Buck ZVS DC-DC Quasi-Resonant Converter: Design, Modeling, Simulation and Experimentation

Size: px
Start display at page:

Download "Buck ZVS DC-DC Quasi-Resonant Converter: Design, Modeling, Simulation and Experimentation"

Transcription

1 hp://dx.doi.og/.5755/j.eee ELEKTRNKA R ELEKTRTECHNKA, N 39-5, VL. XX, N. X, XX Buck ZV C-C Quasi-Resonan Convee: esign, Modeling, imulaion and Expeimenaion Nikolay L. Hinov, Nikolay R. Rangelov epamen of of Powe Eleconics, Technical Univesiy of ofia, Bul Kl. hidski 8, ofia, Bulgaia, hinov@u-sofia.bg, nikan8@gmail.com Absac n he pape wok a expeimenal sudy has been made wih pacical end, of a Buck C C quasi esonan convee, woking wih ZV ( Zeo Volage wiching ). n he wok a mahemaical expessions, fo he paamees, which descibe he wok of he powe pa of he cicui, has been made. Wih hei help a mehod fo designing of a Buck ZV C C quasi esonan convee has been poposed. The advanage of his mehod is he use of simple expessions, which faciliae he designing, bu in he same ime an accepable eo of % is kep, commensuae wih he oleance of he values of he eacive elemens (capacio and induco). The veificaion of hese expessions has been made wih modeling (Malab/imulink), compue simulaions (LTpice) and expeimenal measuemens on a laboaoy sand. ndex Tems Zeo volage swiching, C-C powe convees, of swiching.. NTRUCTN ne of he main mehods fo inceasing he efficiency of convees of elecical enegy is he deceasing of he swiching loses in he powe semiconduco elemens [9,, ]. Theefoe a widely used mehod fo achieving his is he using of a sof swiching shif swiching of he powe elemens on zeo volage o zeo cuen. Fo some convees his is achieved by viue of cicui feaues (fo example esonan invees), and fo ohes by using of a addiional elemens (capacio o induco), which ae conneced paallel o seial o he semiconduco swich. [, 4, 5]. Thus paallel o seial esonan cicuis can be made. These cicuis ae well known in he lieaue wih he name quasi esonan convees. n his pape wok a sudy of a Buck ZV quasi esonan convee has been made. The analysis of hese convees ae in [4, 5, 3], bu hee ae some inaccuacies and incoecly idenified values, and in addiion hese analyses ae no useable fo designing, which is one of he puposes of his wok.. EGN-RENTE ANALY F BUCK ZV QUA-RENANT CNVERTER n figue is shown he cicui of a Buck ZV quasi esonan C-C convee. The cicui consis of ansiso V, diode, file elemens L and C, Load R L esonan Manuscip eceived Apil XX, XX; acceped Apil XX, XX. This eseach was funded by a gan (No.3ПД9-3/3) fom he Reseach Council of he Technical Univesiy of ofia. elemens L и C, which povide he zeo volage swiching. Vin + _ L i W C C Fig.. Cicui of a BUCK ZV convee i The analyze is made unde seady sae and assumpion ha all elemen ae pefec. The cicui is woking in coninuous conducion mode wih negligible ipples hough he file induco. ue o he esonan cicui C -L fo he analysis of he convee some specific aios ae used [4, 5, 9]: - Resonan fequency of he seial L -C cicui fo ideal elemens: = () LC - Raio beween conol fequency and he fequency of he esonan cicui: f s v = () f - Chaaceisic impedance of he esonan cicle: L Z = = L = (3) C C - Nomalized load esisance: RL RL RL CR L R' = = = CR L = = (4) Z L L - Raio beween oupu and inpu volage of he convee ( C volage ansfe funcion ): V = (5) - Nomalized iniial esonan induco and swich cuen when he swich uns on: il () i () L h = = (6) i L C RL

