Simulation of Push-pull Multi-output Quasi-resonant Converter

Size: px
Start display at page:

Download "Simulation of Push-pull Multi-output Quasi-resonant Converter"

Transcription

1 IOSR Jurnal f Electrical and Electrnics Engineering (IOSR-JEEE) e-issn: ,p-ISSN: , Vlue 9, Issue 1 Ver. V (Feb. 14), PP 19-4 Siulatin f Push-pull Multi-utput Quasi-resnant Cnverter T.Anitha 1, S.Arulselvi 1 (Assistant Prfessr, Departent f Electrnics and Instruentatin Engg., Annaalai University,India) (Prfessr, Departent, f Electrnics and Instruentatin Engg., Annaalai University,India) Abstract : Pwer supply vltages in digital systes have been reduced cnsiderably in recent years and ften digital cpnents requiring different vltages are present in the sae bard. This has increased the deand fr ultiple utput pwer distributin systes with tight lad regulatin. In this paper, a detailed analysis and design f a ulti-utput push-pull zer vltage switching (ZVS) quasi resnant cnverter (QRC) has been carried ut. Als siulatin f ulti-utput push-pull zer vltage switching (ZVS) quasi resnant cnverter (QRC) has been carried ut using Matlab/SIMULINK sftware. The prpsed cnverter is suitable fr aerspace applicatins. Keywrds: - cnverters, push-pull cnverter, quasi-resnant cnverters, Zer vltage switching. I. INTRODUCTION Multi-utput PWM - cnverters are widely used in cunicatins, aerspace and cputer systes, as they are usually re cpact and less expensive than a cllectin f single-utput cnverters. Fig.1 shws the scheatic f single pwer cnverter with ultiple utputs, e.g. push-pull cnverter with ultiple secndary windings. In aerspace applicatins the allwable size and weight are highly restricted t accdate greater paylad. In the effrt t increase the pwer density f pwer supplies, the switching frequency is pushed t high values which, in PWM cnverter realizatins, nrally lead t cnsiderable pwer lss, high switching stresses, reduced reliability, and acustic nise. Anther significant drawback f the switch-de peratin is the EMI prduced due t large di/dt and dv/dt. T verce these shrt cings, new failies f QRCs are intrduced [1]-[].Few research papers have been presented abut the design and ipleentatin f push-pull hard switched and Quasi-resnant cnverters[3]-[5].push-pull cnverters is ainly used fr ediu and high pwer applicatins cpared t half-bridge and full-bridge cnverter. It has wide duty rati cntrl and it can be used fr ulti-utput applicatins with lw utput and input ripple current. This paper presents the design f ulti-utput push-pull ZVS-QRC. The prpsed ethd reduces the switching lsses and size f the cnverter. It can be used as high-density pwer supply fr aer-space applicatins. All siulatin wrks are carried ut using MATLAB/SIMULINK sftware. Figure 1 Multiple utputs using single pwer cnverter. II. ANALYSIS OF MULTI-OUTPUT PUSH-PULL ZVS QRC The prpsed push-pull tplgy is basically tw frward cnverters cnnected in anti-phase. An additinal tw resnant tanks are added in this tplgy cpared t PWM push-pull cnverter. The resnant 19 Page

2 Siulatin f Push-pull Multi-utput Quasi-resnant Cnverter tank shapes the switch vltage s that the active switches (S 1 and S ) are turned n at ZVS. Hence the turn-n lsses f the switch will be reduced cnsiderably cpared t PWM cnverters. Bth priary and secndary windings are arranged in a center-tapped cnfiguratin. The push-pull cnverter perates in tw quadrants (I and III) f the B-H curve, see-sawing back and frth as the each priary is activated. This allws the push-pull cnverter t deliver twice the axiu pwer than that f a frward cnverter. This akes the prpsed cnverter effective fr ediu and high pwer applicatins. The different des f peratin are explained in the fllwing sectin. Figure Circuit diagra f ulti-utput push-pull ZVS-QRC. Figure 3 Theretical resnant wavefrs f push-pull ZVS-QRC. T analyze its steady-state behavir, the fllwing assuptins are ade 1. The utput filter C f and the lad R R 1, are a cnstant sink f current I 1 and I respectively.. Seicnductr switches are ideal, i.e. n frward vltage drp in the n-state, leakage current in the ff state and n tie delays at bth. 3. Reactive current in the eleents are ideal. 4. Magnetizing inductance is larger than resnating inductance The fllwing paraeters are defined 1. Characteristic ipedance Z ( L r C ) r. Resnant angular frequency 3. Resnant frequency 1 ( L r * C r ) f / 4. Nralized Lad Resistance Page

