Fuzzy logic controller for the maximum power point tracking in photovoltaic system
|
|
- Kristopher Turner
- 5 years ago
- Views:
Transcription
1 Intrnational Journal of Computr Applications ( ) Fuzzy logic controllr for th maximum powr point tracking in photovoltaic systm G. Balasubramanian Assistant Profssor Dpartmnt of Elctrical Enginring Annamalai Univrsity Annamalainagar-68 2, INDIA S. Singaravlu Associat Profssor Dpartmnt of Elctrical Enginring Annamalai Univrsity Annamalainagar-68 2, INDIA ABSTRACT This papr prsnts afuzzy logic controllr for maximum powr point tracking (MPPT) in photovoltaic systm.an asy and accurat mthod of modling photovoltaic arrays is proposd. Th modl and fuzzy basd control stratgis ar combind to form intllignt controllrs that ar mor accurat and robust.th modl basd controllr is dsignd such that th rfrnc signal for PWM gnrator of th convrtr can b adjustd to achiv maximum powr gnration from th photo voltaic systm. Th proposd fuzzy logic controllr shows bttr prformancs compard to th and MPPT basd approach.a MATLAB basd modling and simulation schm along with MPPT and fuzzy logic controllr is proposd which ar suitabl for studying th I-V and P-V charactristics of a PV array undr a non-uniform irradiation and diffrnt tmpratur. Th modl has bn xprimntally validatd. Gnral Trms Photovoltaic Array, DC-DC Boost convrtr, Fuzzy Logic Kywords MPPT convrtr, Non-linar approach, Choppr, Photovoltaic charactristics 1. INTRODUCTION In rcnt yars, rnwabl nrgy sourcs bcom mor significant sourc of nrgy. Among th rnwabl nrgy sourcs, solar nrgy is sustainabl with lss carbon missions [1-2].Th output powr of a PV array varis according to th sunlight conditions such as solar irradiation, shading and tmpratur. To obtain maximum powr from photovoltaic array, photovoltaic powr systm usually rquirs maximum powr point tracking (MPPT) controllr [3]. Various approachs hav bn rportd to implmnt MPPT such as prturb and obsrv () mthod [4-5], th incrmntal conductanc mthod, constant voltag mthod and short-circuit currnt mthod [6]. Using this mthod th maximum powr point can b found for spcifid solar irradiation and tmpratur condition but thy display oscillatory bhaviour around th maximum powr point undr normal oprating conditions. Morovr th systm will not rspond quickly to rapid changs in tmpratur or irradianc. On th othr hand th convntional controllrs ar fixdgain fdback controllrs. Thrfor thy cannot compnsat th paramtr variations in th procss and cannot adapt changs in th nvironmnt. -controlld systm is lss rsponsiv to ral and rlativly fast altrations in stat and so th systm will b slowr to rach th st point. Rcntly intllignt basd schms hav bn introducd [7-9].Among th intllignt basd mthods fuzzy logic controllr has its own mrits such that th MPPT algorithm can b asily formd. Th shap of th mmbrship function of th fuzzy logic controllrs can b adjustd such that th gap btwn th opration point and maximum powr point can b optimizd. Thrfor in th prsnt papr, an intllignt control tchniqu using fuzzy logic control associatd with a MPPT controllr ar usd to improv nrgy convrsion fficincy of th photovoltaic systm. Th proposd intllignt fuzzy logic procss compriss of xprt knowldg which xtracts maximum powr from a PV modul undr varying solar irradiation, tmpratur and load condition. Mathmatical modling of th systm and th simulation rsults using MATLAB / SIMULINK ar prsntd. Th fuzzy logic controllr basd rsults ar compard with th convntional tchniqus such as and controlling mthods which validat it mrits.an xprimntal stup of th proposd schm has bn built and th rsults obtaind on a PV arrayof 74.8W, 21.2 V, 4.4A rating is prsntd. 2. MODEL OF A PV ARRAY A PV cll can b rprsntd by an quivalnt circuit [1]as shown in Fig. 1. Th charactristics of this PV cll can b obtaind using standard quation (1). I PV D R P R S I PV R Load Fig 1: Equivalnt circuit of PV cll VPV I = I PV I O xp V+R S I 1 V+R SI V t a R p (1) I PV = photovoltaic currnt I O = saturation currnt V t = N S k T/q, thrmal voltag of array Ns = cll connctd in sris T = is th tmpratur of th p-n junction k = Boltzmann constant q = lctron charg R S = quivalnt sris rsistanc of th array R P = quivalnt paralll rsistanc of th array a = diod idality constant 22
2 Intrnational Journal of Computr Applications ( ) Fig. 1 shows th singl diod modl. A singl solar cll will produc only a limitd powr. Thrfor it is usual practic in ordr to gt dsird powr rating th solar clls ar connctd in paralll and sris circuits which form a modul. Such moduls ar again connctd in paralll and sris to form a solar array or panl to gt rquird voltag and currnt. Th quivalnt sris and paralll rsistanc of th array ar dnotd by th symbol R S and R P rspctivly in th quivalnt circuit. From th gnral I-V charactristic of th practical photovoltaic dvic on can b obsrv that th sris rsistanc R S valu will dominat in th voltag sourc rgion and th paralll rsistanc R P valu will dominat in th currnt sourc rgion of opration. Th gnral quation of a PV cll dscribs th rlationship btwn currnt and voltag of th cll. Sinc th valu of shunt rsistanc R P is high compard to valu of sris rsistanc R S th currnt through th paralll rsistanc can b nglctd. Th light gnratd currnt of th photovoltaic cll dpnds linarly on th solar irradiation and is also influncd by th tmpratur [11] givn by th quation (2) I PV = I