2 ELEKTRNKA R ELEKTRTECHNKA, N 39-5, VL. XX, N. X, XX - uy aio: = on (7) Т The wok of he sudied cicui is shown by he wavefoms on figue (when he value of h=). uing one peiod we can see fou diffeen woking sages: age ( < Т ) The esonan induco accumulae enegy. The swich and he diode ae uned on. uing his sage cuens and volages have he following condiions: V =, L =, C =, V LR = V, and he cuen hough he swiching induco is: U G = L ( ) ( ) L L L + = L + i V d i i () (8) i L i i C u U u L U i u U N 3 FF Fig.. Time wavefoms when he convee is woking. Fo he pupose of he sudy i is convenienly o obain expessions in elaive unis, using he expessions menioned above in he pape wok. Thus he cuen hough he induco L is: il ( ) ( ) ' s is s R = = s+ h (9) The elaionship beween he cuen hough he diode i, and he cuen hough he swich i in he cicui is: i = i = ( i s/ ) () o fo he cuen hough he diode, in elaive unis: i( s) R ' = h () This sage ends when he cuen ough he diode becomes zeo. age ( < ) he diode is uned off. uing his sage he following ems ae execued: V =, CR =, =, is = i LR =, V LR =, и V = V. This sage ends in he momen when he ansiso uns off fom he conol sysem. age 3 ( < Т 3) chaging of he esonan capacio and boh diode and he ansiso ae uned off. uing his sage he following ems ae in effec: i =, =, LR = CR T =, V LR =. The volage ove he capacio is deemined wih he following expession: v = vc = i ( ) ( ) C d vc C + = π, () О V = ( π) = ( π) C CR L Whee VC ( ) s =. Afe ansfomaion fo he volage ove he ansiso and he diode, in elaive unis is: v = ( π) R' (3) v = ( π) R' This ends when he volage ove he diode becomes zeo - v (s 3) =. Fom his em we ge he expession: R ' = π+ M (4) 3 VC age 4 ( 3 < T) in is beginning he diode uns on. By he made assumpions fo pefec elemens in he cicui sas a seial esonan pocess wih he following iniial condiions: LR ( s 3) = и v C ( s 3) = V ( s 3) = V. eemine he cuen in he esonan cicui can be made wih diffeen mehods [4, 5, 9, 3], and in elaive unis i is: il i C 3 = = cos (5) A Fom (5) and () he elaive cuen hough he diode is: i 3 = cos (6) A woking in seady mode he following condiion is execued: il ( π ) = i ( ) L = h (7) Fom is applying in (5) and by using of (4) we deemine: π ( ) R' cos = h (8) The volage ove he esonan induco, duing sage 3 is: dil M VC 3 VL = L = sin (9) d( ) R' The volage ove he swich is: V = VC = i ( ) ( 3) C d vc C + = () 3 VM VC 3 = sin + R ' n elaive unis is: v 3 = sin + () R' Fo achieving ZV mode, he following condiion mus be fulfilled: v ( π ) = v ( ) =. o he elaion beween he used facos is: π ( ) R' R' sin = () Afe igonomeic ansfomaions of (8) and () ges:

