SIMPLIFIED sra11c AND DYNAMIC MODELS OF THE 3-LOOP ACI1VE POWER FACTOR CORREC11ON SYSTEMS
|
|
- Jane Powell
- 5 years ago
- Views:
Transcription
1 J q7j ft SIMPLIFIED srac AND DYNAMIC MODELS OF THE 3-LOOP ACIVE POWER FACTOR CORRECON SYSTEMS A. Abramvitz and S. Ben- Yaav Department f Electrical and Cmputer Engineering Ben-Gurin University f the Negev P. 0. Bx 653, Beer-Sheva 8405, ISRAEL Tel: ; Fax: ; Emai: sby@bguee.bgu.ac.il Abstract. Simple static and dynamic mdels f the 3-lp Active Pwer Factr Crrectin (APFC) system are suggested and analyzed. Analytical expressins fr the gain cnstants and the transfer functins f the feedbac and feedfrward lps f the APFC cntrller circuits are btained and their influence n the static and dynamic behavir f the APFC system is discussed. The thery is supprted by cmputer simulatin. Ke~wrds. PFC, mdeling. Intrductin Active Pwer Factr Crrectin (APFC) systems are generally designed arund high frequency cnverters that are cntrlled by tw feedbac lps. The average utput ltage is regulated by an uter lp whereas the inner lp shapes the line current [I]. The reference f the inner current lp is generated by mdulating the rectified pwer line ltage by the uter lp errr signal. Thus the magnitude f the reference is adjusted dynamically t cmply with the pwer requirements f the lad. The cntrl signal fr the inner lp, needed fr adjusting the current level, is cnveniently derived by cmparing the average current level t the desired reference value. The 3- lp APFC cntrller [-4] generates the current reference signal fr the inner lp by the multiplier-squarer-divider circuit as shwn at Fig. I. The inherent nn-linearity f the reference signal analg cmputatin blc and time varying gains f the pwer stage f the APFC systems pse a cntrl prblem. It is clear that the uter lp f the APFC must have nt nly a slw respnse (limited bandwidth) but als a lw gain s that the utput ripple will be heavily attenuated. Otherwise, while stabilizing the utput ltage, the utput ripple will distrt the input current by penetrating int the reference f the current lp. Hwever, the lw feedbac gain may result in a significant steady state errr, which is interpreted as pr utput ltage regulatin r high utput impedance. The bjective f this paper is t present simple static and dynamic mdels that culd be used in analysis and design f the 3-lp APFC systems. We btain the analytical expressins fr the gains f the feedbac and feedfrward lps f the APFC t characterize the systems lw frequency and static behavir. The prpsed mdels were investigated analytically and verified by simulatin. Basic relatinships The usual case f the APFC is when it is fed tm a AC line. The 3-lp APFC cntrller [-4] generals the current reference signal fr the inner lp by the multipliersquarer-divider circuit as shwn at Fig. I. When driven by a sinusidal line ltage vin (9) = y m sin9, the APFC generates the input current by the fllwing algrithm: iin (9) = Im sin9 = K ( Ye )( ~ }v m'in. ) () Fig. I. The 3-lp APFC system blc diagram. Here 9 is the pwer line angle. ve is the ltage feedbac errr amplifier signal and K is the system gain cnstant. Thus in it's steady state the input current is f a sinusidal shape and in phase with the input ltage. Its amplitude Im is directly prprtinal t the errr amplifier ltage ve and inversely prprtinal ltage V m : t the amplitude f the line Im=K(~) () Due t this relatinship, the average input pwer p av is independent f the amplitude f the line ltage and is a linear functin f the errr amplifier ltage: ImVm K Pav=~=ve(9) (3) The steady state ltage feedbac errr amplifier signal ve(9) appeared in the eq. () abve may be expressed as: ve(9)= (Ve-VT)+ve(9) (4) This expressin cntains a dc term, in bracets, and the secnd harmnics ripple cmpnent ve(9) as well. The term Ve represents the perating pint f the errr amplifier and VT is the threshld ltage f the divider input. The threshld VT set t be greater than the lw saturatin level f the errr amplifier. When the pwer demands f the lad drps, the errr amplifier signal swings belw the threshld, cutts ff the input current bringing the pwer level t zer. It is the difference (Ve -VT) which gverns the steady state pwer flw. The secnd harmnic cmpnent ve(9) at the utput f the ltage errr amplifier, appears as respnse t the utput ltage ripple. This signal is f a lw amplitude and
2 des nt cntribute significantly t the pwer flw and thus wuld nt be f ur cncern here. Hwever, it is ne f the main causes fr input current distrtin. The pwer gain cnstant As stated abve, the errr amplifier is the ne which gverns the steady state pwer flw. Hwever, since the dynamic range f the errr amplifier is limited, the chice f the pwer gain cnstant K shuld be cnsidered with sme care especially fr high pwer systems. The highest pwer transfer f the APFC f Fig. ccurs when the errr amplifier ltage is at its high saturatin level Ve = Vemax. Cmbining equatins (3), (4) we deduce that the minimum alwable value f the pwer gain cnstant Kmin t btain the full rated average pwer p max at the utput as: v Pmax Vemax -VT &'mm - ( ) (5) T ensure a prper peratin f the APFC ne shud design the system with a pwer gain K greater than the minimum value Kmin given by eq. (5) abve. The required pwer gain cnstant K may be fund as fllws. We assume that the pwer stage is capable f sustaining the input current thrughut the entire half cycle f the line perid and with the current lp clsed. tightly regulates the average input current iin (9). Fr line frequencies far belw the current lp crssver. the current lp gain rll-ff is negligible and the current gain f the inner lp may be apprximated by its DC gain which is determined by the current sensing netwr Rs. In the mst cmmn case Rs is just a series resistance. Thus, utput ltage f the current sensing netwr vs(9) = Rsiin(9) is frced t fllw the current prgramming signal vs(9) = vcp(9) generated at the multipliers utput. The inner lp transresistanse is therefre: iin (9) -=R (6) vcp(9) s Using this simplificatin and sme elementary netwr analysis, the pwer gain cnstant K may be fund as: Pav t K= ve -Rs 4 ~O where HfO is the lw pass filter (LPF) DC gain, the teidll. t is the average t pea rati f the rectified line ltage at the input f the LPF, these quantities appear in the denumeratr f eq. (7) due t the divider actin and are squared due t the squarer actin. The term = ~~ is the verall gain f the divider-multiplier-squarer circuits. Here p dentes the prprtinal gain which usually is refered by the manufacturer as the divider-multipli~-squarer gain. Other gain cnstants must be deteidlined ~rdingly t the resistances at the input and utput teidlinals f the dividermultiplier-squarer circuit. This is required because the multiplier perates with currents while the blc diagram f Fig. is rated in lts, thus fr the ltage fed inputs the assciated gain is unity. Fr the divider-multipliersquarer circuits using current inputs and utputs, the gain cnstants shuld be defined accrdingly t the resistances Rm and Rac cnnected t thse terminals as fllws: (7) ~=R. ac =Rm T ensure prper peratin f the APFC, that is, its ability t supply full pwer t the lad, the pwer gain cnstant K as defined by system parameters in eq. (7) has t be greater r equal t the minimum required value f the pwer gain as dictated by eq.