jurnals/Cnfrncs. Hr fild f intrst includs Pwr lctrnics, Phtvltaic systm, Pwr systms and High vltag nginring. G. SAHITI was brn in Nllr, India. Sh rcivd th B.Tch (Elctrical and Elctrnic s Enginring dgr frm Jawaharlal Nhru tchnlgical Univrsity, Anantapur in 9 and pursing M.Tch (Pwr Elctrnics frm RGMCET Autnmus, Nandyal. Hr ara f intrst is Pwr Elctrnics, Pht- vltaic nrgy systm fr maximum pwr pint tracking. sahithy.gmatham@gmail.cm. Intrnatinal Jurnal f Emrging Trnds in Elctrical and Elctrnics (IJETEE ISSN: l. 9, Issu., Nv-.
Chapter 2 Linear Waveshaping: High-pass Circuits
Puls and Digital Circuits nkata Ra K., Rama Sudha K. and Manmadha Ra G. Chaptr 2 Linar Wavshaping: High-pass Circuits. A ramp shwn in Fig.2p. is applid t a high-pass circuit. Draw t scal th utput wavfrm
More informationTopic 5: Discrete-Time Fourier Transform (DTFT)
ELEC36: Signals And Systms Tpic 5: Discrt-Tim Furir Transfrm (DTFT) Dr. Aishy Amr Cncrdia Univrsity Elctrical and Cmputr Enginring DT Furir Transfrm Ovrviw f Furir mthds DT Furir Transfrm f Pridic Signals
More informationLecture 26: Quadrature (90º) Hybrid.
Whits, EE 48/58 Lctur 26 Pag f Lctur 26: Quadratur (9º) Hybrid. Back in Lctur 23, w bgan ur discussin f dividrs and cuplrs by cnsidring imprtant gnral prprtis f thrand fur-prt ntwrks. This was fllwd by
More informationSensors and Actuators Introduction to sensors
Snsrs and Actuatrs Intrductin t snsrs Sandr Stuijk (s.stuijk@tu.nl) Dpartmnt f Elctrical Enginring Elctrnic Systms APAITIVE IUITS (haptr., 7., 9., 0.6,.,.) apaciti snsr capacitanc dpnds n physical prprtis
More informationLECTURE 5 Guassian Wave Packet
LECTURE 5 Guassian Wav Pact 1.5 Eampl f a guassian shap fr dscribing a wav pact Elctrn Pact ψ Guassian Assumptin Apprimatin ψ As w hav sn in QM th wav functin is ftn rprsntd as a Furir transfrm r sris.
More informationAnother Explanation of the Cosmological Redshift. April 6, 2010.
Anthr Explanatin f th Csmlgical Rdshift April 6, 010. Jsé Francisc García Juliá C/ Dr. Marc Mrncian, 65, 5. 4605 Valncia (Spain) E-mail: js.garcia@dival.s h lss f nrgy f th phtn with th tim by missin f
More informationLecture 27: The 180º Hybrid.
Whits, EE 48/58 Lctur 7 Pag f 0 Lctur 7: Th 80º Hybrid. Th scnd rciprcal dirctinal cuplr w will discuss is th 80º hybrid. As th nam implis, th utputs frm such a dvic can b 80º ut f phas. Thr ar tw primary
More information. This is made to keep the kinetic energy at outlet a minimum.