PV,n + K I T G G n (2) I PV,n = is th light gnratd currnt at nominal condition (25 C and 1 W/ m 2 ) Δ T = T T n T = actual tmpratur [K] T n = nominal tmpratur [K] K I = currnt cofficints G = irradiation on th dvic surfac [W/m 2 ] G n = nominal irradiation Th currnt and voltag cofficints K V and K I ar includd as shown in quation (3) in ordr to tak th saturation currnt I O which is strongly dpndnt on th tmpratur. I O = I sc,n +K I T xp V oc,n +K V T 1 av t K V = voltag cofficints K I = currnt cofficints Th output voltag is incrasd (whr th currnt rmain unchangd) proportionally on numbr of idntical PV moduls connctd in sris(n sr ). Similarly th output currnt is incrasd (whr th voltag rmain unchangd) proportionally on numbr of idntical PV moduls connctd in paralll (N par ). It can b notd that th quivalnt sris and paralll rsistanc ar dirctly proportional to th numbr of sris moduls and invrsly proportional to th numbr of paralll moduls rspctivly. Th quation for array composd of N sr x N par givn by quation (4) I = I PV N par I O N par xp V+R S Nsr Npar V t an sr V+R S N sr Npar R P N sr Npar I 1 Th paramtr of solar array (KCP-1275 at 25 C, 1W/m 2 ) usd for thortical and xprimntal stup is givn in tabl-1. I (3) (4) PV Array I mp 4.4 A V oc 21.2 V V mp 17. V a 1.3 P max 74.8 W R s.511 Ω I sc 5.2 A R sh Ω N s 36 K v mv/ I O,n 9.83 x 1-8 A K I 2.8 ma/ DC-DC Convrtr (Boost) MPPT and Boost Controllr Tabl-1 3. DC DC BOOST CONVERTER A dual stag powr lctronic systm comprising a boost typ dc-dc convrtr and an invrtr is usd to fd th powr gnratd by th PV array to th load. To maintain th load voltag constant a DC-DC stp up convrtris introducd btwn th PV array and th invrtr.th block schmatic of th proposd schm is shown in Fig.2. In this schm a PV array fds DC-DC convrtr usd in stp-up configuration. Th voltag across th DC-DC convrtr is fd to a thr-phas, six-stp, quasisquar-wav IGBT invrtr a thr-phas fixd amplitud and fixd frquncy supply is obtaind to fd an isolatd load. Invrtr Control Logic Load Fig 2: Systm configuration for PV-basd systm fding powr to th load For a dc-dc boost convrtr, by using th avraging concpt, th input output voltag rlationship for continuous conduction mod is givn by Vo/Vin=1/(1 D) (5) Whr, D = duty cycl. Sinc th duty ratio D is btwn and 1 th output voltag must b highr than th input voltag in magnitud. It should b notd that th control logic of such dc-dc convrtr has to b diffrnt whn it is fd from a stiff DC sourc. Th duty ratio of th choppr is found to incras linarly with incras in cll tmpratur and hnc th intnsity. It has bn obsrvd that whn a PV array is connctd to a boost convrtr, incrasing th duty cycl incrass th avrag PV array currnt and as a rsult, PV array voltag dcrass. Thus, an incras in duty-cycl rsult in shifting th oprating point to th lft on th V-I charactristics of th PV array. Similarly dcrasing th duty cycl dcrass th avrag PV array currnt and as th PV array voltag incrass rsulting in shifting th oprating point of PV array to th right. As th invrtr DC voltag varis with irradiation to obtain constant amplitud and constant frquncy supply from th invrtr, a closd loop fuzzy controllr is incorporatd to automatically vary th duty-cycl of th DC-DC convrtr to obtain constant DC voltag at th invrtr input trminals.th invrtr output is thn applid to an isolatd load. 23
3 Intrnational Journal of Computr Applications ( ) 4. LOGIC MPPT CONTROLLER Th convntional controllrs ar fixd-gain fdback controllrs. Thrfor thy cannot compnsat th paramtr variations in th procss and cannot adapt changs in th nvironmnt. -controlld systm is lss rsponsiv to ral and rlativly fast altrations in stat and so th systm will b slowr to rach th st point. On th othr hand mthod for MPPT tracking will not rspond quickly to rapid changs in tmpratur or irradianc. Thrfor th fuzzy control algorithm is capabl of improving th tracking prformanc as compard with th classical mthods for both linar and nonlinar loads. Also, fuzzy logic is appropriat for nonlinar control bcaus it dos not us complx mathmatical quation. Th block diagram of fuzzy logic controllr (FLC) is shown in Fig.3. Th two FLC input variabls ar th rror E and chang of rror CE. Th bhavior of a FLCdpnds on th shap of mmbrship functions of th rul bas. Knowldg bas mthod. Hr w ar using MIN-MAX fuzzy implication mthod. 4.3 Dfuzzification Onc fuzzification is ovr, output fuzzy rang is locatd. Sinc at this stag a non-fuzzy valu of control is availabl a dfuzzification stag is ndd.cntroid dfuzzification mthod[12] is usd for dfuzzification in th proposd schm. nb nm ns zr ps pm pb Dgr of mmbrship1 Fig 5 (a): Mmbrship function plots for Inputs E(k) CE (k) Fuzzification Intrfac Dcision Making Logic Infrnc ngin Fig 3: Block of Fuzzy controllr Dfuzzification Intrfac Outp nb nm ns zr ps pm pb Dgr of mmbrship1 Fig 5(b): Mmbrship function plots for Δ Vr + Fuzzy logic - modl Vo Z-1 Procss Fig 4: Fuzzy logic control schm In this papr a fuzzy logic control schm (Fig.4) is proposd for maximum solar powr tracking of th PV array with an invrtr for supplying isolatd loads. Thy hav advantags to b robust and rlativly simpl to dsign sinc thy do not rquir th knowldg of th xact modl. On th othr hand th dsignr nds complt knowldg of th PV systm opration. 