(5): t Rm P max ---> (8) 4 Rac R S-0 H~ (V em ax -V T) The value f the pwer gain cnstant K is significantly ~ ~ -~-" ~," ' R ~ f the divider- lwered by the unfarable resistr rati R ac multiplier-squarer as appears in eq. (8). Hwever, the requirement K > Kmin as stated abve is pssible t fulfill in mst f the practical cases since the dc gain f the LP filter HfO is quite lw and the current sensing resistance Rs is made small fr the sae f lw pwer dissipatin. Bth f thse cnditins mae the ~ I term quite large and a RsHf reasnable value f K may be achieved t satisfy eq. (8). It is wrthwhile t mentin that the term () in the denminatr f eq. (3) represents the rati f the average t pea pwer f a sinusidal wave and the (;) term in the denminatr f eq.(7) is the dc t pea ltage rati f the rectified sinusidal wave. These cnstants are inherent t the sine-wave nly and represent wave shape cnstants. Feeding the PFC with input ltage f ther wavefrm (say dc ltage equivalent t the line ltage rms value r even strngly distrted sine) alters the afrementined relatinships. Vltage regulatin r the PFC The steady state DC errr ltage fr any errr amplifier cnfiguratin may be derived frm the abve given equatins (3), (4) and expressed in terms f the average input pwer as: Ve=KPav+VT (9) A cmmn errr amplifier tplgy is shwn at Fig. 3. The amplifiers utput ltage may be expressed as functin f the reference V ref and the utput V ltages f the APFC: V e = VrefHref -V H (0) here H and Href are the dc gain cnstants f the errr amplifier fr its inverting and nn inverting inputs. Fig. 3. Vltage errr amplifier cnfigllratin and its blc diagram.
3 ~ This relatinship states the dependence f the APFC utput ltage n its pwer level. In particularly we can see that the utput ltage f the APFC is a linear functin f pwer. Here we can recgnize the maximum utput ltage f the PFC fr the n lad cnditin as: ( Href YT ) Ymax= Yref~- ~ () and the utput ltage drp under lad as: ~Y=Ymax -Y=m-Pav (3) Substitute Pav = Y 0 and eq. () int () yields the dependence f the utput ltage n the utput dc current 0 as: V=Vmax (4) I + ~ 0 and the utput ltage regulatin as: Y Reg= y- = max + -- KH I (5) The minimum utput ltage which ccurs at full pwer is: Vmin =Vmax -~Pmax (6) As it was mentined abve, the APFC f Fig. supplies the lad a cnstant average pwer which is prprtinal t the errr amplifier signal, see eq. (3). Since the later is limited by its saturatin level Vemax' it inherently limits the pwer transfer t sme maximum value f P max. An attempt t increase the lad pwer beynd P max can nt be fulfllled by the APFC. Thus, in the case f an verlad by a cnstant pwer lad, such as dwnstream DC-DC cnverters, the APFC's utput ltage will drp and the system will eventually cease, hpefully by a prtectin circuitry. In the case f a resistive r cnstant current lad an verlad cnditin may be tlerable. A well designed system culd sustain the lad indefinitely with the APFC's utput ltage drped t maintain its maximum available pwer at the utput, that is VOvl = "p;:;;;il Pmax resistive lad RL and VOvl = -fr 0 current lad 0. Steady state DC mdel r the 3-p PFC fr a the cnstant We prceed t develp the steady state DC mdel f the APFC ltage lp asuming that the line ltage and the lad are eept cnstant. In mst f the practical cases the VT term H Href in eq.(6) abve is much lwer than Vref~ and may be neglected withut significant lss f accuracy. Thus maximum utput ltage may be fairly apprximated as: Href, Vmax = Vref~ (7) YO nw substituting equatin (7) bac int (4) we get We culd rewrite this as: (8) ( Href ~ t) Y=Yref H (9) + ( ~ )(Href~ t) Examining eq. (9) abve reveals that the ltage lp has the fllwing steady state dc characteristics. The steady state dc clsed lp gain is: Y AcL = -= AOL (0) Yref + ~AOL where the steady state dc pen lp gain may be recgnized as: the steady state dc feedbac lp gain as: ~= (HVO ~ ) () and the steady state dc lp gain as: ~AL = ( H ~ t) (3) Thus, the ltage lp may be mdeled by an equivalent scheme f Fig. 4. Eqs. (), (3) abve shw a clear dependence f the APFC lp gains n the lading. Under light lad cnditins, when the term t in the expressins abve tends t infinity. The resulting infinite lp gain ~AOL cuses the utput ltage t apprach its maximum value f Vmax. Under a heavy lad, the lp gain ~AOL as well as the clsed lp gain Ac L. decreases cusing the utput ltage t drp. Examining equatin (4) we can see that the utput ltage drp may be minimized by maximizing the prduct f the pwer gain cnstant K and the ltage errr amplifier gains "vo' "ref" Cnfiguring the errr amplifier as an integratr, with infmite DC gains, results in zer utput ltage drp under any permissible lad cnditins. Dynamic mdel r the uter lps r the 3-lp APFC We nw turn t develp the dynamic mdel f the 3-lp APFC system f Fig.l. Our basic assumptins are: a) the pwer stage is ideal, b) the current lp is ideal. c) there is n energy strage in the pwer stage. Assumptin (a) is justified by the high efficiency f the ff-line cnverters, which may be as high as 95% fr high ltage applicatins. Assumptin (b)!s deduced frm the fllwing reasning. Since the current lp bandwidth is high, its gain rll-ff is negligible within the extremely narrw frequency range defined by the uter lps bandwidth. Therefre, withut significant lss f accuracy, it is pssible t say that the inner lp is seen by the uter lps as if it is a frequency independent blc with fixed