3 R R L / Z 5. The priary current thrugh priary f transfrer (L ) is I I Siulatin f Push-pull Multi-utput Quasi-resnant Cnverter.1 MODES OF OPERATION The switch S 1 and S are alternatively pwer their respective windings. The resnating capacitrs C r1 and C r and resnating inductrs L r1 and are used t fr the resnant tank. The secndary vltage f the transfrer is rectified by fast recvery dides (D 1 and D ) and filtered t prduce a steady ripple free utput vltage V. Lwer and upper part f priary winding circuit is called here afterwards as upper and lwer..1.1 MODE 1: (t,t 1 ) UPPER: The switch S 1 is pened fr the beginning f a new cycle at t equal t t. The current flws thrugh resnant capacitr ( Cr1) and resnant inductr ( L r1). The capacitr vltage rises linearly fr t V. The capacitr vltage is given by the equatin, v I t / C cr1( When the resnant capacitr vltage reaches V at t = t 1.The duratin f this interval T d1 is given by d1 r T 4C V / I LOWER: The switch S pened in the previus cycle is still cntinued. The capacitr vltage v cr in the lwer part decreases linearly fr V t zer. The equatins fr v cr and i are given as v cr I ( V Z sin ωt i I cs t.1. MODE : ( t 1, UPPER: The series resnant L r1 and C r1 frs a resnant circuit. The state equatins are With initial cnditins dv di cr1 dt i 1( Cr1 1 dt ( V vcr1( ) 1 v cr1() V and i () I 1 The slutins fr the abve equatins are given by vcr1( V ) Z i 1( ) cs t r sin t At t equal t t, i 1 reaches zer value and v cr1 reaches its peak value as shwn in fig, 3a. They are given by T The duratin f the de d v cr1 V ) ( Z is given by T d t t1 LOWER: The switch S is turned n when V cr bece zer at t = t 1, t achieve zer vltage cnditin. During this stage the current i increases linearly and reaches the value I at t = t.the crrespnding state equatin fr i is given by di dt V L r The slutin f abve equatin is given by.1.3 MODE 3: t, ) ( t 3 i ) cs t UPPER: The equatins deterining this stage are di 1 dt ( V vcr1( ) 1 cr / dt i1( / Cr dv and 1 1 Page

4 With initial cnditins v i cr1() V () I 1 The slutin fr the equatins are given by i 1( ( I ( V Siulatin f Push-pull Multi-utput Quasi-resnant Cnverter / )cs t vcr 1 1( t T d 3 t4 t3 1 Td 3 ( 1 )sin [ V ( I Z d 3 ( ) / )sin t This stage terinates when V cr ) beces zer. The duratin f this stage is given by Where T ) ] The inductr current is given by LOWER: v cr is zer and With initial cnditins i 1 di 1 (sin [4V I Z]) )cs dt )) i () I The slutin fr abve equatin is.1.4 MODE 4: ) ( V vcr ( t i t ( t 3, t 4 ( )cs( ) UPPER: The switch S 1 is turned n when v cr1 bece zer t achieve zer vltage cnditin. During this de the current i 1 increases linearly and reaches the value I at t equal t t 4. The crrespnding state equatin is With initial cnditin The inductr current 1 di 1 dt V / 1 i () 1 )cs i ( is given by the equatin i1( ((V * ) (( I )cs ) This de terinates when inductr current bece I. The duratin f this stage is given by the equatin T d 4 t4 t3 T d 4 [ IZ 4V ](1 cs ) LOWER: The switch S is pened at t = t 4. The current flws thrugh resnant capacitr ( Cr ) and resnant inductr L r.the capacitr vltage rise s linearly fr zer t and it is gverned by equatin v cr ( ( I Cr1 At the end f this de, a new de cycle starts.. Theretical resnant wavefrs The theretical resnant wavefrs f the prpsed cnverter fr ne switching cycle are shwn in fig.3. Whenever there is a change in switching device fr ne state t anther, the circuit cnfiguratin changes. Each cnfiguratin is referred t as de. In this QRC, fur different stages are identified fr each half f the switching cycle..3 Design The design paraeters are given fr a ulti-utput push-pull ZVS-QRC with fllwing specificatins: V Page

5 Input vltage V 4V Output vltage f secndary1 V 1 5V Output Vltage f secndary V 1V Siulatin f Push-pull Multi-utput Quasi-resnant Cnverter Resnant frequency f 165kHz Switching frequency f s 5kHz Turns rati between priary and secndary n 1= N p1 N s n N p N.3 s The characteristic ipedance Z sqrt( L r C ) r The resnant capacitrs are assued t be equal Cr Cr1 Cr. 47icrF The resnant inductrs are assued t be equal 1. 16H III. OPEN LOOP STUDIES In this sectin the pen lp siulatin f ulti-utput push-pull ZVS-QRC circuit is realized with paraeters btained fr the design. The siulated resnant capacitr vltage and utput vltage f the cnverter are discussed in this sectin. The perfrance f the cnverter is studied fr different lad variatins. The cnverter is siulated using Matlab/SIMULINK sftware in pen lp with design paraeters. The SIMULNK del f the circuit is shwn in figure 4. The gating pulses applied t switch S 1 and S are shwn in fig. 5. It is bserved that the switch S 1 and S are turned n, when the resnant capacitr vltage beces zer t assure ZVS cnditin. The wavefr resebles the theretical wavefrs as shwn in fig 3. Figure 4 Siulink Mdel Diagra fr the Multi Output Push-Pull ZVS-QRC Figure 5 Siulated resnant wavefrs fr upper part and lwer part f priary. 3 Page