3 ELEKTRNKA R ELEKTRTECHNKA, N 39-5, VL. XX, N. X, XX R ' h M = (3) VC Fo he duy aion we ge: = = π + h accosh (4) T π Fo he puposes of he design i is necessay o deemine he elaion beween duy aio and he volage ansfe funcion a consan cuen. niially he aveage value of he inpu cuen is deemined: π ( h) = id s ( s) = (5) π 4π h By assuming fo pefec elemens and lack of losses in he cicui elemens he following elaion is in effec: V =V. Fom he definiion fo he volage ansfe funcion ges: V ( ) h = = = (6) V 4π h n [4, 5, 6, 9, ] ae examined and analyzed he impac of he iniial condiions fo cuen ove he wok of he convee, and he scope of he load esisance fo ZV wok. Fo simplificaion of he calculaions i is ecommended o choose he value h =. Moeove his mode is bes fom he poin of view fo he sess and use of he cicui elemens [4, 5, 3].. METHLGY FR EGNNG The main daa necessay fo designing a Buck ZV convee ae: - npu volage V ; - upu volage V ; - upu cuen ; - Ripple faco fo oupu volage and cuen; - Conol fequency f. Fom he necessay daa menioned above we can see ha hese ae he necessay values fo calculaing andom convees (independenly fom is woking mode is i wih zeo swiching o no). Fo fis sep i begins wih calculaing of he convee wihou esonan cicui (C - L, shown on figue ) sandad Buck convee wih had swiching. Afe ha he values of he esonan elemens mus be deemine. Because he main pupose is o sugges a simple and easy mehod fo designing, a value of h= has been chosen. n his case a simplified kind of he expessions is eceived (3) (4) and (6): R' = M (8) VC 3 π + f f =.99 (9) 4π f f 3π + 3 f f =.9887 (3) 4π f f Excep he eacive componens a suiable semiconduco elemens mus be chosen. This is accomplishing by using he expessions fo hei maximum cuen and volage sess. Fom he pesened analyze he values fo maximum cuen and volage acoss he ansiso is deemined by: M = (3) VM = + V (3) R ' Fo he diode he maximum cuen and volage sess ae: M = (33) VM = V (34) f couse he fequency paamees of he elemens mus be deemined oo duing he design and he pacical ealizaion, because hese cicuis ae woking fo high fequency. [4, 9,, ]. EXAMPLE The necessay daa fo designing is: V i = 3V; V =5V; =ma; f =khz and we choose o wok wih h =. A convenional Buck C C convee wih had swiching is calculaed, by one of he well known design mehods, like he ones in [, 8, 9, ]. Fom he designing we ge he following esuls fo he values of he elemens: L = µh, C= 5µF и R L=75Ω. An induco wih L = 5µH and a capacio wih C= 5,7µF ae chosen. The values of hese file elemens ae deemine so hey can povide a wok in coninuous mode and se values fo he oupu cuen and oupu volage ipple. Afe ha he calculaion of he esonan elemens begins. Fom expession (8) follows ha, M VC=R =,5. Z is deemine by (4) and is value is Z =75/,5=5. Fom (3) afe we eplace he deemined ill now paamees, he value fo he esonan fequency of he seial esonan cicui is f =97775Hz; Wih he deemined esonan fequency he value of he duy aio fom (9) is 54,%; Afe ha he esonan induco mus be deemine fom (4), is value is: L =,73µH; The esonan capacio C is calculaed fom (4) and i is: C =5,3656nF. Fom he deemined values we can see ha he induco and he capacio, in he esonan cicui, ae no wih sandad values. Because of he specificiy of he offeed elemens (hei values ae in sandad ode), a using of a elemens wih sandad values is equied. Thee ae wo possible mehods fo sele his ask, like we can see fom expession (9) and (3). f he values of he esonan capacio and induco ae changed, he duy aio mus be changed oo o he conol fequency. o he values of he elemens poined ou in he assignmen ae kep. The easies way is o change he duy aio (so he woking fequency is kep, which lead o suppession of he elecomagneic inefeence). n his case a sandad values fo he esonan elemens ae se and wih hei new values, he fequency of he esonan cicui mus be calculaed again. o an induco wih L = µh and capacio wih C =6,8nF ae chosen. Afe sandad values ae been used of L and C, hey ae eplaced in (4), he new value of he esonan fequency is - f = 8653Hz. Recalculaion of he duy aio mus be done and he new value is - = 5,6%. Wih hese daa and ceain values he values of he ansiso should be bigge han U M=6V and M=,A, and fo he diode - U M=3V и M=,4A. f couse he elemens should wok wih fequency bigge han khz.

4 ELEKTRNKA R ELEKTRTECHNKA, N 39-5, VL. XX, N. X, XX V. MULATN TUE AN MELNG By he so deemined values of he convee elemens, simulaion eseaches and modeling have been made wih Malab/imulink and LTpice. 3mA 8mA 6mA -6mA -8mA L -3mA 3mA d 35mA -3mA 7V V 3V Fig. 3. Malab/imulink model of a BUCK ZV quasi esonan C-C convee. The pupose of he eseach is checking of he design mehod. n figue 3 is shown he model of he convee in Malab/imulink. n figue 4 he esuls of he modeling ae shown (fom up o down ae cuen ough he ansiso; volage ove he ansiso and he conol signal fo he ansiso). -7V VG 6V 4V V V 8V 6V 4V V V -V.9ms.9ms.93ms.94ms.95ms.96ms.97ms.98ms.99ms 3.ms 3.ms 3.ms Fig. 6. Resuls fom he simulaion of a BUCK ZV quasi esonan C-C convee wih LTpise. Fom he wo simulaion sudies we can see ha he heoeical calculaion and he coecion, elaed o he change of he duy aio, due o using swiching elemens wih sandad values, ae confimed. is impoan o menion ha he condiions fo zeo volage swiching ae fulfilled. Fig. 4. Resuls fom modeling а BUCK ZV quasi esonan C-C convee wih Malab/imulink. n figue 5 is shown he cicui of he sudied convee, which will be simulaed in LTpice. n figue 6 ae shown he esuls of he simulaion (fom up o down ae cuen hough he esonan induco; cuen hough he ansiso; volage ove he ansiso and conol signal fo he ansiso). V. EXPERMENTAL REEARCHE The expeimens ae made on an expeimenal sand, shown on figue 7. The sofwae pa of he conol sysem is implemened wih he sofwae fo visual pogamming LabView, and fo he hadwae pa of he conol sysem a chassis CompacAQ is used wih he conneced modules o i N9 8 inpu AC and N94-8 pogammable TTL inpus/oupus. Fig. 5. imulaion model of a BUCK ZV quasi esonan C-C convee in LTpise Fig. 7. Expeimenal sand By LabView we can achieve a wide ange of vaiaions of he conol fequency and he duy aio, which is vey comfoably fo expeimenal sudies. n figue 8 is shown he block diagam of he pulse geneao.