4 gain. It is further assumed that the cnverter under clsed current lp has sufficient gain t frce the input current t fllw the lw frequency reference signal prduced by the multiplier -di vider -squarer: Ve V in lin = R (4) s V f Were V in' V f, Ve dente the instantaneus input, the feedfrward and the errr amplifier ltages respectively, and R ' as was already mentined abve, is the cmbined gain s f the inner lp and the multiplier-divider-squarer. see Fig. I. Due t the lw value f the cnverter inductr, the average energy strage thrughut the line perid is negligible when cmpared t the prcessed pwer. This fact justifies assumptin (c) abve. Treating the pwer stage as if it has n energy strage, we may use the pwer balance relatinship t btain the charging current Ich supplied by the pwer stage t the hld-up capacitr and the lad: V inlin Ve V in Ich ; = -(5) Y Rs V V f This set f tw nn linear but quit simple equatins characterize the actin f the pwer stage under the current lp cntrl tgether with the current shaping netwr (multiplier-divider-squarer) and may be regarded as the large signal mdel. They als culd be used t simulate the APFC circuits n general purpse circuit simulatrs such as SPICE and prvide a gd insight t the APFC peratin n the pwer line perid scale. Each f the equatins (4) and (5) abve may be expanded int multi-variable Taylr series arund the steady state perating pint. We apprximate the increments f the input current amplitude and utput charging current using nly the first rder terms f the expansin. Linearizatin yields a y parameter mdel fr input and utput circuits: i. = y..v. + y. v + Yif v f (6) I I le e i = Yivi + Yeve +Yfvf + Y (7) This new set f first rder linear equatins describe the dynamics f the small signal variatins, where the cefficients Yxx are the first rder partial derivatives and the lwercase ii' i' vi' ve' vf' V designate the small signal perturbatins f the apprpriate variables. Since the eqs. (4) and (5) are nn linear it is expected that their derivatives wuld depend n the perating pint. Therefre. the steady state perating pint cnditins have t be defined t quantify the Yxx cefficients. A natural chice is t defme the steady state perating pint f the APFC by the average value f the cntrl variables V., In Ve' V f' V. The average values f the cntrl signals f the feed frward and feed bac paths may be btained simply by neglecting their ripple cmpnents as fllws: the ave~age utput ltage as its.nminal ;DC value V = VOC. the steady state ltage at th~ utput f the Ye =- R -- -V rills ( 8 ) S V v f t find that the nns value f the line ltage V rms shud be used t calculate the Yxx parameters value. T be cnsistent with this reasning we define the ltage transfer rati M f the APFC as its dc utput ltage VDC t the rms line ltage V rms rati: Vc M= V \"'7 rms this will be useful t simplifiy the average mdel frmulae belw. The resulting expressins fr y parameters are summarized belw: - (~ ) -l-~ M y..- d -- v. ri -=RL ss Vrms (d ii ) K Yie= ~ ss= ~ (d ii ) 7t yit= ~ ss=-hfu~ y.- ~--.!E.!!) d -l- p a v - 0 v. M ss -=RL Vrms Ye= ~ ~ ich ) = VOC K e ss Y= ~ ~ ich ) = -~=- 0 SS ~~ M Pay! (30) ltage errr amplifier is the average signal which may be - fund frm equatin (3) as ve = K P av and the steady state ltage at the utput f the feed-frward filter as its average ~ { ltage vf = -Hf V m = -Hf V rms. The difficulty t t arises when ne cnsiders the chice f the steady state value f the line ltage t be substituted fr evaluatin f the derivatives y(xx). The candidates are the average
5 J The mdel may be applied in design and analysis f the feedbac and feed-frward lps f the 3-lp APFC system f Fig.. We ntice that resistance present in bth input and utput circuits. The small signal input resistance r. equals the steady state resistance emulated by the APFC twards the line. On the ther hand the small signal utput resistance r equals the equivalent lad resistance. Anther feature the mdel disclses prperly well, is the actin f the feed frward path. Indeed, it may be seen that the feed frward path acts against the line variatins in bth the input and the utput circuits. Hwever, the mst prminent feature f the feed frward is the stabilizatin f the ltage feedbac gain Ye which is made invariant f line amplitude variatins. In the usual case, when the average utput ltage is nly slightly depends n the lad, we may cnsider y e als t a gd extent, as lad independent. Simulatin results T chec the validity f the prpsed thery, the APFC circuit f Fig. was simulated by PSPICE prgram. The simulatin diagram is shwn at Fig. 6 and uses the large signal mdel f the pwer stage, eqs. (4), (5). The circuit parameters were set accrding t the manufacturer recmmendatin, as may be fund in references [3] and [4]. The multiplier terminal resistances and its threshld ltage were cded as parameters f the simulatin prgram and set t the fllwing values Rac = 90, Rm=4, VT=lV. The reference ltage was set t VreF 7.5V and the hld-up capacitr t C = 450~F. The errr amplifier saturatin levels were Vemax= 5.8V and Vemin= 0.V. The errr amplifier dc gains were fund as HreF 9.7, H= 0.35 and the LPF dc gain as Hf= Using eq. (7) the theretical pwer gain cnstant was fund as K= 3, and agreed well with that measured frm simulated wavefrms: K= 5.8. Fig. 7(a) shws the simulated wavefrms f the utput ltage V f the APFC laded with a cnstant pwer lad. As it is predicted by the thery, the utput ltage f the APFC, with fmite ltage errr amplifier dc gain, drps steadily with the increase in the pwer level. T create an errr ltage amplifier with an infmite dc gain the lcal feedbac f the amplifier f Fig. 3 was recnfigured int an series branch. With this imprvement the nminal utput ltage became V max=398.6v.as may be seen at Fig. 7(b) the APFC was able t eep its nminal ltage fr all permissible lading. The theretical maximum pwer level f the APFC was fund by eq. (7) as 7W, the inability f the APFC t sustain 300W lad is demnstrated at Fig. 8. The theretical value f the utput ltage as functin f pwer was calculated using eq. (). Fig. 9 presents a cmparisn between the theretical and simulated results. Gd agreement f the results is fund. Fig. 0 shws the dependence f the APFC's utput ltaje V n the multiplier's threshld level VT. Theretical value f the term ~ in eq.