6 Siulatin f Push-pull Multi-utput Quasi-resnant Cnverter Figure 6 Siulated pen lp utput wavefrs f the secndary1 V 1 and secndary V (vlts). IV. CONCLUSION Theretical analysis and design prcedure f a new buck type push-pull ZVS-QRC was presented. The cnverter rated at 1W, perating at switching frequency f 5kHZ has been siulated using Matlab/SIMULINK sftware. Operating principle and theretical analysis are cnfired by siulatin results. The cnverter can als be ipleented in hardware which will give atching results as that f siulated results. Hence this is suitable fr high-density, ediu pwer requireent, fr exaple in aerspace applicatins. REFERENCES [1] Liu K.H. and LEE F.C.Y., Zer-vltage Switching Technique in DC-Dc Cnverters, IEEE Specialists Cnference Recrd, 1986,pp [] I.Barbi, J.C.Blacell,D.C.Martins and F.B.Liban, Buck Quasi-Resnant Cnverter perating at Cnstant Frequency:Analysis, Design and Experiantatin,IEEE,pp [3] Wildn C.P., de Araga Filh,I.Barbi, A Cparisn Between Tw Current-Fed Push-Pull DC-DC Cnverters-Analysis,Design and Experientatin, IEEE, 1996, pp [4] Grver V., T.Bascpe and I.Barbi, Islated Flyback-Current-Fed Push-Pull Cnverter Fr Pwer Factr Crrectin,IEEE,1996,pp [5] B.Swainathan and V.Raanarayanan, A Nvel Resnant Transitin Push-Pull DC-DC Cnverter,J.Indian Inst Sci,Nv.- Dec.4,pp Page

ZVS Boost Converter. (a) (b) Fig 6.29 (a) Quasi-resonant boost converter with M-type switch. (b) Equivalent circuit.

ZVS 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 information

A Novel Isolated Buck-Boost Converter

A 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 information

Design and Simulation of Dc-Dc Voltage Converters Using Matlab/Simulink

Design 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 information

Synchronous Motor V-Curves

Synchronous 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 information

1. Transformer A transformer is used to obtain the approximate output voltage of the power supply. The output of the transformer is still AC.

1. 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 information

A Non-Insulated Resonant Boost Converter

A Non-Insulated Resonant Boost Converter A Nn-Insulated Resnant Bst Cnverter Peng Shuai, Yales R. De Nvaes, Francisc Canales and Iv Barbi ISEA-Institute fr Pwer Electrnics and Electrical Drives, RWTH-Aachen University, Aachen, Germany Email:

More information

Time varying fields and Maxwell's equations Chapter 9

Time varying fields and Maxwell's equations Chapter 9 Tie varying fields and Maxwell's equatins hapter 9 Dr. Naser Abu-Zaid Page 9/7/202 FARADAY LAW OF ELETROMAGNETI INDUTION A tie varying agnetic field prduces (induces) a current in a clsed lp f wire. The

More information

A High Step-Down Interleaved Buck Converter with Active-Clamp Circuits for Wind Turbines

A High Step-Down Interleaved Buck Converter with Active-Clamp Circuits for Wind Turbines Energies 01, 5, 5150-5170; di:10.3390/en515150 Article OPEN ACCESS energies ISSN 1996-1073 www.mdpi.cm/jurnal/energies A High Step-Dwn Interleaved Buck Cnverter with Active-Clamp Circuits fr Wind Turbines

More information

ECE 2100 Circuit Analysis

ECE 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 information

Applying 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 :

Applying 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 information

A Comparison of AC/DC Piezoelectric Transformer Converters with Current Doubler and Voltage Doubler Rectifiers

A 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 information

Lab 11 LRC Circuits, Damped Forced Harmonic Motion

Lab 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 information

1) p represents the number of holes present. We know that,

1) p represents the number of holes present. We know that, ECE650R : Reliability Physics f Nanelectrnic Devices Lecture 13 : Features f FieldDependent NBTI Degradatin Date : Oct. 11, 2006 Classnte : Saakshi Gangwal Review : Pradeep R. Nair 13.0 Review In the last

More information

2. Find i, v, and the power dissipated in the 6-Ω resistor in the following figure.

2. Find i, v, and the power dissipated in the 6-Ω resistor in the following figure. CSC Class exercise DC Circuit analysis. Fr the ladder netwrk in the fllwing figure, find I and R eq. Slutin Req 4 ( 6 ) 5Ω 0 0 I Re q 5 A. Find i, v, and the pwer dissipated in the 6-Ω resistr in the fllwing

More information

Chapter 30. Inductance

Chapter 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 information

Harmonic Motion (HM) Oscillation with Laminar Damping

Harmonic Motion (HM) Oscillation with Laminar Damping Harnic Mtin (HM) Oscillatin with Lainar Daping If yu dn t knw the units f a quantity yu prbably dn t understand its physical significance. Siple HM r r Hke' s Law: F k x definitins: f T / T / Bf x A sin

More information

Copyright Paul Tobin 63

Copyright 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 information

Revision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax

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 information

Unit/Comments. %; Equal Output Loads %; Equal Output Loads Full Load

Unit/Comments. %; Equal Output Loads %; Equal Output Loads Full Load 600 series Single, Dual, Triple DC/DC Cnverter DESCRIPTIONS The 600 series 6 watts high perfrmance DC/DC cnverters are cst effective slutin t the high reliability and perfrmance requirements f pwer distributin

More information

GENERAL FORMULAS FOR FLAT-TOPPED WAVEFORMS. J.e. Sprott. Plasma Studies. University of Wisconsin