4.1 Fuzzification Thmmbrship function valus ar assignd to th linguistic variabls using svn fuzzy subst calld ngativ big (nb), ngativ mdium (nm), ngativ small (ns), zro(zr), positiv small (ps),positiv mdium (pm),positiv big (pb).fuzzy associativ mmory for th proposd systm is givn in Tabl-2.Variabl and Δ ar slctd as th input variabls, whr is th rror btwn th rfrnc voltag (Vr) and actual voltag (Vo) of th systm, Δ is th chang in rror in th sampling intrval. Th output variabl is th rfrnc signalfor PWM gnrator U. Triangular mmbrship functions ar slctd for all ths procss. Th rang of ach mmbrship function is dcidd by th prvious knowldg of th proposd schm paramtrs. 4.2 Infrnc ngin Infrnc ngin mainly consist of Fuzzy rul bas and fuzzy implication sub blocks. Th inputs ar now fuzzifid ar fd to th infrnc ngin and th rul bas is thn applid. Th output fuzzy st ar thn idntifid using fuzzy implication U Vo nb nm ns zr ps pm pb Dgr of mmbrship1 Fig 5(c): Mmbrship function plots for U U Tabl 2 Fuzzy associativ mmory for thproposd systm Δ nb nm ns zr ps pm pb nb nb nb nb nm nm ns zr nm nb nb nm nm ns zr ps ns nb nm nm ns zr ps pm zr nm nm ns zr ps pm pm ps nm ns zr ps pm pm pb pm ns zr ps pm pm pb pb pb zr ps pm pm pb pb pb Th mmbrship function of th variabls rror, chang in rror and chang in rfrnc signal for PWM gnrator ar shown in Fig. 5a-5c rspctivly. 5. RESULTS AND DISCUSSION A MATLAB basd modling and simulation schm (Appndix) along with MPPT and fuzzy logic controllr is proposd which ar suitabl for studying th I-V andp-v charactristics of a PV array undr a non-uniform irradiation and diffrnt tmpratur. Th fuzzy logic controllr basd rsults ar compard with th convntional tchniqus such as and controlling mthods which validat it mrits. 24
4 Control signal Panl Powr (W) Currnt (A) Powr (W) Intrnational Journal of Computr Applications ( ) 5.1 Simulation of Photovoltaic charactristics Th bhavior th PV clls and its charactristics ar discussd in this sction. It is found that th st of P-V&I-V charactristics ar highly nonlinar and dpndnt on solar irradianc of th PV array. Th combination of V and I that maximizs th output dpnds on irradiation and is also affctd by th tmpratur of th cll. 25 C 5 C 75 C 1 C 125 C Powr (W) Currnt (A) 1 W/m 2 8 W/m 2 6 W/m 2 4 W/m 2 2 W/m 2 Voltag (V) Fig 6(a): I-V Charactristics for diffrnt irradiations Voltag (V) Fig 6(b): P-V Charactristics Voltag (V) Fig 6(c): I-V Charactristics Voltag (V) Fig 6(d): P-V Charactristics for diffrnt tmpratur Fig.6(a)shows I-V charactristics of a PV cll. It can b obsrvd that as th cll tmpratur rmain constant, thpv output voltag rmains narly constant whil th PV output currnt incrass with incrasing solar intnsity. Fig.6(b)& Fig.6(c) shows P-V&I-V charactristics of a PV cll rspctivly. Fig.6(d) shows P-V curv plottd for diffrnt valus of tmpratur. 5.2 Simulation of, and Fuzzy logic MPPT Controllrs An xtnsiv simulation work nsurd ralizd MATLAB nvironmnt is prformd. Som slctd rsults ar prsntd with a comparison btwn systm incorporating diffrnt configurations as, and Fuzzy MPPT controllrs. To highlight th proposd systm good prformancs, th following simulation wr prsntd for fast solar irradianc [13] from 5 to 1 W/m 2 at fixd tmpraturof 25 C and fast dcras and incras in tmpratur variations from 4 C to 2 C and 2 C to 4 C rspctivly at fixd solar irradiancof 1w/m 2. From th simulation rsults, it can b dducd that th fuzzy controllr is fastr than controllr and in th transitional stat, and prsnt also much smothr signal with lss fluctuation in stady stat. 8 6 Fuzzy Tim (Sc) Tim (Sc) Fig 7: Rspons of th PV panl for a fast solar irradianc from 5 to 1W/m 2 at 25 c 25
5 Control Signal Panl Powr (W) Control Signal Panl Powr(W) Intrnational Journal of Computr Applications ( ) Tim(Sc) Tim(Sc) Fig 8: Rspons of th PV panl for a fast tmpratur variation from 4 c to 2 c at a solar irradianc of 1W/m E Tim(sc) Tim(Sc) Fig 9: Rspons of th PV panl for a fast tmpratur variation from 2 c to 4 c at a solar irradianc of 1W/m 2 6. EXPERIMENTAL INVESTIGATION Th PV array in th proposd schm shown in Fig.1(b) consist of solar PV array of 74.8W, 21.2V, 4.4A (15 panls connctd in sris). A load of 8Ω pr-phas was connctd in star across th invrtr trminals. A DC-DC convrtr (L=4μH, C=.25F) was constructd with IGBT (4 A, 6 V) as a switch with a switching frquncy of 2 KHz shown in Fig.1 (a). Th closd loop firing schm was mployd to triggr th DC-DC convrtr.a 5Hz, thr-phas IGBT invrtr was fabricatd, and a microcontrollr C 16F877A was usd to triggr th IGBT in 18 dgr conduction mod. Th abov schm was tstd for diffrnt conditions of irradiations. Fig 1(a): DC-DC-Convrtr - Invrtr Fig 1(b): Solar Panl 26