5 ELEKTRNKA R ELEKTRTECHNKA, N 39-5, VL. XX, N. X, XX C 6.8 nf L uh L 5 uh W C Vin C 5.7uF RL 75Ω Fig.. Powe cicui of he expeimenal sand. Fig. 8. Block diagam of he pulse geneao n he following figues ae shown he esuls fom he measuemens wih he oscilloscope. n figue ae shown he volage ove he ansiso and he conol pulses. Fom he gaphical esuls we can see ha he zeo volage swiching is achieved. Fig. 9. Fon panel of he pulse geneao n figue 9 is shown he fon panel, fom his panel we can change he fequency and he duy aio of he viual insumen. As we can see fom he fon panel i is vey comfoable o se he paamees of he conol pulse fo he ansiso and so we can achieve diffeen woking egimes of he convee. Fo he ealizaion of he powe cicui he following elemens ae used: one MFET ansiso model 6R65, high fequency diode model 6APU4, dive HCPL3 wih inegaed opocouple, esonan induco wih he following value of µh, esonan capacio wih he following value of 6,8nF, file induco wih he following value of 5µH, file capacio wih he following value of 5,7µF and load esiso wih he following value of 75Ω. The cicui of he expeimenal sand of a ZV Busk C-C convee is shown on figue. The measuemens ae done wih oscilloscope model Tekonix T. The volages ae measued wih volage scope wih scale :. The cuens ae measued wih cuen scope. Fig.. Volage acoss he ansiso and conol pulses. n figue ae shown he cuen hough he ansiso and he volage ove i. As we can see when he ansiso uns on we have zeo volage and cuen swiching. These esuls show ha he poposed mehod fo designing is coec, because in he calculaions we have acceped zeo iniial condiion fo he cuen. n figue 3 ae shown he volage ove he swich and he cuen hough he esonan induco and on figue 4 he oupu volage ipples. When woking wih conol fequency of khz allows us he achieving of small ipples (96mV), when he oupu file capacio is wih small value 5,7µF [3, ].