GENERAL 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 information

Lecture 2: Single-particle Motion

Lecture 2: Single-particle Motion Lecture : Single-particle Mtin Befre we start, let s l at Newtn s 3 rd Law Iagine a situatin where frces are nt transitted instantly between tw bdies, but rather prpagate at se velcity c This is true fr

More information

Series and Parallel Resonances

Series 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 information

THERMAL-VACUUM VERSUS THERMAL- ATMOSPHERIC TESTS OF ELECTRONIC ASSEMBLIES

THERMAL-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 information

Dead-beat controller design

Dead-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 information

Y.J. Cho **, Hazim Awbi** & Taghi Karimipanah* *) Fresh AB, SWEDEN **) University of Reading, UK

Y.J. Cho **, Hazim Awbi** & Taghi Karimipanah* *) Fresh AB, SWEDEN **) University of Reading, UK The Characteristics f Wall Cnfluent Jets fr Ventilated Enclsures 9 th Internatinal Cnference n Air Distributin in Rs niversity f Cibra PORTGAL Y.J. Ch **, Hazi Awbi** & Taghi Kariipanah* *) Fresh AB, SWEDEN

More information

rcrit (r C + t m ) 2 ] crit + t o crit The critical radius is evaluated at a given axial location z from the equation + (1 , and D = 4D = 555.

rcrit (r C + t m ) 2 ] crit + t o crit The critical radius is evaluated at a given axial location z from the equation + (1 , and D = 4D = 555. hapter 1 c) When the average bld velcity in the capillary is reduced by a factr f 10, the delivery f the slute t the capillary is liited s that the slute cncentratin after crit 0.018 c is equal t er at

More information

Bicycle Generator Dump Load Control Circuit: An Op Amp Comparator with Hysteresis

Bicycle 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 information

JAZAN University. Department: Electrical Engineering. Names & ID: Electronics LAB - 1/ / Electronics LAB - EngE : 314 G:...

JAZAN University. Department: Electrical Engineering. Names & ID: Electronics LAB - 1/ / Electronics LAB - EngE : 314 G:... Electrnics LAB - EngE : 314 G:... Electrnics LAB - 1/2-201. /201. Electrnics LAB - EngE : 314 G:... Electrnics LAB - 2/2-201. /201. Silicn JAZAN University Experiment 1: characteristics Electrnics LAB

More information

Sections 15.1 to 15.12, 16.1 and 16.2 of the textbook (Robbins-Miller) cover the materials required for this topic.

Sections 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 information

Three charges, all with a charge of 10 C are situated as shown (each grid line is separated by 1 meter).

Three charges, all with a charge of 10 C are situated as shown (each grid line is separated by 1 meter). Three charges, all with a charge f 0 are situated as shwn (each grid line is separated by meter). ) What is the net wrk needed t assemble this charge distributin? a) +0.5 J b) +0.8 J c) 0 J d) -0.8 J e)

More information

A Comparative Study on Predictive and ISVM Direct Torque Control Methods for a Doubly Fed Induction Machine Fed by an Indirect Matrix Converter

A Comparative Study on Predictive and ISVM Direct Torque Control Methods for a Doubly Fed Induction Machine Fed by an Indirect Matrix Converter A Cmparative Study n Predictive and ISVM Direct Trque Cntrl Methds fr a Dubly Fed Inductin Machine Fed by an Indirect Matrix Cnverter Dwnladed frm ijeee.iust.ac.ir at 1:59 IRDT n Tuesday May 8th 018 M.

More information

Lecture 13 - Boost DC-DC Converters. Step-Up or Boost converters deliver DC power from a lower voltage DC level (V d ) to a higher load voltage V o.

Lecture 13 - Boost DC-DC Converters. Step-Up or Boost converters deliver DC power from a lower voltage DC level (V d ) to a higher load voltage V o. ecture 13 - Bt C-C Cnverter Pwer Electrnic Step-Up r Bt cnverter eliver C pwer frm a lwer vltage C level ( ) t a higher la vltage. i i i + v i c T C (a) + R (a) v 0 0 i 0 R1 t n t ff + t T i n T t ff =

More information

Dr. Kasra Etemadi February 27, 2007

Dr. Kasra Etemadi February 27, 2007 Dr. Kasra Eteadi February 7, 7 Chapter 4:Transients Chapter 5: Sinusidal Surces Chapter 6: nnsinusidal surces Furier Trasr Transer Functin Filters Lwpass Filters Highpass Filters andpass Filters Surce

More information

Linearization of the Output of a Wheatstone Bridge for Single Active Sensor. Madhu Mohan N., Geetha T., Sankaran P. and Jagadeesh Kumar V.

Linearization 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 information

Verification of Quality Parameters of a Solar Panel and Modification in Formulae of its Series Resistance

Verification 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 information

Supplementary Course Notes Adding and Subtracting AC Voltages and Currents

Supplementary 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 information

PHYSICS Unit 3 Trial Examination

PHYSICS Unit 3 Trial Examination STAV Publishing Pty Ltd 005 PHYSICS Unit 3 Trial Examinatin SOLUTIONS BOOK Published by STAV Publishing Pty Ltd. STAV Huse, 5 Munr Street, Cburg VIC 3058 Australia. Phne: 6 + 3 9385 3999 Fax: 6 + 3 9386

More information

Impedance matching concept given ZL, design a matching network to have in=0 or selected value. matching. Zin (=Z Z o )

Impedance matching concept given ZL, design a matching network to have in=0 or selected value. matching. Zin (=Z Z o ) Chapter 5 Ipedance atching and tuning 5. Matching with luped eleents -sectin atching netwrks using Sith chart 5. Single-stub tuning shunt stub, series stub 5.3 Duble-stub tuning frbidden regin 5.4 The

More information

Relationships Between Frequency, Capacitance, Inductance and Reactance.