(6) was fund as.839v and stands in gd agreement with that measured frm simulatin wavefrms:.8v. The APFC's y -parameters set was calculated as suggested by equatin (30). Accrding t the data abve, we get: Yii= , Yir 0.936, Yie= 36.3, Yi= , Yf = f Fig. 5 the APFC with a resistive lad, RL = 580.Q, was simulated with its line ltage perturbed, by amplitude mdulatin. Cmparisn f the simulated wavefrms f bth circuits may be seen at Fig.. The input current (upper trace) and the utput ltage (lwer trace) f the APFC and its mdel are shwn as a respnse t the perturbed line ltage. A gd agreement f the "real" and equivalent circuits respnses may be fund. Cnclusins Simple static and dynamic mdels f the 3-lp Average Current Mde Active Pwer Factr Crrectin (APFC) system were suggested and analyzed. Analytical expressins fr the APFC's pwer gain cnstant and utput ltage regulatin as functin f circuit parameters where btained. Based n the y- parameter apprach. the small signal equivalent circuit f the uter lps f the APFC was presented. The thery was supprted by cmputer simulatin. The presented mdels described well the static and dynamic behavir f the system. The prpsed thery may be useful in the analysis and design f the uter lps f the 3-lp APFC systems. References [] Williams. I. B.: Design f feedbac lp in Unity pwer factr AC t DC cnverter. IEEE PESC 989 Rec., 989, pp [] Dixn. L. H.. "High pwer factr preregulatrs fr ffline pwer supplies", Unitrde Seminar Prceedings 990 [3] L. H. Dixn, "High pwer factr preregulatr design ptimizatin", Unitrde Seminar Prceedings 99 [4] P. C. Tdd, "UC3854 cntrlled pwer factr crrectin circuit design". Unitrde Applicatins Handb Fig. 6. PSPICE simulatin diagram f the "real" 3-lp APFC f Fig. I. 0.36, y = 4, y 0 =.74. T verify the prpsed mdel e
Revision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax
.7.4: Direct frequency dmain circuit analysis Revisin: August 9, 00 5 E Main Suite D Pullman, WA 9963 (509) 334 6306 ice and Fax Overview n chapter.7., we determined the steadystate respnse f electrical
More informationA Comparison of AC/DC Piezoelectric Transformer Converters with Current Doubler and Voltage Doubler Rectifiers
A Cmparisn f AC/DC Piezelectric Transfrmer Cnverters with Current Dubler and ltage Dubler Rectifiers Gregry vensky, Svetlana Brnstein and Sam Ben-Yaakv* Pwer Electrnics abratry Department f Electrical
More informationDesign and Simulation of Dc-Dc Voltage Converters Using Matlab/Simulink
American Jurnal f Engineering Research (AJER) 016 American Jurnal f Engineering Research (AJER) e-issn: 30-0847 p-issn : 30-0936 Vlume-5, Issue-, pp-9-36 www.ajer.rg Research Paper Open Access Design and
More informationOP AMP CHARACTERISTICS
O AM CHAACTESTCS Static p amp limitatins EFEENCE: Chapter 5 textbk (ESS) EOS CAUSED BY THE NUT BAS CUENT AND THE NUT OFFSET CUENT Op Amp t functin shuld have fr the input terminals a DC path thrugh which
More informationA Novel Isolated Buck-Boost Converter
vel slated uck-st Cnverter S-Sek Kim *,WOO-J JG,JOOG-HO SOG, Ok-K Kang, and Hee-Jn Kim ept. f Electrical Eng., Seul atinal University f Technlgy, Krea Schl f Electrical and Cmputer Eng., Hanyang University,
More informationRelationships Between Frequency, Capacitance, Inductance and Reactance.
P Physics Relatinships between f,, and. Relatinships Between Frequency, apacitance, nductance and Reactance. Purpse: T experimentally verify the relatinships between f, and. The data cllected will lead
More informationDead-beat controller design
J. Hetthéssy, A. Barta, R. Bars: Dead beat cntrller design Nvember, 4 Dead-beat cntrller design In sampled data cntrl systems the cntrller is realised by an intelligent device, typically by a PLC (Prgrammable
More informationDetermining the Accuracy of Modal Parameter Estimation Methods
Determining the Accuracy f Mdal Parameter Estimatin Methds by Michael Lee Ph.D., P.E. & Mar Richardsn Ph.D. Structural Measurement Systems Milpitas, CA Abstract The mst cmmn type f mdal testing system
More informationCurrent/voltage-mode third order quadrature oscillator employing two multiple outputs CCIIs and grounded capacitors
Indian Jurnal f Pure & Applied Physics Vl. 49 July 20 pp. 494-498 Current/vltage-mde third rder quadrature scillatr emplying tw multiple utputs CCIIs and grunded capacitrs Jiun-Wei Hrng Department f Electrnic
More informationOTHER USES OF THE ICRH COUPL ING CO IL. November 1975
OTHER USES OF THE ICRH COUPL ING CO IL J. C. Sprtt Nvember 1975 -I,," PLP 663 Plasma Studies University f Wiscnsin These PLP Reprts are infrmal and preliminary and as such may cntain errrs nt yet eliminated.
More informationECEN 4872/5827 Lecture Notes
ECEN 4872/5827 Lecture Ntes Lecture #5 Objectives fr lecture #5: 1. Analysis f precisin current reference 2. Appraches fr evaluating tlerances 3. Temperature Cefficients evaluatin technique 4. Fundamentals
More information1. Transformer A transformer is used to obtain the approximate output voltage of the power supply. The output of the transformer is still AC.
PHYSIS 536 Experiment 4: D Pwer Supply I. Intrductin The prcess f changing A t D is investigated in this experiment. An integrated circuit regulatr makes it easy t cnstruct a high-perfrmance vltage surce
More informationECE 2100 Circuit Analysis
ECE 00 Circuit Analysis Lessn 6 Chapter 4 Sec 4., 4.5, 4.7 Series LC Circuit C Lw Pass Filter Daniel M. Litynski, Ph.D. http://hmepages.wmich.edu/~dlitynsk/ ECE 00 Circuit Analysis Lessn 5 Chapter 9 &
More informationSections 15.1 to 15.12, 16.1 and 16.2 of the textbook (Robbins-Miller) cover the materials required for this topic.
Tpic : AC Fundamentals, Sinusidal Wavefrm, and Phasrs Sectins 5. t 5., 6. and 6. f the textbk (Rbbins-Miller) cver the materials required fr this tpic.. Wavefrms in electrical systems are current r vltage
More informationSynchronous Motor V-Curves
Synchrnus Mtr V-Curves 1 Synchrnus Mtr V-Curves Intrductin Synchrnus mtrs are used in applicatins such as textile mills where cnstant speed peratin is critical. Mst small synchrnus mtrs cntain squirrel
More informationOscillator. Introduction of Oscillator Linear Oscillator. Stability. Wien Bridge Oscillator RC Phase-Shift Oscillator LC Oscillator
Oscillatr Intrductin f Oscillatr Linear Oscillatr Wien Bridge Oscillatr Phase-Shift Oscillatr L Oscillatr Stability Oscillatrs Oscillatin: an effect that repeatedly and regularly fluctuates abut the mean
More informationModule 4: General Formulation of Electric Circuit Theory
Mdule 4: General Frmulatin f Electric Circuit Thery 4. General Frmulatin f Electric Circuit Thery All electrmagnetic phenmena are described at a fundamental level by Maxwell's equatins and the assciated
More informationSection I5: Feedback in Operational Amplifiers
Sectin I5: eedback in Operatinal mplifiers s discussed earlier, practical p-amps hae a high gain under dc (zer frequency) cnditins and the gain decreases as frequency increases. This frequency dependence
More informationGENERAL FORMULAS FOR FLAT-TOPPED WAVEFORMS. J.e. Sprott. Plasma Studies. University of Wisconsin
GENERAL FORMULAS FOR FLAT-TOPPED WAVEFORMS J.e. Sprtt PLP 924 September 1984 Plasma Studies University f Wiscnsin These PLP Reprts are infrmal and preliminary and as such may cntain errrs nt yet eliminated.