6 ELEKTRNKA R ELEKTRTECHNKA, N 39-5, VL. XX, N. X, XX calculaions esuls, simulaions, mahemaical modeling and expeimens is shown. As we can see hee is a vey good coincidence beween hem (diffeence beween hem no moe han %), despie he assumpions and simplificaions. TABLE. CMPARNG F THE REULT. Paamees LTpice imulink Expeimens Calculaed/ e V (V) (ma) Δ V (mv) V M (V) M (ma) Fig.. Volage ove he ansiso and he cuen hough i. n he ohe side i would be ineesing achieving zeo volage swiching wih possible low value of he volage ove he ansiso. The feaue sudies of he auhos ae dieced in fuhe opimizaions of he design mehod, which will lead o easie way of choosing he elemens of he esonan cicui. All his will lead o a lile volage sess of he powe ansiso. ACKNWLEGMENT This wok is suppoed by he Reseach Council of he Technical Univesiy of ofia unde Conac :3ПД9-3/3 udy of C C convees fo elecical enegy wih low swiching losses. Fig. 3. Volage ove he ansiso and ove he esonan induco. Fig. 4.upu volage ipples.. CNCLUN The made simulaion and expeimenal eseaches of he Buck ZV C C convee check and confimed he poposed, fom he auhos, design mehod. The main pupose in he aicle is finding a comfoable and easy expession fo simple designing of convees, wihou using complicaed calculaions. n able a compaison beween REFERENCE [] Bown M., Powe upply Cookbook, econd Ediion, Elsevie, xfod, UK,. [] Eickson R. W.,. Maksimovic, Fundamenals of Powe Eleconics, econd Ediion, Kluwe Academic Publishes Goup,. [3] Jankovskis J.,. epins, N. Ponomaenko, Effecs of pead pecum on upu File of Buck Convee, cienific Jounal Eleconics and Elecical Engineeing, Vol. 9, No 5, 3, Kaunas, Lihuania, pp [4] Kazimieczuk M. K. and. Czakowski, Resonan Powe Convees, EEE Pess and John Wiley & ons, New Yok, NY nd Ediion, pp. -595, BN ,. [5] Kazimieczuk M. K., Pulse-Widh Modulaed C-C Powe Convees, John Wiley & ons, New Yok, NY, 8, pp. -78, BN-: , BN-3: [6] Kizhanovski V. G.,. V. Chenov, and M. K. Kazimieczuk, Low-volage eleconic ballas based on Class E oscillao, EEE Tans. Powe Eleconics, vol., no. 3, pp , May 7. [7] Lunca E., A. alceanu, Viual nsumenaion Appoach fo Teaching EMC Conceps, cienific Jounal Eleconics and Elecical Engineeing, Vol. 7, No,, Kaunas, Lihuania, pp [8] Mask R., emysifying wiching Powe upplies, Elsevie, xfod, UK, 5. [9] Mohan, Ned; Undeland, Toe M.; Robbins, William P., Powe Eleconics - Convees, Applicaions, and esign (3d Ediion), 3 John Wiley & ons. [] Rashid M. H., Powe Eleconics handbook: devices, cicuis, and applicaions, Academic Pess, 7. [] Rashid M. H., Powe Eleconics: Cicuis, evices and Applicaions, Peason/Penice Hall, 3. [] epins., J. Jankovskis, udy of Fequency Modulaed Boos Convee peaing in isconinuous Conducion Mode, cienific Jounal Eleconics and Elecical Engineeing, Vol., No 6,, Kaunas, Lihuania, pp [3] Zinoviev G., Fundamenals of Powe Eleconics - pa, Novosibisk ae Univesiy, Novosibisk, Russia, 4, (in Russian).

Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch

Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch Two-dimensional Effecs on he CS Ineacion Foces fo an Enegy-Chiped Bunch ui Li, J. Bisognano,. Legg, and. Bosch Ouline 1. Inoducion 2. Pevious 1D and 2D esuls fo Effecive CS Foce 3. Bunch Disibuion Vaiaion

More information

Non-sinusoidal Signal Generators

Non-sinusoidal Signal Generators Non-sinusoidal Signal Geneaos ecangle, iangle, saw ooh, pulse, ec. Muliibao cicuis: asable no sable saes (wo quasi-sable saes; i emains in each sae fo pedeemined imes) monosable one sable sae, one unsable

More information

Lecture 17: Kinetics of Phase Growth in a Two-component System:

Lecture 17: Kinetics of Phase Growth in a Two-component System: Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien

More information

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as

More information

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion

More information

Lecture 22 Electromagnetic Waves

Lecture 22 Electromagnetic Waves Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should

More information

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,

More information

Research on the Algorithm of Evaluating and Analyzing Stationary Operational Availability Based on Mission Requirement

Research on the Algorithm of Evaluating and Analyzing Stationary Operational Availability Based on Mission Requirement Reseach on he Algoihm of Evaluaing and Analyzing Saionay Opeaional Availabiliy Based on ission Requiemen Wang Naichao, Jia Zhiyu, Wang Yan, ao Yilan, Depamen of Sysem Engineeing of Engineeing Technology,

More information

Computer Propagation Analysis Tools

Computer Propagation Analysis Tools Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion

More information

Low-complexity Algorithms for MIMO Multiplexing Systems

Low-complexity Algorithms for MIMO Multiplexing Systems Low-complexiy Algoihms fo MIMO Muliplexing Sysems Ouline Inoducion QRD-M M algoihm Algoihm I: : o educe he numbe of suviving pahs. Algoihm II: : o educe he numbe of candidaes fo each ansmied signal. :