Runnr Francis Turbin Th shap th blads a Francis runnr is cmplx. Th xact shap dpnds n its spciic spd. It is bvius rm th quatin spciic spd (Eq.5.8) that highr spciic spd mans lwr had. This rquirs that th
More informationAnalysis of the Output Ripple of the DC DC Boost Charger for Li-Ion Batteries
Jurnal f Pwr Elctrnics, Vl. 4, N., pp. 35-4, January 4 35 JPE 4--4 http://dx.di.rg/.63/ JPE.4.4..35 ISSN(Print: 598-9 / ISSN(nlin: 93-478 Analysis f th utput ippl f th Bst hargr fr i-in Battris Van-Sang
More informationLecture 2a. Crystal Growth (cont d) ECE723
Lctur 2a rystal Grwth (cnt d) 1 Distributin f Dpants As a crystal is pulld frm th mlt, th dping cncntratin incrpratd int th crystal (slid) is usually diffrnt frm th dping cncntratin f th mlt (liquid) at
More informationModern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom
Mdrn Physics Unit 5: Schrödingr s Equatin and th Hydrgn Atm Lctur 5.6: Enrgy Eignvalus f Schrödingr s Equatin fr th Hydrgn Atm Rn Rifnbrgr Prfssr f Physics Purdu Univrsity 1 Th allwd nrgis E cm frm th
More informationMODEL-INVERSE BASED REPETITIVE CONTROL
MODEL-INVERSE BASED REPETITIVE CONTROL T. Hart*, J. Hätönn*, D.H. Owns* Dparmnt f Autmatic Cntrl and Systms Enginring Th Univrsity f Shffild Mappin Strt S1 3JD Shffild Unitd Kingdm Tl: +44(01114 550 Fax:
More informationMHT-CET 5 (PHYSICS) PHYSICS CENTERS : MUMBAI /DELHI /AKOLA /LUCKNOW / NASHIK /PUNE /NAGPUR / BOKARO / DUBAI # 1
1. (D) Givn, mass f th rckts, m = 5000 kg; Exhaust spd, v = 800 m/s Acclratin, a = 0 m/s m Lt is amunt f gas pr scnd, t Frc = m (a + g) mu m a g t m 800 m a g t 5000 10 0 5000 0 m 5000 0 187.5 kg sc t
More information... = ρi. Tmin. Tmax. 1. Time Lag 2. Decrement Factor 3. Relative humidity 4. Moisture content
9//8 9//9 9/7/ 56-5 9 * - - midvar@sutch.ac.ir 7555- * -...... : «Rsarch Nt» Effct f mistur cntnt f building matrials n thrmal prfrmanc f xtrir building walls A. Omidvar *, B. Rsti - Assist. Prf., Mch.
More informationA Unified Theory of rf Plasma Heating. J.e. Sprott. July 1968
A Unifid Thry f rf Plasma Hating by J.. Sprtt July 968 PLP 3 Plasma Studis Univrsity f iscnsin INTRODUCfION In this papr, th majr rsults f PLP's 86 and 07 will b drivd in a mr cncis and rigrus way, and
More information6. Negative Feedback in Single- Transistor Circuits
Lctur 8: Intrductin t lctrnic analg circuit 36--366 6. Ngativ Fdback in Singl- Tranitr ircuit ugn Paprn, 2008 Our aim i t tudy t ffct f ngativ fdback n t mall-ignal gain and t mall-ignal input and utput
More informationCOLLECTOR SELECTION FOR SOLAR EJECTOR COOLING SYSTEM
Slar Enrgy Vl. 71, N. 4, pp. 69 74, 001 Prgamn P II: S0038 09X(01)0004 1 001 Publishd by Elsvir Scinc Ltd Printd in Grat Britain 0038-09X/01/$ - s frnt mattr www.lsvir.cm/ lcat/ slnr COLLECTOR SELECTION
More informationSERBIATRIB th International Conference on Tribology. Kragujevac, Serbia, May 2011
Srbian Triblgy Scity SERBIATRIB 11 1 th Intrnatinal Cnfrnc n Triblgy Kragujvac, Srbia, 11 13 May 11 Faculty f Mchanical Enginring in Kragujvac EFFECT OF CHANGES OF VISCOSITY OF MINERA OI IN THE FUNCTION
More informationN J of oscillators in the three lowest quantum
. a) Calculat th fractinal numbr f scillatrs in th thr lwst quantum stats (j,,,) fr fr and Sl: ( ) ( ) ( ) ( ) ( ).6.98. fr usth sam apprach fr fr j fr frm q. b) .) a) Fr a systm f lcalizd distinguishabl
More informationFUNDAMENTAL AND SECOND HARMONIC AMPLITUDES IN A COLLISIONAL MAGNETOACTIVE PLASMA UDC B. M. Jovanović, B. Živković
FACTA UNIVERSITATIS Sris: Physics, Chmistry and Tchnlgy Vl., N 5, 3, pp. 45-51 FUNDAMENTAL AND SECOND HARMONIC AMPLITUDES IN A COLLISIONAL MAGNETOACTIVE PLASMA UDC 533.9 B. M. Jvanvić, B. Živkvić Dpartmnt
More informationThe pn junction: 2 Current vs Voltage (IV) characteristics
Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n
More informationDesign Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance
TECHNICAL NTE 30 Dsign Guidlins for Quartz Crystal scillators Introduction A CMS Pirc oscillator circuit is wll known and is widly usd for its xcllnt frquncy stability and th wid rang of frquncis ovr which
More informationEven/Odd Mode Analysis of the Wilkinson Divider
//9 Wilkinn Dividr Evn and Odd Md Analyi.dc / Evn/Odd Md Analyi f th Wilkinn Dividr Cnidr a matchd Wilkinn pwr dividr, with a urc at prt : Prt Prt Prt T implify thi chmatic, w rmv th grund plan, which
More informationA Brief and Elementary Note on Redshift. May 26, 2010.