6 Intrnational Journal of Computr Applications ( ) Th simulatd thr phas voltag and currntwavform at th output of th invrtr shown in Fig. 11(a). Th simulatd currnt wavform (Fig. 11(b)) shows, vn though th load is applid at.8 sconds th voltag across th load rmains constant. Currnt (A) Voltag (V) Currnt (A) Voltag (V) Tim (sc) Fig 11(a): Simulatd Voltag & currnt wavform at output of th invrtr undr nominal load Tim (sc) Fig 11(b): Simulatd Voltag & currnt wavform at output of th invrtr undr suddn chang in load Fig 12: Voltag and currnt wavform (xprimntal) (On phas alon shown for clarity) Th xprimntal voltag and currnt wavform (on phas alon shown for clarity) at th output of th invrtr is shown in Fig. 12. Som harmonics hav bn introducd in th proposd schm found in th wavforms it can b liminatd by introducing ncssary filtrs. 7. CONCLUSION A simpl powr lctronic controllr for intrfacing photovoltaic arrays with DC-DC convrtr has bn dvlopd. By applying th puls width modulation (PWM) control schm with appropriat MPPT algorithm to th powr switchs and th DC-DC convrtr can draw maximum powr from photovoltaic array. Th rsults obtaind from th xprimntal invstigation and simulation studis of th proposd schm ar compard and it has bn found that th simulation rsults closly agr with th xprimntally obtaind rsults, thus validating th xprimntal powr circuit and control circuits of th invrtr. So, th fuzzy logic control is an ffctiv tool to track and xtract maximum powr to th isolatd load. 8. ACKNOWLEDGEMENT Th authors thank th authoritis of Annamalai Univrsity for th facilitis providd. 9. REFERENCES [1] Mayssa Farhat and Lassaad Sbita, Advancd Fuzzy MPPT Control Algorithm for Photovoltaic Systm, Scinc Acadmy Transactions on Rnwabl Enrgy Systms Enginring and Tchnology, 211, vol. 1, no. 1, pp , Mar [2] T. Tafticht, K. Agbossou, M.L. Doumbia, and A. Chriti, An Improvd Maximum powr point tracking mthod for photovoltaic systm, Rnwabl nrgy, vol.33, pp , 28. [3] Yun Tiam Tan, Danil S. Kirschn, and Nicholas Jnkins, A Modl basd PV Gnration suitabl for stability analysis, IEEE trans. on nrgy conv., vol.19, no.4, pp , Dc.24. [4] C. R. Sullivan and M. J. Powrs, A high-fficincy maximum powr point trackr for photovoltaic array in a solar-powrd rac vhicl, in Proc. IEEE PESC, [5] N. Fmia, Optimizing Duty-cyclPrturbation of MPPT Tchniqu,35th Annual IEEE Powr ElctronicsSpcialists Confrnc.,24. [6] E. Koutroulis E, K. Kalaitzakis, and NC. Voulgaris, Dvlopmnt of a microcontrollr basd photovoltaic maximum powr point tracking control sytm, IEEE trans. on Powr Elctronics, vol. 16, no. 1, pp , 21. [7] Abdulhadi Varnham, M. Abdulrahman, Al-Ibrahim, S. Gurvindr, Virk, and Djaml Azzi, Soft computing modl basd controllrs for incrasd photovoltaic plant fficincis, IEEE trans. on nrgy conv., vol. 22, no. 4, pp , Dc. 27. [8] A. Damak1, A. Gusmi and A. Mami, Modling and fuzzy control of a photovoltaic-assistd watring systm, Journal of Enginring and Tchnology Rsarch, Vol.1, pp. 7-13, 29. [9] B.Krishna Kumar, Matlab basd Modlling of Photovoltaic Panls and thir Efficint, Utilization for Maximum Powr Gnration, 1st National Confrnc on Intllignt Elctrical Systms, NCIES, Salm, India, pp ,
7 Intrnational Journal of Computr Applications ( ) [1] M.G.Villalva, J.R.Gazol, and E.R.Filho, Comprhnsiv Approach to Modling and Simulation of Photovoltaic Arrays", IEEE trans. on Powr Elctronics, vol.24, no.5, pp , May 29. [11] H. Patl, and V. Agarwal, MATLAB basd modling to study th ffcts of partial shading on PV array charactristics, IEEE trans. on nrgy conv., vol. 23, no.1, pp , Mar. 28. [12] Timothy, andj. Ross, Fuzzy logic with nginring applications, McGraw hill intrnational ditions, Elctrical nginring sris, Nw York, [13] C. Larbs, S.M. AitChikh and T. Obidi, Gntic alogorithms optimizd fuzzy logic control for th maximum powr point tracking in photovoltaic systm, Rnwabl Enrgy., vol. 34, no.1, pp , Oct. 29. APPENDIX A MATLAB basd modling and simulation schm along with MPPT and fuzzy logic controllr is proposd (Fig. 13) which ar suitabl for studying th I-V and P-V charactristics of a PV array undr a non-uniform irradiation and diffrnt tmpratur. Th configuration of th proposd schm is simulatd undr diffrnt condition of irradiations (.4 kw/m 2 to1kw/m 2 ) in th powr systm block st platform of th MATLAB. Th simulatd currnt wavform (Fig.11(b)) shows, vn though suddn chang in load is applid at.8 sconds th voltag across th load rmains constant. In ordr to achiv th load voltag constant th actual voltag fd to th invrtr is compard with th rfrnc maximum voltag that can b obtaind at th load for a givn V oc and I sc.th rror is calculatd and accordingly th rfrnc signal to th PWM gnrator is changd in ordr to maintain th load voltag constant. Fig 13: Photovoltaic and MPPT Fuzzy controllr implmntd in SIMULINK 28
Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a
204 Intrnational Confrnc on Computr Scinc and Elctronic Tchnology (ICCSET 204) Rotor Stationary Control Analysis Basd on Coupling KdV Equation Finit Stady Analysis Liu Dalong,a, Xu Lijuan2,a Dpartmnt of
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 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 informationFull Order Observer Controller Design for Two Interacting Tank System Based on State Space Approach
Intrnational Journal of Application or Innovation in Enginring & Managmnt (IJAIEM) Wb Sit: www.ijaim.org Email: ditor@ijaim.org Volum 6, Issu 7, July 07 ISSN 39-4847 Full Ordr Obsrvr Controllr Dsign for
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 informationFinite Element Model of a Ferroelectric
Excrpt from th Procdings of th COMSOL Confrnc 200 Paris Finit Elmnt Modl of a Frrolctric A. Lópz, A. D Andrés and P. Ramos * GRIFO. Dpartamnto d Elctrónica, Univrsidad d Alcalá. Alcalá d Hnars. Madrid,
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 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 informationNumerical considerations regarding the simulation of an aircraft in the approaching phase for landing
INCAS BULLETIN, Volum, Numbr 1/ 1 Numrical considrations rgarding th simulation of an aircraft in th approaching phas for landing Ionl Cristinl IORGA ionliorga@yahoo.com Univrsity of Craiova, Alxandru