More information

A Novel Resonant LLC Soft-Switching Buck Converter

A Novel Resonant LLC Soft-Switching Buck Converter Novel Resonan C Sof-Swiching Buck Convee Masoud Jabbai Elecical Engineeing Depaen, Najafabad Banch, slaic zad Univesiy sfahan, an Masuod.jabbai@gail.co Habib Kazei Elecical Engineeing Depaen, Najafabad

More information

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION Inenaional Jounal of Science, Technology & Managemen Volume No 04, Special Issue No. 0, Mach 205 ISSN (online): 2394-537 STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE

More information

An Automatic Door Sensor Using Image Processing

An Automatic Door Sensor Using Image Processing An Auomaic Doo Senso Using Image Pocessing Depamen o Elecical and Eleconic Engineeing Faculy o Engineeing Tooi Univesiy MENDEL 2004 -Insiue o Auomaion and Compue Science- in BRNO CZECH REPUBLIC 1. Inoducion

More information

On Control Problem Described by Infinite System of First-Order Differential Equations

On Control Problem Described by Infinite System of First-Order Differential Equations Ausalian Jounal of Basic and Applied Sciences 5(): 736-74 ISS 99-878 On Conol Poblem Descibed by Infinie Sysem of Fis-Ode Diffeenial Equaions Gafujan Ibagimov and Abbas Badaaya J'afau Insiue fo Mahemaical

More information

works must be obtained from the IEEE.

works must be obtained from the IEEE. NAOSTE: Nagasaki Univesiy's Ac Tile Auho(s) Opeaion chaaceisics impoveme hal-wave eciie sel exciaion Hiayama, Taashi; Higuchi, Tsuyosh Ciaion CEMS 7, pp.8-8 ssue Dae 7- URL Righ hp://hl.hanle.ne/69/6 (c)7

More information

An Open cycle and Closed cycle Gas Turbine Engines. Methods to improve the performance of simple gas turbine plants

An Open cycle and Closed cycle Gas Turbine Engines. Methods to improve the performance of simple gas turbine plants An Open cycle and losed cycle Gas ubine Engines Mehods o impove he pefomance of simple gas ubine plans I egeneaive Gas ubine ycle: he empeaue of he exhaus gases in a simple gas ubine is highe han he empeaue

More information

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy

More information

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security 1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,

More information

Servomechanism Design

Servomechanism Design Sevomechanism Design Sevomechanism (sevo-sysem) is a conol sysem in which he efeence () (age, Se poin) changes as ime passes. Design mehods PID Conol u () Ke P () + K I ed () + KDe () Sae Feedback u()

More information

DESIGN AND IMPLEMENTATION OF A DIGITALLY-CONTROLLED PHASE-SHIFT FULL-BRIDGE CONVERTER WITH OUTPUT SYNCHRONOUS RECTIFIER AND CURRENT DOUBLER

DESIGN AND IMPLEMENTATION OF A DIGITALLY-CONTROLLED PHASE-SHIFT FULL-BRIDGE CONVERTER WITH OUTPUT SYNCHRONOUS RECTIFIER AND CURRENT DOUBLER 83 Jounal of Technology, Vol. 3, o. 4, pp. 83-97 (17) DESIG AD IMPLEMETATIO OF A DIGITALLY-COTROLLED PHASE-SHIFT FULL-BRIDGE COVERTER WITH OUTPUT SYCHROOUS RECTIFIER AD CURRET DOUBLER Shun-Chung Wang 1,

More information

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission

More information

Design Considerations for Achieving ZVS in a Half Bridge Inverter that Drives a Piezoelectric Transformer with No Series Inductor

Design Considerations for Achieving ZVS in a Half Bridge Inverter that Drives a Piezoelectric Transformer with No Series Inductor Design onsideaions fo Achievg ZS a Half Bidge Invee ha Dives a iezoelecic Tansfoe wih No Seies Induco Svelana Bonse and Sa Ben-Yaaov* owe Eleconics aboaoy Depaen of Elecical and opue Engeeg Ben-Guion Univesiy

More information

Chapter 2: Principles of steady-state converter analysis

Chapter 2: Principles of steady-state converter analysis Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance, capacior charge balance, and he small ripple approximaion 2.3. Boos converer example 2.4. Cuk converer