A Brif and Elmntary Nt n Rdshift May 26, 2010. Jsé Francisc García Juliá C/ Dr. Marc Mrncian, 65, 5. 46025 Valncia (Spain) E-mail: js.garcia@dival.s Abstract A rasnabl xplanatin f bth rdshifts: csmlgical
More informationStatus of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.)
Status of LAr TPC R&D (2) 214/Dc./23 Nutrino frontir workshop 214 Ryosuk Sasaki (Iwat U.) Tabl of Contnts Dvlopmnt of gnrating lctric fild in LAr TPC Introduction - Gnrating strong lctric fild is on of
More informationExam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.
Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r
More informationEXERGY ANALYSIS OF A DUAL-MODE REFRIGERATION SYSTEM FOR ICE STORAGE AIR CONDITIONING
Intrnatinal Jurnal n Architctural Scinc, Vlum 6, Numbr 1, p.1-6, 005 EXERGY ANALYSIS OF A DUAL-MODE REFRIGERATION SYSTEM FOR ICE STORAGE AIR CONDITIONING Guiyin Fang*, Lin Xing*, Fan Yang* and Hui Li #
More informationSwitched Capacitor Realizations of Fractional-Order Differentiators and Integrators Based on an Operator with Improved Performance
340 P. VARSNEY, M.UPTA,.S. VISWESWARAN, SWITCE CAPACITOR REALIZATIONS OF FRACTIONALORER Switchd Capacitr Ralizatins f FractinalOrdr iffrntiatrs and Intgratrs Basd n an Opratr with Imprvd Prfrmanc Pragya
More informationde/dx Effectively all charged particles except electrons
de/dx Lt s nxt turn our attntion to how chargd particls los nrgy in mattr To start with w ll considr only havy chargd particls lik muons, pions, protons, alphas, havy ions, Effctivly all chargd particls
More information5 Curl-free fields and electrostatic potential
5 Curl-fr filds and lctrstatic tntial Mathmaticall, w can gnrat a curl-fr vctr fild E(,, ) as E = ( V, V, V ), b taking th gradint f an scalar functin V (r) =V (,, ). Th gradint f V (,, ) is dfind t b
More informationElements of Statistical Thermodynamics
24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,
More informationMCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17)
MCB37: Physical Biology of th Cll Spring 207 Homwork 6: Ligand binding and th MWC modl of allostry (Du 3/23/7) Hrnan G. Garcia March 2, 207 Simpl rprssion In class, w drivd a mathmatical modl of how simpl
More informationOPTICAL OSCILLATOR STRENGTHS FOR THE ELECTRON QUANTUM TRANSITIONS IN ELLIPTIC NANOTUBES
OPTICAL OSCILLATOR STRENGTHS FOR THE ELECTRON QUANTUM TRANSITIONS IN ELLIPTIC NANOTUBES V. A. HOLOVATSKY, O. M. VOITSEKHIVSKA, V. I. GUTSUL Chrnivtsi Natinal Univrsity, Chrnivtsi, 58012, Ukrain, thrphys@chnu.cv.ua
More informationMAGNETIC MONOPOLE THEORY
AGNETIC ONOPOLE THEORY S HUSSAINSHA Rsarch schlar f ECE, G.Pullaiah Cllg f Enginring and Tchnlgy, Kurnl, Andhra Pradsh, India Eail: ssshaik80@gail.c Cll: +91 9000390153 Abstract: Th principal bjctiv f
More informationMicrowave Engineering
Micrwav Enginring hng-hsing Hsu Dpartmnt f Elctrical Enginring Natinal Unitd Univrsity Outlin. Transmissin Lin Thry. Transmissin Lins and Wavguids Gnral lutins fr TEM, TE, and TM wavs ; Paralll Plat wavguid