More informationThe influence of electron trap on photoelectron decay behavior in silver halide
Th influnc of lctron trap on photolctron dcay bhavior in silvr halid Rongjuan Liu, Xiaowi Li 1, Xiaodong Tian, Shaopng Yang and Guangshng Fu Collg of Physics Scinc and Tchnology, Hbi Univrsity, Baoding,
More informationRecursive Estimation of Dynamic Time-Varying Demand Models
Intrnational Confrnc on Computr Systms and chnologis - CompSysch 06 Rcursiv Estimation of Dynamic im-varying Dmand Modls Alxandr Efrmov Abstract: h papr prsnts an implmntation of a st of rcursiv algorithms
More informationDynamic Performance Simulation of Hybrid Excitation Claw-pole Alternator
Intrnational Confrnc on Enrgy, Powr and Elctrical Enginring (EPEE 016) Dynamic Prformanc Simulation of Hybrid Excitation Claw-pol Altrnator Jiapng Li 1, Changqing Zhu 1,*, Min Cong and Yiming Shn 1 1 School
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 informationThe Control of Electromagnetic Filter by Using FPGA Based PI Type Fuzzy Controller
Th Control of Elctromagntic Filtr by Using FPGA Basd PI Typ Fuzzy Controllr Ilkr Ali OZKAN a, Ismail SARITAS b, Saadtdin HERDEM b a Dpartmnt of Computr Enginring, b Dpartmnt of Elctrical and Elctronics
More informationHomotopy perturbation technique
Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,
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 informationDetermination of Vibrational and Electronic Parameters From an Electronic Spectrum of I 2 and a Birge-Sponer Plot
5 J. Phys. Chm G Dtrmination of Vibrational and Elctronic Paramtrs From an Elctronic Spctrum of I 2 and a Birg-Sponr Plot 1 15 2 25 3 35 4 45 Dpartmnt of Chmistry, Gustavus Adolphus Collg. 8 Wst Collg
More informationA Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes
Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical
More informationA Propagating Wave Packet Group Velocity Dispersion
Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to
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 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 informationHigher order derivatives
Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss 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 informationA General Thermal Equilibrium Discharge Flow Model
Journal of Enrgy and Powr Enginring 1 (216) 392-399 doi: 1.17265/1934-8975/216.7.2 D DAVID PUBLISHING A Gnral Thrmal Equilibrium Discharg Flow Modl Minfu Zhao, Dongxu Zhang and Yufng Lv Dpartmnt of Ractor
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 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 informationApplication of Vague Soft Sets in students evaluation
Availabl onlin at www.plagiarsarchlibrary.com Advancs in Applid Scinc Rsarch, 0, (6):48-43 ISSN: 0976-860 CODEN (USA): AASRFC Application of Vagu Soft Sts in studnts valuation B. Chtia*and P. K. Das Dpartmnt
More informationFull Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient
Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full
More informationSTABILITY ANALYSIS OF FUZZY CONTROLLERS USING THE MODIFIED POPOV CRITERION
SABILIY ANALYSIS OF FUZZY CONROLLERS USING HE MODIFIED POPOV CRIERION Mauricio Gonçalvs Santana Junior Instituto cnológico d Aronáutica Pça Mal Eduardo Goms, 50 Vila das Acácias - CEP 2228-900 São José
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 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 informationLinear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let
It is impossibl to dsign an IIR transfr function with an xact linar-phas It is always possibl to dsign an FIR transfr function with an xact linar-phas rspons W now dvlop th forms of th linarphas FIR transfr
More informationKoch Fractal Boundary Single feed Circularly Polarized Microstrip Antenna
1 Journal of Microwavs, Optolctronics and Elctromagntic Applications, Vol. 6, No. 2, Dcmbr 2007 406 Koch Fractal Boundary Singl fd Circularly Polarizd Microstrip Antnna P. Nagswara Rao and N. V. S.N Sarma
More informationSimulated Analysis of Tooth Profile Error of Cycloid Steel Ball Planetary Transmission
07 4th Intrnational Matrials, Machinry and Civil Enginring Confrnc(MATMCE 07) Simulatd Analysis of Tooth Profil Error of Cycloid Stl Ball Plantary Transmission Ruixu Hu,a, Yuquan Zhang,b,*, Zhanliang Zhao,c,
More information2/12/2013. Overview. 12-Power Transmission Text: Conservation of Complex Power. Introduction. Power Transmission-Short Line
//03 Ovrviw -owr Transmission Txt: 4.6-4.0 ECEGR 45 owr ystms Consrvation of Complx owr hort in owr Transmission owr Transmission isualization Radial in Mdium and ong in owr Transmission oltag Collaps
More informationStudies of Turbulence and Transport in Alcator C-Mod Ohmic Plasmas with Phase Contrast Imaging and Comparisons with GYRO*
Studis of Turbulnc and Transport in Ohmic Plasmas with Phas Contrast Imaging and Comparisons with GYRO* L. Lin 1, M. Porkolab 1, E.M. Edlund 1, J.C. Rost 1, M. Grnwald 1, D.R. Mikklsn 2, N. Tsujii 1 1
More informationCh. 24 Molecular Reaction Dynamics 1. Collision Theory
Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic
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 informationTRANSISTOR AND DIODE STUDIES. Prof. H. J. Zimmermann Prof. S. J. Mason C. R. Hurtig Prof. R. B. Adler Dr. W. D. Jackson R. E.