More informationZVS Boost Converter. (a) (b) Fig 6.29 (a) Quasi-resonant boost converter with M-type switch. (b) Equivalent circuit.
EEL6246 Pwer Electrnics II Chapter 6 Lecture 6 Dr. Sam Abdel-Rahman ZVS Bst Cnverter The quasi-resnant bst cnverter by using the M-type switch as shwn in Fig. 6.29(a) with its simplified circuit shwn in
More informationLecture 02 CSE 40547/60547 Computing at the Nanoscale
PN Junctin Ntes: Lecture 02 CSE 40547/60547 Cmputing at the Nanscale Letʼs start with a (very) shrt review f semi-cnducting materials: - N-type material: Obtained by adding impurity with 5 valence elements
More informationLab 11 LRC Circuits, Damped Forced Harmonic Motion
Physics 6 ab ab 11 ircuits, Damped Frced Harmnic Mtin What Yu Need T Knw: The Physics OK this is basically a recap f what yu ve dne s far with circuits and circuits. Nw we get t put everything tgether
More informationBicycle Generator Dump Load Control Circuit: An Op Amp Comparator with Hysteresis
Bicycle Generatr Dump Lad Cntrl Circuit: An Op Amp Cmparatr with Hysteresis Sustainable Technlgy Educatin Prject University f Waterl http://www.step.uwaterl.ca December 1, 2009 1 Summary This dcument describes
More informationSeries and Parallel Resonances
Series and Parallel esnances Series esnance Cnsider the series circuit shwn in the frequency dmain. The input impedance is Z Vs jl jl I jc C H s esnance ccurs when the imaginary part f the transfer functin
More informationENSC Discrete Time Systems. Project Outline. Semester
ENSC 49 - iscrete Time Systems Prject Outline Semester 006-1. Objectives The gal f the prject is t design a channel fading simulatr. Upn successful cmpletin f the prject, yu will reinfrce yur understanding
More informationT(s) 1+ T(s) 2. Phase Margin Test for T(s) a. Unconditionally Stable φ m = 90 o for 1 pole T(s) b. Conditionally Stable Case 1.
Lecture 49 Danger f Instability/Oscillatin When Emplying Feedback In PWM Cnverters A. Guessing Clsed Lp Stability Frm Open Lp Frequency Respnse Data. T(s) versus T(s) + T(s) 2. Phase Margin Test fr T(s)
More informationMicro and Smart Systems
Micr and Smart Systems Lecture 33 OpAmps Circuits and signal cnditining fr micrsystems devices Prf K.N.Bhat, ECE Department, IISc Bangalre email: knbhat@gmail.cm Tpics fr Discussin Amplifiers and Op Amp
More informationSupplementary Course Notes Adding and Subtracting AC Voltages and Currents
Supplementary Curse Ntes Adding and Subtracting AC Vltages and Currents As mentined previusly, when cmbining DC vltages r currents, we nly need t knw the plarity (vltage) and directin (current). In the
More informationLead/Lag Compensator Frequency Domain Properties and Design Methods
Lectures 6 and 7 Lead/Lag Cmpensatr Frequency Dmain Prperties and Design Methds Definitin Cnsider the cmpensatr (ie cntrller Fr, it is called a lag cmpensatr s K Fr s, it is called a lead cmpensatr Ntatin
More informationReview Problems 3. Four FIR Filter Types
Review Prblems 3 Fur FIR Filter Types Fur types f FIR linear phase digital filters have cefficients h(n fr 0 n M. They are defined as fllws: Type I: h(n = h(m-n and M even. Type II: h(n = h(m-n and M dd.
More informationPhysics 2B Chapter 23 Notes - Faraday s Law & Inductors Spring 2018
Michael Faraday lived in the Lndn area frm 1791 t 1867. He was 29 years ld when Hand Oersted, in 1820, accidentally discvered that electric current creates magnetic field. Thrugh empirical bservatin and
More informationChE 471: LECTURE 4 Fall 2003
ChE 47: LECTURE 4 Fall 003 IDEL RECTORS One f the key gals f chemical reactin engineering is t quantify the relatinship between prductin rate, reactr size, reactin kinetics and selected perating cnditins.