More informationPerformance of Microstrip Directional Coupler Using Synthesis Technique
ISSN: 78 8875 Vl., Issu, March 0 Prrmanc Micrstrip Dirctinal uplr Using Synthsis Tchniqu Vijayan T Asst. Prssr, Dpt E&I, Bharath Univrsity, hnnai-60007, India ABSTRAT: Th intrducd dsign mthd rquirs nly
More informationDUAL NATURE OF MATTER AND RADIATION
Chaptr 11 DUAL NATURE OF MATTER AND RADIATION Intrdctin Light xhibit dal natr - wav natr and particl natr. In Phnmna lik Intrfrnc, diffrctin tc wav natr is xhibitd. In pht lctric ffct, cmptn ffct tc particl
More informationELEC 372 LECTURE NOTES, WEEK 11 Dr. Amir G. Aghdam Concordia University
ELEC 37 LECTURE NOTES, WEE Dr Amir Aghdam Cncrdia Univrity Part f th nt ar adaptd frm th matrial in th fllwing rfrnc: Mdrn Cntrl Sytm by Richard C Drf and Rbrt H Bihp, Prntic Hall Fdback Cntrl f Dynamic
More informationSynchronous machines
Synchronous gnrator (altrnator): transorms mchanical nrgy into lctric nrgy; dsignd to gnrat sinusoidal oltags and currnts; usd in most powr plants, or car altrnators, tc. Synchronous motor: transorms lctric
More informationChapter 2: Examples of Mathematical Models for Chemical Processes
Chaptr 2: Exampls Mathmatical Mdls r Chmical Prcsss In this chaptr w dvlp mathmatical mdls r a numbr lmntary chmical prcsss that ar cmmnly ncuntrd in practic. W will apply th mthdlgy discussd in th prvius
More informationPrinciples of Humidity Dalton s law
Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid
More informationExtraction of Doping Density Distributions from C-V Curves
Extraction of Doping Dnsity Distributions from C-V Curvs Hartmut F.-W. Sadrozinski SCIPP, Univ. California Santa Cruz, Santa Cruz, CA 9564 USA 1. Connction btwn C, N, V Start with Poisson quation d V =
More informationChapter 6: Polarization and Crystal Optics
Chaptr 6: Polarization and Crystal Optics * P6-1. Cascadd Wav Rtardrs. Show that two cascadd quartr-wav rtardrs with paralll fast axs ar quivalnt to a half-wav rtardr. What is th rsult if th fast axs ar
More informationSuperheterodyne Amplification for Increase the Working Frequency
Jurnal f Elctrmagntic Analysis and Applicatins, 7, 9, 43-5 http://www.scirp.rg/jurnal/jmaa ISSN Onlin: 94-749 ISSN Print: 94-73 Suprhtrdyn Amplificatin fr Incras th Wrking Frquncy Svtlana Kshvaya, Vladimir
More informationSIMULATION OF 2.4 GHz LOW-POWER CMOS LC QUADRATURE VOLTAGE CONTROLLED OSCILLATOR
IJSS : 6(), 0, pp. 3-36 SIMULTION OF.4 GHz LOW-POWER CMOS LC QUDRTURE VOLTGE CONTROLLED OSCILLTOR Srja B.S and Radha S. Sathyabama Univrsity, E-mail: srjaabs@gmail.cm Dpartmnt f ECE, SSN Cllg f Enginring,
More informationLesson 8 Case Studies
0.43 Lssn 8 Cas Studis Yu Will Larn Instrumntatin fr:. Lasr phtchmistry and phtlctrchmistry B. Scanning Prb Micrscpy C. PI cntrl in chmical nginring s wll as data tratmnt and prsntatin 1. Lasr phtchmistry