XI. TANSISTO AND DIODE STUDIES Prof. H. J. Zimmrmann Prof. S. J. Mason C.. Hurti Prof.. B. Adlr Dr. W. D. Jackson. E. Nlson A. DESIGN OF TANSFOMEESS TANSISTO AUDIO AMPIFIES Considrabl ffort by many oranizations
More informationSlide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS
Slid DIGITAL SIGAL PROCESSIG UIT I DISCRETE TIME SIGALS AD SYSTEM Slid Rviw of discrt-tim signals & systms Signal:- A signal is dfind as any physical quantity that varis with tim, spac or any othr indpndnt
More informationA Recent Approach to Repetitive Control Strategy for Induced Draft Fan
Europan Journal of Applid Scincs 9 (5): 258-264, 217 ISSN 279-277 IDOSI Publications, 217 DOI: 1.5829/idosi.jas.217.258.264 A Rcnt Approach to Rptitiv Control Stratgy for Inducd Draft Fan 1 1 1 2 G. Thanigaivl,
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 informationElectronic Circuits. BJT Amplifiers. Manar Mohaisen Office: F208 Department of EECE
Elctronic Circuits BJT mplifirs Manar Mohaisn Offic: F208 Email: manar.subhi@kut.ac.kr Dpartmnt of EECE viw of th Prcdnt Lctur Explain th DC Oprating Point Explain th Voltag-dividr Bias Othr Bias Mthods
More information5.80 Small-Molecule Spectroscopy and Dynamics
MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts
More informationRational Approximation for the one-dimensional Bratu Equation
Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in
More informationA Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction
Int. J. Opn Problms Compt. Math., Vol., o., Jun 008 A Pry-Prdator Modl with an Altrnativ Food for th Prdator, Harvsting of Both th Spcis and with A Gstation Priod for Intraction K. L. arayan and. CH. P.
More informationLINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM
Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL
More informationQuasi-Classical States of the Simple Harmonic Oscillator
Quasi-Classical Stats of th Simpl Harmonic Oscillator (Draft Vrsion) Introduction: Why Look for Eignstats of th Annihilation Oprator? Excpt for th ground stat, th corrspondnc btwn th quantum nrgy ignstats
More informationKinetic Integrated Modeling of Heating and Current Drive in Tokamak Plasmas
1 HW/P-1 Kintic Intgratd Modling of Hating and Currnt riv in okamak Plasmas A. Fukuyama 1), H. Nuga 1), S. Murakami 1) 1) Graduat School of Enginring, Kyoto Univrsity, Kyoto, Japan -mail contact of main
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 informationTwo Products Manufacturer s Production Decisions with Carbon Constraint
Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint
More informationThermodynamical insight on the role of additives in shifting the equilibrium between white and grey tin
hrmodynamical insight on th rol of additivs in shifting th quilibrium btwn whit and gry tin Nikolay Dmntv Dpartmnt of Chmistry, mpl Univrsity, Philadlphia, PA 19122 Abstract In this study mthods of statistical
More informationEXST Regression Techniques Page 1
EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy
More informationGENERATING GAUSSIAN FUNCTIONS USING LOW- VOLTAGE MOS-TRANSLINEAR CIRCUITS
ENERATN AUSSAN FUNCTONS USN O- OTAE MOS-TRANSNEAR CRCUTS SANCHEZ-OPEZ CAROS 1, AZ-SANCHEZ AEJANRO, TEO-CUAUTE ESTEBAN Elctronics partmnt NAOE uis Enriqu Erro no. 1. P.O.Box 51 and 16. 7 MEXCO Abstract:
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 informationDavisson Germer experiment
Announcmnts: Davisson Grmr xprimnt Homwork st 5 is today. Homwork st 6 will b postd latr today. Mad a good guss about th Nobl Priz for 2013 Clinton Davisson and Lstr Grmr. Davisson won Nobl Priz in 1937.