Relationships 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 information

Speed Synchronization of Single-Phase Induction Motors by Electromagnetic Shaft System

Speed Synchronization of Single-Phase Induction Motors by Electromagnetic Shaft System WA ANAON n Y and ONOL Ali. Akayleh, ad. Addasi, aleh A. Al-Jufut peed ynchrnizatin f ingle-phase nductin trs by lectragnetic haft yste AL. AKAYLH, AD. ADDA, ALH A. AL-JUOU * Departent f lectrical Pwer

More information

RECHARGEABLE batteries are extensively applied in

RECHARGEABLE batteries are extensively applied in 105 IEEE TRANSACTIONS ON INDUSTRY APPLICATIONS, VOL. 45, NO. 3, MAY/JUNE 009 Implementatin and Analysis f an Imprved Series-Laded Resnant DC DC Cnverter Operating Abve Resnance fr Battery Chargers Ying-Chun

More information

Current-Source Modular Medium-Voltage Grid- Connected System with High-Frequency Isolation for Photovoltaic Applications

Current-Source Modular Medium-Voltage Grid- Connected System with High-Frequency Isolation for Photovoltaic Applications Current-Surce Mdular Mediu-ltage Grid- Cnnected Syste with High-Frequency slatin fr Phtvltaic Applicatins Ahed Darwish *, and Mhaed A. Elgenedy, Meber, EEE * a.badawy@lancaster.ac.uk Abstract Large-scale

More information

Multi Level Reinjection ac/dc Converters for HVDC

Multi Level Reinjection ac/dc Converters for HVDC Multi Level Reinjectin ac/dc Cnverters fr HVDC Lasantha Bernard Perera A thesis presented fr the degree f Dctr f Philsphy in Electrical and Cmputer Engineering at the University f Canterbury, Christchurch,

More information

FE Analysis of a Vibrating Rigid Circular Piston in Water

FE Analysis of a Vibrating Rigid Circular Piston in Water FE Analysis f a Vibrating Rigid Circular Pistn in Water K. Jagadeeshl and M. S. Vijaya2 I-Sr. Lecturer, 2 -Visiting Prfessr, Center fr Electrnic Materials and Devices Research, M. S. Raaiah Schl f Advanced

More information

BASIC DIRECT-CURRENT MEASUREMENTS

BASIC 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 information

^YawataR&D Laboratory, Nippon Steel Corporation, Tobata, Kitakyushu, Japan

^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 information

Minimum Loss Design of a 100 khz Inductor with Litz Wire

Minimum Loss Design of a 100 khz Inductor with Litz Wire IEEE IAS Annual Meeting New Orleans, LA, Octber 5-9, 1997 Minimum Lss Design f a 100 khz Inductr with Litz Wire Ashkan Rahimi-Kian Ali Keyhani Jeffrey M. Pwell Student Member, IEEE Senir Member, IEEE Department

More information

Current/voltage-mode third order quadrature oscillator employing two multiple outputs CCIIs and grounded capacitors

Current/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 information

Chapter 16. Capacitance. Capacitance, cont. Parallel-Plate Capacitor, Example 1/20/2011. Electric Energy and Capacitance

Chapter 16. Capacitance. Capacitance, cont. Parallel-Plate Capacitor, Example 1/20/2011. Electric Energy and Capacitance summary C = ε A / d = πε L / ln( b / a ) ab C = 4πε 4πε a b a b >> a Chapter 16 Electric Energy and Capacitance Capacitance Q=CV Parallel plates, caxial cables, Earth Series and parallel 1 1 1 = + +..

More information

TOPPER SAMPLE PAPER 2 Class XII- Physics

TOPPER 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 information

Inertial Mass of Charged Elementary Particles

Inertial Mass of Charged Elementary Particles David L. Bergan 1 Inertial Mass Inertial Mass f Charged Eleentary Particles David L. Bergan Cn Sense Science P.O. Bx 1013 Kennesaw, GA 30144-8013 Inertial ass and its prperty f entu are derived fr electrdynaic

More information

Micro and Smart Systems

Micro 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 information

Module 4: General Formulation of Electric Circuit Theory

Module 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 information

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string?

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string? Term: 111 Thursday, January 05, 2012 Page: 1 Q1. A string f length L is fixed at bth ends. Which ne f the fllwing is NOT a pssible wavelength fr standing waves n this string? Q2. λ n = 2L n = A) 4L B)

More information

Chapter - 7 ALTERNATING CURRENT

Chapter - 7 ALTERNATING CURRENT hapter - 7 AENANG UEN A simple type f ac is ne which varies with time is simple harmnic manner- epresented by sine curve. ac vltage = sin t - Where = NAB Amplitude and = NAB ac current - - sin Where, Amplitude

More information

SFDMB3638F. Specifications and Applications Information. orce LED Driver. Mass: 7 grams typ. 10/15/08 Preliminary. Package Configuration

SFDMB3638F. 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 information

CHAPTER 5. Solutions for Exercises

CHAPTER 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 information

1.1 The main transmission network of Eskom The classical two generator model 11

1.1 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 information

T(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.