More informationA Control Strategy for Photovoltaic-Solid Polymer Electrolysis System Based on Surface Temperature of PV Panel
Amrican Journal of Applid Scincs 5 (7): 5-, ISSN 1546-939 Scinc Publications Corrsponding Author: A Control Stratgy for Photovoltaic-Solid Polymr Elctrolysis Systm Basd on Surfac Tmpratur of PV Panl 1
More informationChapter 33 Gauss s Law
Chaptr 33 Gauss s Law 33 Gauss s Law Whn askd t find th lctric flux thrugh a clsd surfac du t a spcifid nn-trivial charg distributin, flks all t ftn try th immnsly cmplicatd apprach f finding th lctric
More informationFuzzy logic controller for the maximum power point tracking in photovoltaic system
Intrnational Journal of Computr Applications (975 8887) Fuzzy logic controllr for th maximum powr point tracking in photovoltaic systm G. Balasubramanian Assistant Profssor Dpartmnt of Elctrical Enginring
More informationBORH S DERIVATION OF BALMER-RYDBERG FORMULA THROUGH QUANTUM MECHANICS
BORH S DERIVATION OF BALMER-RYDBERG FORMULA THROUGH QUANTUM MECHANICS Musa D. Abdullahi Umaru Musa Yar adua Univrsity, P.M.B. 18 Katsina, Katsina Stat, Nigria musadab@utlk.cm Abstract Accrding t classical
More informationExergy, Economic and Environmental Analysis for Simple and Combined Heat and Power IC Engines
Sustainability 2015, 7, 4411-4424; di:10.3390/su7044411 Articl OPEN AESS sustainability ISSN 2071-1050 www.mdpi.cm/jurnal/sustainability Exrgy, Ecnmic and Envirnmntal Analysis fr Simpl and mbind Hat and
More informationVoltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes
Lctur 1. oltag, Currnt, Powr, Sris sistanc, Paralll sistanc, and Diods Whn you start to dal with lctronics thr ar thr main concpts to start with: Nam Symbol Unit oltag volt Currnt ampr Powr W watt oltag
More informationLecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e
8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain
More informationEnergy Management for a Power-Split Plug-in Hybrid Electric Vehicle Based on Dynamic Programming and Neural Networks
This articl has n accptd fr pulicatin in a futur issu f this jurnal, ut has nt n fully ditd. Cntnt may chang prir t final pulicatin. Citatin infrmatin: DOI.9/TVT.3.87, IEEE Transactins n Vhicular Tchnlgy
More informationAdditivity of Capacitive and Inductive Coupling in Submicronic Interconnects
Additivity f apacitiv and Inductiv upling in Submicrnic Intrcnncts Jan-Etinn Lrival, Dnis Dschacht, Yvs Quéré, Thirry L Guguc, Fabric Hurt T cit this vrsin: Jan-Etinn Lrival, Dnis Dschacht, Yvs Quéré,
More informationEinstein Equations for Tetrad Fields
Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for
More informationCosmological and Intrinsic Redshifts. November 19, 2010.
Csmlgical and Intrinsic Rdshifts Nvmbr 19, 21. Jsé Francisc García Juliá C/ Dr. Marc Mrncian, 65, 5. 4625 Valncia (Spain) E-mail: js.garcia@dival.s Abstract In a rcnt articl, a singl tird light mchanism,
More informationWhy is a E&M nature of light not sufficient to explain experiments?