More informationProtection of ungrounded systems using an advanced relay element
ENG 460 Prtectin f ungrunded systems using an advanced relay element A reprt submitted t the schl f Engineering and Energy, Murdch University in partial fulfilment f the requirements fr the degree f Bachelr
More informationECE 2100 Circuit Analysis
ECE 2100 Circuit Analysis Lessn 25 Chapter 9 & App B: Passive circuit elements in the phasr representatin Daniel M. Litynski, Ph.D. http://hmepages.wmich.edu/~dlitynsk/ ECE 2100 Circuit Analysis Lessn
More informationPerformance Bounds for Detect and Avoid Signal Sensing
Perfrmance unds fr Detect and Avid Signal Sensing Sam Reisenfeld Real-ime Infrmatin etwrks, University f echnlgy, Sydney, radway, SW 007, Australia samr@uts.edu.au Abstract Detect and Avid (DAA) is a Cgnitive
More informationKinetic Model Completeness
5.68J/10.652J Spring 2003 Lecture Ntes Tuesday April 15, 2003 Kinetic Mdel Cmpleteness We say a chemical kinetic mdel is cmplete fr a particular reactin cnditin when it cntains all the species and reactins
More informationSupplementary Course Notes Adding and Subtracting AC Voltages and Currents
Supplementary Curse Ntes Adding and Subtracting AC Vltages and Currents As mentined previusly, when cmbining DC vltages r currents, we nly need t knw the plarity (vltage) and directin (current). In the
More informationOF SIMPLY SUPPORTED PLYWOOD PLATES UNDER COMBINED EDGEWISE BENDING AND COMPRESSION
U. S. FOREST SERVICE RESEARCH PAPER FPL 50 DECEMBER U. S. DEPARTMENT OF AGRICULTURE FOREST SERVICE FOREST PRODUCTS LABORATORY OF SIMPLY SUPPORTED PLYWOOD PLATES UNDER COMBINED EDGEWISE BENDING AND COMPRESSION
More informationComputational modeling techniques
Cmputatinal mdeling techniques Lecture 4: Mdel checing fr ODE mdels In Petre Department f IT, Åb Aademi http://www.users.ab.fi/ipetre/cmpmd/ Cntent Stichimetric matrix Calculating the mass cnservatin relatins
More informationApplying Kirchoff s law on the primary circuit. V = - e1 V+ e1 = 0 V.D. e.m.f. From the secondary circuit e2 = v2. K e. Equivalent circuit :
TRANSFORMERS Definitin : Transfrmers can be defined as a static electric machine which cnverts electric energy frm ne ptential t anther at the same frequency. It can als be defined as cnsists f tw electric
More informationSFDMB3638F. Specifications and Applications Information. orce LED Driver. Mass: 7 grams typ. 10/15/08 Preliminary. Package Configuration
Specificatins and Applicatins Infrmatin 1/1/8 Prelimary Smart Fr rce LED Driver The ERG Smart Frce Series f LED Drivers are specifically designed fr applicatins which require high efficiency, small ftprt
More informationA Self-Sensing Homopolar Magnetic Bearing: Analysis and Experimental Results
A Self-Sensing Hmplar Magnetic Bearing: Analysis and Experimental Results Perry Tsa Seth R. Sanders Gabriel Risk Department f Electrical Engineering and Cmputer Science University f Califrnia, Berkeley
More informationCHAPTER 3 INEQUALITIES. Copyright -The Institute of Chartered Accountants of India
CHAPTER 3 INEQUALITIES Cpyright -The Institute f Chartered Accuntants f India INEQUALITIES LEARNING OBJECTIVES One f the widely used decisin making prblems, nwadays, is t decide n the ptimal mix f scarce
More informationCopyright Paul Tobin 63
DT, Kevin t. lectric Circuit Thery DT87/ Tw-Prt netwrk parameters ummary We have seen previusly that a tw-prt netwrk has a pair f input terminals and a pair f utput terminals figure. These circuits were
More informationCS 477/677 Analysis of Algorithms Fall 2007 Dr. George Bebis Course Project Due Date: 11/29/2007
CS 477/677 Analysis f Algrithms Fall 2007 Dr. Gerge Bebis Curse Prject Due Date: 11/29/2007 Part1: Cmparisn f Srting Algrithms (70% f the prject grade) The bjective f the first part f the assignment is
More information1.1 The main transmission network of Eskom The classical two generator model 11
LIST OF FIGURS Figure Page 1.1 The main transmissin netwrk f skm 4 2.1 The classical tw generatr mdel 11 2.2 Obtaining the lcatin f the electrical centre. The line cnnecting A with B represents the netwrk
More informationTOPPER SAMPLE PAPER 2 Class XII- Physics
TOPPER SAMPLE PAPER 2 Class XII- Physics Time: Three Hurs Maximum Marks: 70 General Instructins (a) All questins are cmpulsry. (b) There are 30 questins in ttal. Questins 1 t 8 carry ne mark each, questins
More informationBootstrap Method > # Purpose: understand how bootstrap method works > obs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(obs) >
Btstrap Methd > # Purpse: understand hw btstrap methd wrks > bs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(bs) > mean(bs) [1] 21.64625 > # estimate f lambda > lambda = 1/mean(bs);
More informationEDA Engineering Design & Analysis Ltd
EDA Engineering Design & Analysis Ltd THE FINITE ELEMENT METHOD A shrt tutrial giving an verview f the histry, thery and applicatin f the finite element methd. Intrductin Value f FEM Applicatins Elements
More information(2) Even if such a value of k was possible, the neutrons multiply
CHANGE OF REACTOR Nuclear Thery - Curse 227 POWER WTH REACTVTY CHANGE n this lessn, we will cnsider hw neutrn density, neutrn flux and reactr pwer change when the multiplicatin factr, k, r the reactivity,
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 informationThermodynamics Partial Outline of Topics
Thermdynamics Partial Outline f Tpics I. The secnd law f thermdynamics addresses the issue f spntaneity and invlves a functin called entrpy (S): If a prcess is spntaneus, then Suniverse > 0 (2 nd Law!)
More informationStudy Group Report: Plate-fin Heat Exchangers: AEA Technology
Study Grup Reprt: Plate-fin Heat Exchangers: AEA Technlgy The prblem under study cncerned the apparent discrepancy between a series f experiments using a plate fin heat exchanger and the classical thery
More informationTransduction Based on Changes in the Energy Stored in an Electrical Field
Lecture 6-3 Transductin Based n Changes in the Energy Stred in an Electrical ield Department f Mechanical Engineering Example:Capacitive Pressure Sensr Pressure sensitive capacitive device With separatin
More informationChapter 30. Inductance
Chapter 30 nductance 30. Self-nductance Cnsider a lp f wire at rest. f we establish a current arund the lp, it will prduce a magnetic field. Sme f the magnetic field lines pass thrugh the lp. et! be the
More informationLecture 20a. Circuit Topologies and Techniques: Opamps
Lecture a Circuit Tplgies and Techniques: Opamps In this lecture yu will learn: Sme circuit tplgies and techniques Intrductin t peratinal amplifiers Differential mplifier IBIS1 I BIS M VI1 vi1 Vi vi I
More informationGeneral Amplifiers. Analog Electronics Circuits Nagamani A N. Lecturer, PESIT, Bangalore 85. Cascade connection - FET & BJT
Analg lectrnics Circuits Nagamani A N Lecturer, PST, Bangalre 85 mail nagamani@pes.edu General Amplifiers Cascade cnnectin - FT & BJT Numerical Cascde cnnectin arlingtn cnnectin Packaged arlingtn cnnectin
More informationFall 2013 Physics 172 Recitation 3 Momentum and Springs
Fall 03 Physics 7 Recitatin 3 Mmentum and Springs Purpse: The purpse f this recitatin is t give yu experience wrking with mmentum and the mmentum update frmula. Readings: Chapter.3-.5 Learning Objectives:.3.
More informationBASIC DIRECT-CURRENT MEASUREMENTS
Brwn University Physics 0040 Intrductin BASIC DIRECT-CURRENT MEASUREMENTS The measurements described here illustrate the peratin f resistrs and capacitrs in electric circuits, and the use f sme standard
More informationFlipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System
Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed
More informationLinearization of the Output of a Wheatstone Bridge for Single Active Sensor. Madhu Mohan N., Geetha T., Sankaran P. and Jagadeesh Kumar V.