More informationSliding Mode Flow Rate Observer Design
Sliding Mod Flow Rat Obsrvr Dsign Song Liu and Bin Yao School of Mchanical Enginring, Purdu Univrsity, Wst Lafaytt, IN797, USA liu(byao)@purdudu Abstract Dynamic flow rat information is ndd in a lot of
More informationEffects of Electron Model on Three-Grid Ion Engine Analyses
Effcts of Elctron Modl on Thr-Grid Ion Engin Analyss IEPC-2011-205 Prsntd at th 32nd Intrnational Elctric Propulsion Confrnc, Wisbadn Grmany Takshi Miyasaka 1 and Katsuo Asato 2 Gifu Univrsity, Gifu, 501-1193,
More informationDynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA *
17 nd Intrnational Confrnc on Mchanical Control and Automation (ICMCA 17) ISBN: 978-1-6595-46-8 Dynamic Modlling of Hoisting Stl Wir Rop Da-zhi CAO, Wn-zhng DU, Bao-zhu MA * and Su-bing LIU Xi an High
More informationImpact of the Sampling Period on the Design of Digital PID Controllers
Impact of th Sampling Priod on th Dsign of Digital PID Controllrs Dimitris Tsamatsoulis Halyps Building Matrials S.A. 17 th klm Nat. Road Athns Korinth, Aspropyrgos, Grc d.tsamatsoulis@halyps.gr Abstract
More informationAutotuning of Digitally Controlled Buck Converters based on Relay Feedback
Autotuning of Digitally Controlld Buck Convrtrs basd on Rlay Fdback W. Stfanutti, P. Mattavlli DIEGM Univrsity of Udin Italy [stfanutti,mattavlli]@uniud.it S. Saggini ST Microlctronics Industrial & Powr
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 informationHospital Readmission Reduction Strategies Using a Penalty-Incentive Model
Procdings of th 2016 Industrial and Systms Enginring Rsarch Confrnc H. Yang, Z. Kong, and MD Sardr, ds. Hospital Radmission Rduction Stratgis Using a Pnalty-Incntiv Modl Michll M. Alvarado Txas A&M Univrsity
More informationTorque Ripple Minimization in Switched Reluctance Motor Using Passivity-Based Robust Adaptive Control
Intrnational Journal of Elctrical and Elctronics Enginring 5: orqu Rippl Minimization in Switchd Rluctanc Motor Using Passivity-Basd Control M.M. Namazi, S.M. Saghaiannjad, and A. Rashidi Abstract In this
More informationLife Science Journal 2013;10(4) Thyristor Controlled Series Capacitor (TCSC) for Power System Stabilization
Thyristor Controlld Sris Capacitor () or or Systm Stabilization Mansour Babikr dris and Ali Juma Elzubia Dpt. o Elctrical Enginring, Faculty o Enginring, Misurata Univrsity Abstract: Th dynamic stability
More informationAn Extensive Study of Approximating the Periodic. Solutions of the Prey Predator System
pplid athmatical Scincs Vol. 00 no. 5 5 - n xtnsiv Study of pproximating th Priodic Solutions of th Pry Prdator Systm D. Vnu Gopala Rao * ailing addrss: Plot No.59 Sctor-.V.P.Colony Visahapatnam 50 07
More informationSIMPLE ONE-DIMENSIONAL CALCULATION OF HALL THRUSTER FLOWFIELDS
SIMPLE ONE-DIMENSIONAL CALCULATION OF HALL THRUSTER FLOWFIELDS Hirokazu Tahara, Takashi Fujioka, Atsushi Shirasakiand Takao Yoshikawa Graduat School of Enginring Scinc, Osaka Univrsity 1-3, Machikanyama,
More informationProcdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is
Procdings of IC-IDC0 EFFECTS OF STOCHASTIC PHASE SPECTRUM DIFFERECES O PHASE-OLY CORRELATIO FUCTIOS PART I: STATISTICALLY COSTAT PHASE SPECTRUM DIFFERECES FOR FREQUECY IDICES Shunsu Yamai, Jun Odagiri,
More informationCalculation of electromotive force induced by the slot harmonics and parameters of the linear generator
Calculation of lctromotiv forc inducd by th lot harmonic and paramtr of th linar gnrator (*)Hui-juan IU (**)Yi-huang ZHANG (*)School of Elctrical Enginring, Bijing Jiaotong Univrity, Bijing,China 8++58483,
More informationTransitional Probability Model for a Serial Phases in Production
Jurnal Karya Asli Lorkan Ahli Matmatik Vol. 3 No. 2 (2010) pag 49-54. Jurnal Karya Asli Lorkan Ahli Matmatik Transitional Probability Modl for a Srial Phass in Production Adam Baharum School of Mathmatical
More informationA nonequilibrium molecular dynamics simulation of evaporation
Intrnational Confrnc Passiv and Low Enrgy Cooling 543 A nonquilibrium molcular dynamics simulation of vaporation Z.-J. Wang, M. Chn and Z.-Y. Guo Dpartmnt of Enginring Mchanics, Tsinghua Univrsity, Bijing
More informationChapter 8: Electron Configurations and Periodicity
Elctron Spin & th Pauli Exclusion Principl Chaptr 8: Elctron Configurations and Priodicity 3 quantum numbrs (n, l, ml) dfin th nrgy, siz, shap, and spatial orintation of ach atomic orbital. To xplain how
More informationBackground: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.
Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby
More informationTitle: Vibrational structure of electronic transition
Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum
More informationBifurcation Theory. , a stationary point, depends on the value of α. At certain values
Dnamic Macroconomic Thor Prof. Thomas Lux Bifurcation Thor Bifurcation: qualitativ chang in th natur of th solution occurs if a paramtr passs through a critical point bifurcation or branch valu. Local
More informationTopology Optimization of Suction Muffler for Noise Attenuation
Purdu Univrsity Purdu -Pubs Intrnational Comprssor Enginring Confrnc School of Mchanical Enginring 2012 Topology Optimization of Suction Mufflr for Nois Attnuation Jin Woo L jinwool@ajou.ac.kr Dong Wook
More informationFinite element discretization of Laplace and Poisson equations
Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization
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 informationLecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac.