T(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 information

Lecture 02 CSE 40547/60547 Computing at the Nanoscale

Lecture 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 information

Scheduling of a pipeless multi-product batch plant using mixed-integer programming combined with heuristics

Scheduling of a pipeless multi-product batch plant using mixed-integer programming combined with heuristics Scheduling f a pipeless ulti-prduct batch plant using ixed-integer prgraing cbined with heuristics Sebastian Panek 1, Sebastian Engell 1, Cathrin Lessner 2 1 University f Drtund Prcess Cntrl Lab (BCI-AST),

More information

Edexcel GCSE Physics

Edexcel GCSE Physics Edexcel GCSE Physics Tpic 10: Electricity and circuits Ntes (Cntent in bld is fr Higher Tier nly) www.pmt.educatin The Structure f the Atm Psitively charged nucleus surrunded by negatively charged electrns

More information

Section I5: Feedback in Operational Amplifiers

Section 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 information

Modulation Technique to Reverse Power Flow for the Isolated Series Resonant DC-DC Converter with Clamped Capacitor Voltage

Modulation Technique to Reverse Power Flow for the Isolated Series Resonant DC-DC Converter with Clamped Capacitor Voltage Mdulatin Technique t Reverse Pwer Flw fr the Islated Series Resnant DC-DC Cnverter with Clamped Capacitr Vltage Yu Du, Student Member, IEEE, Srdjan M. Lukic, Member, IEEE, Bris S. Jacbsn, Senir Member,

More information

Modelling of NOLM Demultiplexers Employing Optical Soliton Control Pulse

Modelling of NOLM Demultiplexers Employing Optical Soliton Control Pulse Micwave and Optical Technlgy Letters, Vl. 1, N. 3, 1999. pp. 05-08 Mdelling f NOLM Demultiplexers Emplying Optical Slitn Cntrl Pulse Z. Ghassemly, C. Y. Cheung & A. K. Ray Electrnics Research Grup, Schl

More information

Phys102 Final-061 Zero Version Coordinator: Nasser Wednesday, January 24, 2007 Page: 1

Phys102 Final-061 Zero Version Coordinator: Nasser Wednesday, January 24, 2007 Page: 1 Crdinatr: Nasser Wednesday, January 4, 007 Page: 1 Q1. Tw transmitters, S 1 and S shwn in the figure, emit identical sund waves f wavelength λ. The transmitters are separated by a distance λ /. Cnsider

More information

TURN-ON SIMULATION OF FIELD-CONTROLLED THYRISTOR

TURN-ON SIMULATION OF FIELD-CONTROLLED THYRISTOR SIMULATION OF SEMICONDUCTOR DEVICES AND PROCESSES Vl. 4 Edited by W. Fichtner, D. Aetnmer - Zurich (Switzerland) September 12-14,1991 - Hartung-Grre TURN-ON SIMULATION OF FIELD-CONTROLLED THYRISTOR Adrian

More information

Q1. A) 48 m/s B) 17 m/s C) 22 m/s D) 66 m/s E) 53 m/s. Ans: = 84.0 Q2.

Q1. A) 48 m/s B) 17 m/s C) 22 m/s D) 66 m/s E) 53 m/s. Ans: = 84.0 Q2. Phys10 Final-133 Zer Versin Crdinatr: A.A.Naqvi Wednesday, August 13, 014 Page: 1 Q1. A string, f length 0.75 m and fixed at bth ends, is vibrating in its fundamental mde. The maximum transverse speed

More information

HEAT CONDUCTION IN CONVECTIVELY COOLED ECCENTRIC SPHERICAL ANNULI A Boundary Integral Moment Method

HEAT CONDUCTION IN CONVECTIVELY COOLED ECCENTRIC SPHERICAL ANNULI A Boundary Integral Moment Method Yilazer, A., et al.: Heat Cnductin in Cnvectively Cled Eccentric... THERMAL SCIENCE, Year 017, Vl. 1, N. 5, pp. 55-66 55 Intrductin HEAT CONDUCTION IN CONVECTIVELY COOLED ECCENTRIC SPHERICAL ANNULI A Bundary

More information

APPLICATION GUIDE (v4.1)

APPLICATION GUIDE (v4.1) 2.2.3 VitalSensrs VS-300 Sensr Management Statin Remte/Relay Guide Implementing Remte-IN/Relay-OUT Digital I/O Fieldbus Objective: Equipment: Becme familiar with the instrument wiring requirements fr the

More information

Physics 2B Chapter 23 Notes - Faraday s Law & Inductors Spring 2018

Physics 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 information

Coupled Inductors and Transformers

Coupled Inductors and Transformers Cupled nductrs and Transfrmers Self-nductance When current i flws thrugh the cil, a magnetic flux is prduced arund it. d d di di v= = = dt di dt dt nductance: = d di This inductance is cmmnly called self-inductance,

More information

Part a: Writing the nodal equations and solving for v o gives the magnitude and phase response: tan ( 0.25 )