Linearizatin f the Output f a Wheatstne Bridge fr Single Active Sensr Madhu Mhan N., Geetha T., Sankaran P. and Jagadeesh Kumar V. Dept. f Electrical Engineering, Indian Institute f Technlgy Madras, Chennai
More informationLevel Control in Horizontal Tank by Fuzzy-PID Cascade Controller
Wrld Academy f Science, Engineering and Technlgy 5 007 Level Cntrl in Hrizntal Tank by Fuzzy-PID Cascade Cntrller Satean Tunyasrirut, and Santi Wangnipparnt Abstract The paper describes the Fuzzy PID cascade
More informationA Novel Electro-thermal Simulation Approach to Power IGBT Modules for Automotive Traction Applications
Special Issue Recent R&D Activities f Pwer Devices fr Hybrid Electric Vehicles 27 Research Reprt A Nvel Electr-thermal Simulatin Apprach t Pwer IGBT Mdules fr Autmtive Tractin Applicatins Takashi Kjima,
More informationGeneral Chemistry II, Unit II: Study Guide (part 1)
General Chemistry II, Unit II: Study Guide (part 1) CDS Chapter 21: Reactin Equilibrium in the Gas Phase General Chemistry II Unit II Part 1 1 Intrductin Sme chemical reactins have a significant amunt
More informationEXPERIMENTAL STUDY ON DISCHARGE COEFFICIENT OF OUTFLOW OPENING FOR PREDICTING CROSS-VENTILATION FLOW RATE
EXPERIMENTAL STUD ON DISCHARGE COEFFICIENT OF OUTFLOW OPENING FOR PREDICTING CROSS-VENTILATION FLOW RATE Tmnbu Gt, Masaaki Ohba, Takashi Kurabuchi 2, Tmyuki End 3, shihik Akamine 4, and Tshihir Nnaka 2
More informationMODULE TITLE : OPERATIONAL AMPLIFIERS TOPIC TITLE : FILTERS LESSON 1 : FILTERS
MODULE TITLE : OPEATIONAL AMPLIFIES TOPIC TITLE : FILTES LESSON : FILTES OA - 4 - Teesside University 0 INTODUCTION An electrical filter is a device which is designed t pass sme frequencies and reject
More information^YawataR&D Laboratory, Nippon Steel Corporation, Tobata, Kitakyushu, Japan
Detectin f fatigue crack initiatin frm a ntch under a randm lad C. Makabe," S. Nishida^C. Urashima,' H. Kaneshir* "Department f Mechanical Systems Engineering, University f the Ryukyus, Nishihara, kinawa,
More informationKinematic transformation of mechanical behavior Neville Hogan
inematic transfrmatin f mechanical behavir Neville Hgan Generalized crdinates are fundamental If we assume that a linkage may accurately be described as a cllectin f linked rigid bdies, their generalized
More informationNUROP CONGRESS PAPER CHINESE PINYIN TO CHINESE CHARACTER CONVERSION
NUROP Chinese Pinyin T Chinese Character Cnversin NUROP CONGRESS PAPER CHINESE PINYIN TO CHINESE CHARACTER CONVERSION CHIA LI SHI 1 AND LUA KIM TENG 2 Schl f Cmputing, Natinal University f Singapre 3 Science
More informationElectric Current and Resistance
Electric Current and Resistance Electric Current Electric current is the rate f flw f charge thrugh sme regin f space The SI unit f current is the ampere (A) 1 A = 1 C / s The symbl fr electric current
More informationLeast Squares Optimal Filtering with Multirate Observations
Prc. 36th Asilmar Cnf. n Signals, Systems, and Cmputers, Pacific Grve, CA, Nvember 2002 Least Squares Optimal Filtering with Multirate Observatins Charles W. herrien and Anthny H. Hawes Department f Electrical
More informationSimulation of Push-pull Multi-output Quasi-resonant Converter
IOSR Jurnal f Electrical and Electrnics Engineering (IOSR-JEEE) e-issn: 78-1676,p-ISSN: 3-3331, Vlue 9, Issue 1 Ver. V (Feb. 14), PP 19-4 Siulatin f Push-pull Multi-utput Quasi-resnant Cnverter T.Anitha
More informationSimulation of Line Outage Distribution Factors (L.O.D.F) Calculation for N-Buses System
Simulatin f Line Outage Distributin Factrs (L.O.D.F) Calculatin fr N-Buses System Rashid H. AL-Rubayi Department f Electrical Engineering, University f Technlgy Afaneen A. Abd Department f Electrical Engineering,
More information2.161 Signal Processing: Continuous and Discrete Fall 2008
MIT OpenCurseWare http://cw.mit.edu 2.161 Signal Prcessing: Cntinuus and Discrete Fall 2008 Fr infrmatin abut citing these materials r ur Terms f Use, visit: http://cw.mit.edu/terms. Massachusetts Institute
More informationRelationship Between Amplifier Settling Time and Pole-Zero Placements for Second-Order Systems *
Relatinship Between Amplifier Settling Time and Ple-Zer Placements fr Secnd-Order Systems * Mark E. Schlarmann and Randall L. Geiger Iwa State University Electrical and Cmputer Engineering Department Ames,
More information11. DUAL NATURE OF RADIATION AND MATTER
11. DUAL NATURE OF RADIATION AND MATTER Very shrt answer and shrt answer questins 1. Define wrk functin f a metal? The minimum energy required fr an electrn t escape frm the metal surface is called the
More informationCompressibility Effects
Definitin f Cmpressibility All real substances are cmpressible t sme greater r lesser extent; that is, when yu squeeze r press n them, their density will change The amunt by which a substance can be cmpressed
More information1996 Engineering Systems Design and Analysis Conference, Montpellier, France, July 1-4, 1996, Vol. 7, pp
THE POWER AND LIMIT OF NEURAL NETWORKS T. Y. Lin Department f Mathematics and Cmputer Science San Jse State University San Jse, Califrnia 959-003 tylin@cs.ssu.edu and Bereley Initiative in Sft Cmputing*
More informationDYNAMIC MODELLING OF N-CARDAN TRANSMISSIONS WITH SHAFTS IN SPATIAL CONFIGURATION. Part II. THE ALGORITHM OF DYNAMIC MODELLING
Fascicle f Management and Technlgical Engineering, Vlume VI (XVI), 7 DYNAMIC MODELLING OF N-CARDAN TRANSMISSIONS WITH SHAFTS IN SPATIAL CONFIGURATION. Part II. THE ALGORITHM OF DYNAMIC MODELLING Cdrua
More informationOptimization Programming Problems For Control And Management Of Bacterial Disease With Two Stage Growth/Spread Among Plants
Internatinal Jurnal f Engineering Science Inventin ISSN (Online): 9 67, ISSN (Print): 9 676 www.ijesi.rg Vlume 5 Issue 8 ugust 06 PP.0-07 Optimizatin Prgramming Prblems Fr Cntrl nd Management Of Bacterial
More informationFlipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System
Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed
More informationInterference is when two (or more) sets of waves meet and combine to produce a new pattern.