1 Th wird world of photons Why is a E&M natur of light not sufficint to xplain xprimnts? Do photons xist? Som quantum proprtis of photons 2 Black body radiation Stfan s law: Enrgy/ ara/ tim = Win s displacmnt
More information15. Stress-Strain behavior of soils
15. Strss-Strain bhavior of soils Sand bhavior Usually shard undr draind conditions (rlativly high prmability mans xcss por prssurs ar not gnratd). Paramtrs govrning sand bhaviour is: Rlativ dnsity Effctiv
More informationDefinition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.
Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind
More information:2;$-$(01*%<*=,-./-*=0;"%/;"-*
!"#$%'()%"*#%*+,-./-*+01.2(.*3+456789*!"#$%"'()'*+,-."/0.%+1'23"45'46'7.89:89'/' ;8-,"$4351415,8:+#9' Dr. Ptr T. Gallaghr Astrphyscs Rsarch Grup Trnty Cllg Dubln :2;$-$(01*%
More informationOptoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30 10:55 PM
Optolctronics EE/OPE 451, OPT 444 Fall 009 Sction 1: T/Th 9:30 10:55 PM John D. Williams, Ph.D. Dpartmnt of Elctrical and Computr Enginring 406 Optics uilding UAHuntsvill, Huntsvill, AL 35899 Ph. (56)
More informationIVE(TY) Department of Engineering E&T2520 Electrical Machines 1 Miscellaneous Exercises
TRANSFORMER Q1 IE(TY) Dpartmnt of Enginring E&T50 Elctrical Machins 1 Miscllanous Exrciss Q Q3 A singl phas, 5 ka, 0/440, 60 Hz transformr gav th following tst rsults. Opn circuit tst (440 sid opn): 0
More information1 Isoparametric Concept
UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric
More informationFunctional Verification for SystemC Descriptions Using Constraint Solving
Functinal Vrificatin fr SystmC Dscriptins Using Cnstraint Slving Fabrizi Frrandi Plitcnic di Milan Dipartimnt di Elttrnica Infrmazin frrandi@lt.plimi.it Michl Rndin Plitcnic di Milan Dipartimnt di Elttrnica
More informationChemical Physics II. More Stat. Thermo Kinetics Protein Folding...
Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg
More informationAerE 344: Undergraduate Aerodynamics and Propulsion Laboratory. Lab Instructions
ArE 344: Undrgraduat Arodynamics and ropulsion Laboratory Lab Instructions Lab #08: Visualization of th Shock Wavs in a Suprsonic Jt by using Schlirn tchniqu Instructor: Dr. Hui Hu Dpartmnt of Arospac
More informationMulti-level Discrete Wavelet Transform Architecture Design
Prcdings f th Wrld Cngrss n Enginring 009 Vl I WCE 009, July - 3, 009, ndn, U.K. Multi-lvl Discrt Wavlt Transfrm Architctur Dsign Dhaha Dia, Mdin Zghid, Taufi Saidani, Mhamd Atri, Blgacm Buallgu, Mhsn
More informationMath 34A. Final Review
Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right
More informationWavelet-Based Method for Fog Signal Denoising
Jurnal f Autmatin and Cntrl Enginring, Vl., N. 2, Jun 23 Wavlt-Basd Mthd fr Fg Signal Dnising Yu Zu Cllg f Autmatin, Harbin Enginring Univrsity, Harbin, China Email: andrw22.zu@gmail.cm Jinchu Ca Dpartmnt
More informationContrast limited Adaptive Histogram Equalization and Discrete Wavelet Transform Method Used for Image Enhancement
2017 IJRI Vlum 2, Issu 8 ISSN: 2456-3315 Cntrast limitd Adaptiv Histgram qualizatin and Discrt Wavlt ransfrm Mthd Usd fr Imag nhancmnt 1 Smitha N, 2 Ujwala B S, 3 Dr. Manjunatha P, 4 Chthan L S 1 M.ch.
More information22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.
Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M
More informationEvaluating Reliability Systems by Using Weibull & New Weibull Extension Distributions Mushtak A.K. Shiker
Evaluating Rliability Systms by Using Wibull & Nw Wibull Extnsion Distributions Mushtak A.K. Shikr مشتاق عبذ الغني شخير Univrsity of Babylon, Collg of Education (Ibn Hayan), Dpt. of Mathmatics Abstract
More information(Upside-Down o Direct Rotation) β - Numbers
Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg
More informationPart 7: Capacitance And Capacitors
Part 7: apacitanc And apacitors 7. Elctric harg And Elctric Filds onsidr a pair of flat, conducting plats, arrangd paralll to ach othr (as in figur 7.) and sparatd by an insulator, which may simply b air.
More informationAnswer Homework 5 PHA5127 Fall 1999 Jeff Stark
Answr omwork 5 PA527 Fall 999 Jff Stark A patint is bing tratd with Drug X in a clinical stting. Upon admiion, an IV bolus dos of 000mg was givn which yildd an initial concntration of 5.56 µg/ml. A fw
More informationStatistical Thermodynamics: Sublimation of Solid Iodine
c:374-7-ivap-statmch.docx mar7 Statistical Thrmodynamics: Sublimation of Solid Iodin Chm 374 For March 3, 7 Prof. Patrik Callis Purpos:. To rviw basic fundamntals idas of Statistical Mchanics as applid
More informationWhat are those βs anyway? Understanding Design Matrix & Odds ratios
Ral paramtr stimat WILD 750 - Wildlif Population Analysis of 6 What ar thos βs anyway? Undrsting Dsign Matrix & Odds ratios Rfrncs Hosmr D.W.. Lmshow. 000. Applid logistic rgrssion. John Wily & ons Inc.
More informationContinuous probability distributions
Continuous probability distributions Many continuous probability distributions, including: Uniform Normal Gamma Eponntial Chi-Squard Lognormal Wibull EGR 5 Ch. 6 Uniform distribution Simplst charactrizd
More informationSpeeding Up Back-Propagation Neural Networks
Prcdings f t 005 Infrming Scinc and IT Educatin Jint Cnfrnc Spding Up Back-Prpagatin Nural Ntwrks Mammd A. Otair Jrdan Univrsity f Scinc and Tcnlgy, Irbd, Jrdan tair@just.du.j Walid A. Salam Princss Summaya
More informationVerification of Quality Parameters of a Solar Panel and Modification in Formulae of its Series Resistance
Verificatin f Quality Parameters f a Slar Panel and Mdificatin in Frmulae f its Series Resistance Sanika Gawhane Pune-411037-India Onkar Hule Pune-411037- India Chinmy Kulkarni Pune-411037-India Ojas Pandav
More informationIn this lecture... Subsonic and supersonic nozzles Working of these nozzles Performance parameters for nozzles
Lct-30 Lct-30 In this lctur... Subsonic and suprsonic nozzls Working of ths nozzls rformanc paramtrs for nozzls rof. Bhaskar Roy, rof. A M radp, Dpartmnt of Arospac, II Bombay Lct-30 Variation of fluid
More informationECE507 - Plasma Physics and Applications
ECE507 - Plasma Physics and Applications Lctur 7 Prof. Jorg Rocca and Dr. Frnando Tomasl Dpartmnt of Elctrical and Computr Enginring Collisional and radiativ procsss All particls in a plasma intract with
More informationCO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS
CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS Stig Holst ABB Automation Products Swdn Bapuji S Palki ABB Utilitis India This papr rports
More information2008 AP Calculus BC Multiple Choice Exam
008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl
More informationAnalytical Modelling of conventional DMG-SOI MOSFET using Different Gate Dielectric Material
Intrnational Journal of Enginring Tchnology, Managmnt and Applid Scincs www.ijtmas.com May 017, olum 5, Issu 5, ISSN 349-4476 Analytical Modlling of convntional DMG-SOI MOSFET using Diffrnt Gat Dilctric
More informationSolar Power Density cos. Module 10: Solar Energy. Solar Energy (Whr/m 2 /day) Zenith Angle 5/10/2009. Professor Mohamed A. El Sharkawi.