Part a: Writing the nodal equations and solving for v o gives the magnitude and phase response: tan ( 0.25 ) + - Hmewrk 0 Slutin ) In the circuit belw: a. Find the magnitude and phase respnse. b. What kind f filter is it? c. At what frequency is the respnse 0.707 if the generatr has a ltage f? d. What is the

More information

C Soldering Temperature, for 10 seconds 300 (1.6mm from case )

C Soldering Temperature, for 10 seconds 300 (1.6mm from case ) l l l l l l Advanced Prcess Technlgy Dynamic dv/dt Rating 175 C Operating Temperature Fast Switching Fully Avalanche Rated Lead-Free Descriptin Fifth Generatin HEXFET Pwer MOSFETs frm Internatinal Rectifier

More information

Physics 102. Second Midterm Examination. Summer Term ( ) (Fundamental constants) (Coulomb constant)

Physics 102. Second Midterm Examination. Summer Term ( ) (Fundamental constants) (Coulomb constant) ε µ0 N mp T kg Kuwait University hysics Department hysics 0 Secnd Midterm Examinatin Summer Term (00-0) July 7, 0 Time: 6:00 7:0 M Name Student N Instructrs: Drs. bdel-karim, frusheh, Farhan, Kkaj, a,

More information

Lecture XXX. Approximation Solutions to Boltzmann Equation: Relaxation Time Approximation. Readings: Brennan Chapter 6.2 & Notes. Prepared By: Hua Fan

Lecture XXX. Approximation Solutions to Boltzmann Equation: Relaxation Time Approximation. Readings: Brennan Chapter 6.2 & Notes. Prepared By: Hua Fan Prepared y: Hua Fan Lecture XXX Apprxiatin Slutins t ltann Equatin: Relaxatin ie Apprxiatin Readings: rennan Chapter 6. & Ntes Gergia Insitute echnlgy ECE 645-Hua Fan Apprxiatin Slutins the ltann Equatin

More information

L a) Calculate the maximum allowable midspan deflection (w o ) critical under which the beam will slide off its support.

L a) Calculate the maximum allowable midspan deflection (w o ) critical under which the beam will slide off its support. ecture 6 Mderately arge Deflectin Thery f Beams Prblem 6-1: Part A: The department f Highways and Public Wrks f the state f Califrnia is in the prcess f imprving the design f bridge verpasses t meet earthquake

More information

Oscillator. Introduction of Oscillator Linear Oscillator. Stability. Wien Bridge Oscillator RC Phase-Shift Oscillator LC Oscillator

Oscillator. 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 information

INDUCTANCE Self Inductance

INDUCTANCE Self Inductance DUCTCE 3. Sef nductance Cnsider the circuit shwn in the Figure. S R When the switch is csed the current, and s the magnetic fied, thrugh the circuit increases frm zer t a specific vaue. The increasing

More information

Protection of ungrounded systems using an advanced relay element

Protection 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 information

Kinetics of Particles. Chapter 3

Kinetics of Particles. Chapter 3 Kinetics f Particles Chapter 3 1 Kinetics f Particles It is the study f the relatins existing between the frces acting n bdy, the mass f the bdy, and the mtin f the bdy. It is the study f the relatin between

More information

ENG2410 Digital Design Sequential Circuits: Part B

ENG2410 Digital Design Sequential Circuits: Part B ENG24 Digital Design Sequential Circuits: Part B Fall 27 S. Areibi Schl f Engineering University f Guelph Analysis f Sequential Circuits Earlier we learned hw t analyze cmbinatinal circuits We will extend

More information

4) What is the magnitude of the net electric field at the center of the square?

4) What is the magnitude of the net electric field at the center of the square? Fur charges are n the fur crners f a square. Q = +5C, Q = -0C, Q 3 = +5C, Q 4 = -0C. The side length f each side f the square is 3 m. Q Q ) What is the directin f the frce n Q due t ONLY Q 4? (a) up (b)

More information

Plan o o. I(t) Divide problem into sub-problems Modify schematic and coordinate system (if needed) Write general equations

Plan o o. I(t) Divide problem into sub-problems Modify schematic and coordinate system (if needed) Write general equations STAPLE Physics 201 Name Final Exam May 14, 2013 This is a clsed bk examinatin but during the exam yu may refer t a 5 x7 nte card with wrds f wisdm yu have written n it. There is extra scratch paper available.

More information

SIMPLIFIED sra11c AND DYNAMIC MODELS OF THE 3-LOOP ACI1VE POWER FACTOR CORREC11ON SYSTEMS

SIMPLIFIED sra11c AND DYNAMIC MODELS OF THE 3-LOOP ACI1VE POWER FACTOR CORREC11ON SYSTEMS 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

More information

Numerical Simulation of the Thermal Resposne Test Within the Comsol Multiphysics Environment

Numerical Simulation of the Thermal Resposne Test Within the Comsol Multiphysics Environment Presented at the COMSOL Cnference 2008 Hannver University f Parma Department f Industrial Engineering Numerical Simulatin f the Thermal Respsne Test Within the Cmsl Multiphysics Envirnment Authr : C. Crradi,