Lctur 2: Discrt-Tim Signals & Systms Rza Mohammadkhani, Digital Signal Procssing, 2015 Univrsity of Kurdistan ng.uok.ac.ir/mohammadkhani 1 Signal Dfinition and Exampls 2 Signal: any physical quantity that
More informationContemporary, atomic, nuclear, and particle physics
Contmporary, atomic, nuclar, and particl physics 1 Blackbody radiation as a thrmal quilibrium condition (in vacuum this is th only hat loss) Exampl-1 black plan surfac at a constant high tmpratur T h is
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 informationPerformance Prediction of the Single-Sided Linear. Induction Motors for Transportation Considers. Longitudinal End Effect by Using Analytic Method
Contmporary Enginring Scincs, Vol., 9, no., 95-14 Prformanc Prdiction of th Singl-Sidd Linar Induction Motors for Transportation Considrs Longitudinal End Effct by Using Analytic Mthod Ali Suat Grçk Univrsity
More informationISSN Article. Analysis of the Coupling Behavior of PEM Fuel Cells and DC-DC Converters
Enrgis 29, 2, 71-96; doi:1.339/n2171 OPEN ACCESS nrgis ISSN 1996-173 www.mdpi.com/journal/nrgis Articl Analysis of th Coupling Bhavior of PEM Ful Clls and DC-DC Convrtrs Markus Grötsch 1,, Michal Mangold
More informationOptics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007
Optics and Non-Linar Optics I - 007 Non-linar Optics Tutorial Sht Novmbr 007 1. An altrnativ xponntial notion somtims usd in NLO is to writ Acos (") # 1 ( Ai" + A * $i" ). By using this notation and substituting
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 information2. Laser physics - basics
. Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"
More informationPHASE-ONLY CORRELATION IN FINGERPRINT DATABASE REGISTRATION AND MATCHING
Anall Univrsităţii d Vst din Timişoara Vol. LII, 2008 Sria Fizică PHASE-OLY CORRELATIO I FIGERPRIT DATABASE REGISTRATIO AD ATCHIG Alin C. Tusda, 2 Gianina Gabor Univrsity of Orada, Environmntal Faculty,
More informationIterative learning control with initial rectifying action for nonlinear continuous systems X.-D. Li 1 T.W.S. Chow 2 J.K.L. Ho 3 J.
Publishd in IET Control Thory and Applications Rcivd on 24th Dcmbr 27 Rvisd on 21st May 28 doi: 1.149/it-cta:27486 ISSN 1751-8644 Itrativ larning control with initial rctifying action for nonlinar continuous
More informationESE (Prelims) - Offline Test Series ELECTRICAL ENGINEERING SUBJECT: Power Electronics & Drives, Power Systems and Signals & Systems SOLUTIONS
TEST ID: 8 ESE- 9 (Prlims) - Offlin Tst Sris ELECTRICAL ENGINEERING Tst-5 SUBJECT: Powr Elctronics & Drivs, Powr Systms and Signals & Systms SOLUTIONS. Ans: (b) Powr diod rcovry dpnds on th charg stord
More informationA New Optical Waveguide for Implementation of Multi-wavelengths Narrowband Filters for DWDM Systems
IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.6 No.8B, August 6 39 A Nw Optical Wavguid for Implmntation of Multi-wavlngths Narrowband Filtrs for DWDM Systms A. Rostami [a, b] a)-
More informationTypes of Transfer Functions. Types of Transfer Functions. Types of Transfer Functions. Ideal Filters. Ideal Filters
Typs of Transfr Typs of Transfr x[n] X( LTI h[n] H( y[n] Y( y [ n] h[ k] x[ n k] k Y ( H ( X ( Th tim-domain classification of an LTI digital transfr function is basd on th lngth of its impuls rspons h[n]:
More informationProblem Set 6 Solutions
6.04/18.06J Mathmatics for Computr Scinc March 15, 005 Srini Dvadas and Eric Lhman Problm St 6 Solutions Du: Monday, March 8 at 9 PM in Room 3-044 Problm 1. Sammy th Shark is a financial srvic providr
More informationNusselt number correlations for simultaneously developing laminar duct flows of liquids with temperature dependent properties
Journal of Physics: Confrnc Sris OPEN ACCESS Nusslt numbr corrlations for simultanously dvloping laminar duct flows of liquids with tmpratur dpndnt proprtis To cit this articl: Stfano Dl Giudic t al 2014
More informationTREATMENT OF THE PLASMA NONLINEAR ABSORPTION LAW AT LINEARLY POLARIZED LASER RADIATION OF RELATIVISTIC INTENSITIES. A. G.
Armnian Journal of Physics, 15, vol. 8, issu, pp. 64-7 TREATMENT OF THE PLASMA NONLINEAR ABSORPTION LAW AT LINEARLY POLARIZED LASER RADIATION OF RELATIVISTIC INTENSITIES A. G. Ghazaryan Cntr of Strong
More informationMCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems
MCE503: Modling and Simulation o Mchatronic Systms Discussion on Bond Graph Sign Convntions or Elctrical Systms Hanz ichtr, PhD Clvland Stat Univrsity, Dpt o Mchanical Enginring 1 Basic Assumption In a
More informationThe graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the
Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th
More informationDynamic response of a finite length euler-bernoulli beam on linear and nonlinear viscoelastic foundations to a concentrated moving force
Journal of Mchanical Scinc and Tchnology 2 (1) (21) 1957~1961 www.springrlink.com/contnt/1738-9x DOI 1.17/s1226-1-7-x Dynamic rspons of a finit lngth ulr-brnoulli bam on linar and nonlinar viscolastic
More informationSearch sequence databases 3 10/25/2016
Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an
More informationModified Direct Torque Control for Single-phase Induction Motor Drives
Modifid Dirct Torqu Control for Singl-phas Induction Motor Drivs THANATCHAI KULWORAWANICHPONG and TAWAT CHUCHIT Powr Systm Rsarch Unit School of Elctrical Enginring Suranar Univrsity of Tchnology Univrsity
More information