5/10/009 Mul 10: Slar Enrgy rfr Mham A. El Sharkawi Slar wr Dnity c t : lar pwr nity n arth in kw/m wa p : xtratrrtrial pwr nity (1.353 kw/m ) :znith angl (angl frm th utwar nrmal n th arth urfac t th
More informationOvercoming the shrink-and-swell effect in water level control strategy on industrial boiler-drum
Standard Scintific Rsarch and Essays Vol1 (1): 019-024, Fbruary 2013 http://www.standrsjournals.org/journals/ssre Rsarch Articl Ovrcoming th shrink-and-swll ffct in watr lvl control stratgy on industrial
More informationKinetic theory says that molecules are in constant motion. Perfume molecules moving across the room are evidence of this.
Chaptr 13- Th Stats f Mattr Gass- indfinit vum and shap, w dnsity. Liquids- dfinit vum, indfinit shap, and high dnsity. Sids- dfinit vum and shap, high dnsity Sids and iquids hav high dnsitis bcaus thir
More informationMEASURING HEAT FLUX FROM A COMPONENT ON A PCB
MEASURING HEAT FLUX FROM A COMPONENT ON A PCB INTRODUCTION Elctronic circuit boards consist of componnts which gnrats substantial amounts of hat during thir opration. A clar knowldg of th lvl of hat dissipation
More informationThe Language of SOCIAL MEDIA. Christine Dugan
Th Languag f SOCIAL MEDIA Christin Dugan Tabl f Cntnts Gt th Wrd Out...4 A Nw Kind f Languag...6 Scial Mdia Talk...12 Cnncting with Othrs...28 Changing th Dictinary...36 Glssary...42 Indx...44 Chck It
More informationsection 1 Influencing Change Toolkit How to: Influence People
Influncing Chang Tlkit Hw t: Influnc Ppl Influncing ppl mans having an ffct n thm, changing r mdifying thir viw. In rdr t influnc chang, w nd t influnc th ppl wh ar in a psitin t mak that chang happn.
More informationEstimation of apparent fraction defective: A mathematical approach
Availabl onlin at www.plagiarsarchlibrary.com Plagia Rsarch Library Advancs in Applid Scinc Rsarch, 011, (): 84-89 ISSN: 0976-8610 CODEN (USA): AASRFC Estimation of apparnt fraction dfctiv: A mathmatical
More informationorbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the
Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly
More informationCharacteristics of Gliding Arc Discharge Plasma
Caractristics of Gliding Arc Discarg Plasma Lin Li( ), Wu Bin(, Yang Ci(, Wu Cngkang ( Institut of Mcanics, Cins Acadmy of Scincs, Bijing 8, Cina E-mail: linli@imc.ac.cn Abstract A gliding arc discarg
More informationLast time. Resistors. Circuits. Question. Quick Quiz. Quick Quiz. ( V c. Which bulb is brighter? A. A B. B. C. Both the same
Last tim Bgin circuits Rsistors Circuits Today Rsistor circuits Start rsistor-capacitor circuits Physical layout Schmatic layout Tu. Oct. 13, 2009 Physics 208 Lctur 12 1 Tu. Oct. 13, 2009 Physics 208 Lctur
More information0WAVE PROPAGATION IN MATERIAL SPACE
0WAVE PROPAGATION IN MATERIAL SPACE All forms of EM nrgy shar thr fundamntal charactristics: 1) thy all tral at high locity 2) In traling, thy assum th proprtis of was 3) Thy radiat outward from a sourc
More informationNEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA
NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals
More information7.4 Potential Difference and Electric Potential
7.4 Potntial Diffrnc and Elctric Potntial In th prvious sction, you larnd how two paralll chargd surfacs produc a uniform lctric fild. From th dfinition of an lctric fild as a forc acting on a charg, it
More information1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:
Elctromagntic Induction. Lorntz forc on moving charg Point charg moving at vlocity v, F qv B () For a sction of lctric currnt I in a thin wir dl is Idl, th forc is df Idl B () Elctromotiv forc f s any
More information