More information

NATURAL CONVECTION HEAT TRANSFER FROM A HEAT SINK WITH FINS OF DIFFERENT CONFIGURATION

NATURAL CONVECTION HEAT TRANSFER FROM A HEAT SINK WITH FINS OF DIFFERENT CONFIGURATION Internatinal Jurnal f Innvatin and Applied Studies ISSN 2028-9324 Vl. 9 N. 3 Nv. 2014, pp. 1043-1047 2014 Innvative Space f Scientific Research Jurnals http://www.ijias.issr-jurnals.rg/ NATURAL CONVECTION

More information

ECE 2100 Circuit Analysis

ECE 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 information

ANALYSIS OF FILL FACTOR LOSSES IN THIN FILM CdS/CdTe PHOTOVOLTAIC DEVICES

ANALYSIS OF FILL FACTOR LOSSES IN THIN FILM CdS/CdTe PHOTOVOLTAIC DEVICES ANALYSIS OF FILL FACTOR LOSSES IN THIN FILM CdS/CdTe PHOTOVOLTAIC DEVICES T. Ptlg, N. Spalatu, V. Cibanu,. Hiie *, A. Mere *, V. Mikli *, V. Valdna * Department Physics, Mldva State University, 60, A.

More information

IMPROVEMENTS TO VOLTAGE SAG RIDE-THROUGH PERFORMANCE OF AC VARIABLE SPEED DRIVES

IMPROVEMENTS TO VOLTAGE SAG RIDE-THROUGH PERFORMANCE OF AC VARIABLE SPEED DRIVES IMPOVENTS TO VOLTAGE SAG IDE-THOUGH PEFOMANCE OF AC VAIABLE SPEED DIVES aj Narayanan, Dn Platt, Sarath Perera Integral Energy Pwer Quality Centre Schl f Electrical, Cmputer and Telecmmunicatins Engineering

More information

(2) Even if such a value of k was possible, the neutrons multiply

(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 information

TEMPERATURE CONSIDERATIONS FOR SCR CONTROLS

TEMPERATURE CONSIDERATIONS FOR SCR CONTROLS AN 10-18 Applicatin Nte 10-18 PAYNE ENGINEERING TEMPERATURE CONSIDERATIONS FOR SCR CONTROLS q = (h c + h r ) A (T s - T amb ) TEMPERATURE CONSIDERATIONS FOR SCR CONTROLS Thyristr cntrls - mre cmmnly called

More information

Electric Current and Resistance

Electric 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 information

clicker 1/25/2011 All C s are 8.00 nf. The battery is 12 V. What is the equivalent capacitance? summary o

clicker 1/25/2011 All C s are 8.00 nf. The battery is 12 V. What is the equivalent capacitance? summary o /5/0 summary C = ε / d = πε / ln( b / a ) ab C = 4πε 4πε a b a b >> a Capacitance Parallel plates, caxial cables, Earth Series and parallel cmbinatins Energy in a capacitr Dielectrics Dielectric strength

More information

Supply Voltage Effects on the Operation of Residential Air Conditioning Appliances: Experimental Analysis

Supply Voltage Effects on the Operation of Residential Air Conditioning Appliances: Experimental Analysis upply Vltage Effects n the Operatin f Residential Air Cnditining Appliances: Experimental Analysis J.M. Maza Ortega 1, M. Burgs Payán 1, J.M. Rmer Grdón 2 and M. Pinilla Rdríguez 2 1 Department f Electrical

More information

Department of Electrical Engineering, University of Waterloo. Introduction

Department of Electrical Engineering, University of Waterloo. Introduction Sectin 4: Sequential Circuits Majr Tpics Types f sequential circuits Flip-flps Analysis f clcked sequential circuits Mre and Mealy machines Design f clcked sequential circuits State transitin design methd

More information

Physics 321 Solutions for Final Exam

Physics 321 Solutions for Final Exam Page f 8 Physics 3 Slutins fr inal Exa ) A sall blb f clay with ass is drpped fr a height h abve a thin rd f length L and ass M which can pivt frictinlessly abut its center. The initial situatin is shwn

More information

SSR study for the Thyristor Controlled Series Compensation application on the Kanpur-Ballabgarh 400kV line in India

SSR study for the Thyristor Controlled Series Compensation application on the Kanpur-Ballabgarh 400kV line in India SSR study fr the Thyristr Cntrlled Series Cpensatin applicatin n the Kanpur-Ballabgarh kv line in India Sujatha Subhash, A K Tripathy, K R Padiyar, Satish Nayyar, Manj Kuar, P J Thakkar & K K Arya Abstract

More information

A Variable Voltage MPPT Control Method for Photovoltaic Generation System

A Variable Voltage MPPT Control Method for Photovoltaic Generation System WSEAS TRANSACTIONS n CIRCUITS and SYSTEMS A Variable Vltage MPPT Cntrl Methd fr Phtvltaic Generatin System Liu Liqun Department f Electrical Engineering, Shanghai Jiatng University, Shanghai, 4, China;

More information

SOFT MASSIVE SPRING Objectives: Apparatus: Introduction:

SOFT MASSIVE SPRING Objectives: Apparatus: Introduction: SOFT MASSIVE SPRING Objectives: ) T deterine the spring cnstant and the ass crrectin factr fr the given sft assive spring by static (equilibriu extensin) ethd. 2) T deterine the spring cnstant and the

More information