Interference Interference is when tw (r mre) sets f waves meet and cmbine t prduce a new pattern. This pattern can vary depending n the riginal wave directin, wavelength, amplitude, etc. The tw mst extreme
More informationA Few Basic Facts About Isothermal Mass Transfer in a Binary Mixture
Few asic Facts but Isthermal Mass Transfer in a inary Miture David Keffer Department f Chemical Engineering University f Tennessee first begun: pril 22, 2004 last updated: January 13, 2006 dkeffer@utk.edu
More informationPattern Recognition 2014 Support Vector Machines
Pattern Recgnitin 2014 Supprt Vectr Machines Ad Feelders Universiteit Utrecht Ad Feelders ( Universiteit Utrecht ) Pattern Recgnitin 1 / 55 Overview 1 Separable Case 2 Kernel Functins 3 Allwing Errrs (Sft
More informationROUNDING ERRORS IN BEAM-TRACKING CALCULATIONS
Particle Acceleratrs, 1986, Vl. 19, pp. 99-105 0031-2460/86/1904-0099/$15.00/0 1986 Grdn and Breach, Science Publishers, S.A. Printed in the United States f America ROUNDING ERRORS IN BEAM-TRACKING CALCULATIONS
More informationDerailment Safety Evaluation by Analytic Equations
PAPER Derailment Safety Evaluatin by Analytic Equatins Hideyuki TAKAI General Manager, Track Technlgy Div. Hirnari MURAMATSU Assistant Senir Researcher, Track Gemetry & Maintenance, Track Technlgy Div.
More informationCHAPTER 5. Solutions for Exercises
HAPTE 5 Slutins fr Exercises E5. (a We are given v ( t 50 cs(00π t 30. The angular frequency is the cefficient f t s we have ω 00π radian/s. Then f ω / π 00 Hz T / f 0 ms m / 50 / 06. Furthermre, v(t attains
More informationThermodynamics and Equilibrium
Thermdynamics and Equilibrium Thermdynamics Thermdynamics is the study f the relatinship between heat and ther frms f energy in a chemical r physical prcess. We intrduced the thermdynamic prperty f enthalpy,
More informationSPH3U1 Lesson 06 Kinematics
PROJECTILE MOTION LEARNING GOALS Students will: Describe the mtin f an bject thrwn at arbitrary angles thrugh the air. Describe the hrizntal and vertical mtins f a prjectile. Slve prjectile mtin prblems.
More informationTHERMAL TEST LEVELS & DURATIONS
PREFERRED RELIABILITY PAGE 1 OF 7 PRACTICES PRACTICE NO. PT-TE-144 Practice: 1 Perfrm thermal dwell test n prtflight hardware ver the temperature range f +75 C/-2 C (applied at the thermal cntrl/munting
More informationModeling the Nonlinear Rheological Behavior of Materials with a Hyper-Exponential Type Function
www.ccsenet.rg/mer Mechanical Engineering Research Vl. 1, N. 1; December 011 Mdeling the Nnlinear Rhelgical Behavir f Materials with a Hyper-Expnential Type Functin Marc Delphin Mnsia Département de Physique,
More informationTechnical Bulletin. Generation Interconnection Procedures. Revisions to Cluster 4, Phase 1 Study Methodology
Technical Bulletin Generatin Intercnnectin Prcedures Revisins t Cluster 4, Phase 1 Study Methdlgy Release Date: Octber 20, 2011 (Finalizatin f the Draft Technical Bulletin released n September 19, 2011)
More informationExam #1. A. Answer any 1 of the following 2 questions. CEE 371 October 8, Please grade the following questions: 1 or 2
CEE 371 Octber 8, 2009 Exam #1 Clsed Bk, ne sheet f ntes allwed Please answer ne questin frm the first tw, ne frm the secnd tw and ne frm the last three. The ttal ptential number f pints is 100. Shw all
More informationExam #1. A. Answer any 1 of the following 2 questions. CEE 371 March 10, Please grade the following questions: 1 or 2
CEE 371 March 10, 2009 Exam #1 Clsed Bk, ne sheet f ntes allwed Please answer ne questin frm the first tw, ne frm the secnd tw and ne frm the last three. The ttal ptential number f pints is 100. Shw all
More informationTHERMAL-VACUUM VERSUS THERMAL- ATMOSPHERIC TESTS OF ELECTRONIC ASSEMBLIES
PREFERRED RELIABILITY PAGE 1 OF 5 PRACTICES PRACTICE NO. PT-TE-1409 THERMAL-VACUUM VERSUS THERMAL- ATMOSPHERIC Practice: Perfrm all thermal envirnmental tests n electrnic spaceflight hardware in a flight-like
More informationWe can see from the graph above that the intersection is, i.e., [ ).
MTH 111 Cllege Algebra Lecture Ntes July 2, 2014 Functin Arithmetic: With nt t much difficulty, we ntice that inputs f functins are numbers, and utputs f functins are numbers. S whatever we can d with
More informationMATHEMATICS SYLLABUS SECONDARY 5th YEAR
Eurpean Schls Office f the Secretary-General Pedaggical Develpment Unit Ref. : 011-01-D-8-en- Orig. : EN MATHEMATICS SYLLABUS SECONDARY 5th YEAR 6 perid/week curse APPROVED BY THE JOINT TEACHING COMMITTEE
More informationABSORPTION OF GAMMA RAYS
6 Sep 11 Gamma.1 ABSORPTIO OF GAMMA RAYS Gamma rays is the name given t high energy electrmagnetic radiatin riginating frm nuclear energy level transitins. (Typical wavelength, frequency, and energy ranges
More informationFebruary 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA
February 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA Mental Experiment regarding 1D randm walk Cnsider a cntainer f gas in thermal
More informationGeneral Chemistry II, Unit I: Study Guide (part I)
1 General Chemistry II, Unit I: Study Guide (part I) CDS Chapter 14: Physical Prperties f Gases Observatin 1: Pressure- Vlume Measurements n Gases The spring f air is measured as pressure, defined as the
More information