More information

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder#

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder# .#W.#Erickson# Deparmen#of#Elecrical,#Compuer,#and#Energy#Engineering# Universiy#of#Colorado,#Boulder# Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance,

More information

2.4 Cuk converter example

2.4 Cuk converter example 2.4 Cuk converer example C 1 Cuk converer, wih ideal swich i 1 i v 1 2 1 2 C 2 v 2 Cuk converer: pracical realizaion using MOSFET and diode C 1 i 1 i v 1 2 Q 1 D 1 C 2 v 2 28 Analysis sraegy This converer

More information

The Production of Polarization

The Production of Polarization Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview

More information

PHYS PRACTICE EXAM 2

PHYS PRACTICE EXAM 2 PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,

More information

KINEMATICS OF RIGID BODIES

KINEMATICS OF RIGID BODIES KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid

More information

A Weighted Moving Average Process for Forecasting. Shou Hsing Shih Chris P. Tsokos

A Weighted Moving Average Process for Forecasting. Shou Hsing Shih Chris P. Tsokos A Weighed Moving Aveage Pocess fo Foecasing Shou Hsing Shih Chis P. Tsokos Depamen of Mahemaics and Saisics Univesiy of Souh Floida, USA Absac The objec of he pesen sudy is o popose a foecasing model fo

More information

Circuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt.

Circuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt. 4/08/00 eview Fomul s icuis cice s BL B A B I I I I E...... s n n hging Q Q 0 e... n... Q Q n 0 e Q I I0e Dischging Q U Q A wie mde of bss nd nohe wie mde of silve hve he sme lengh, bu he dimee of he bss

More information

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias

More information

4. Fundamental of A.C. Circuit

4. Fundamental of A.C. Circuit 4. Fundaenal of A.. icui 4. Equaion fo geneaion of alenaing induce EMF An A geneao uses he pinciple of Faaday s elecoagneic inducion law. saes ha when cuen caying conduco cu he agneic field hen ef induced

More information

RC, RL and RLC circuits

RC, RL and RLC circuits Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.

More information

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard Complex Analysis R.G. Halbud R.Halbud@ucl.ac.uk Depamen of Mahemaics Univesiy College London 202 The shoes pah beween wo uhs in he eal domain passes hough he complex domain. J. Hadamad Chape The fis fundamenal

More information

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay)

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay) Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens

More information

The k-filtering Applied to Wave Electric and Magnetic Field Measurements from Cluster

The k-filtering Applied to Wave Electric and Magnetic Field Measurements from Cluster The -fileing pplied o Wave lecic and Magneic Field Measuemens fom Cluse Jean-Louis PINÇON and ndes TJULIN LPC-CNRS 3 av. de la Recheche Scienifique 4507 Oléans Fance jlpincon@cns-oleans.f OUTLINS The -fileing

More information

Chapter 7. Interference

Chapter 7. Interference Chape 7 Inefeence Pa I Geneal Consideaions Pinciple of Supeposiion Pinciple of Supeposiion When wo o moe opical waves mee in he same locaion, hey follow supeposiion pinciple Mos opical sensos deec opical

More information

Discretization of Fractional Order Differentiator and Integrator with Different Fractional Orders

Discretization of Fractional Order Differentiator and Integrator with Different Fractional Orders Inelligen Conol and Auomaion, 207, 8, 75-85 hp://www.scip.og/jounal/ica ISSN Online: 253-066 ISSN Pin: 253-0653 Disceizaion of Facional Ode Diffeeniao and Inegao wih Diffeen Facional Odes Qi Zhang, Baoye

More information

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes]

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes] ENGI 44 Avance alculus fo Engineeing Faculy of Engineeing an Applie cience Poblem e 9 oluions [Theoems of Gauss an okes]. A fla aea A is boune by he iangle whose veices ae he poins P(,, ), Q(,, ) an R(,,

More information

L1, L2, N1 N2. + Vout. C out. Figure 2.1.1: Flyback converter

L1, L2, N1 N2. + Vout. C out. Figure 2.1.1: Flyback converter page 11 Flyback converer The Flyback converer belongs o he primary swiched converer family, which means here is isolaion beween in and oupu. Flyback converers are used in nearly all mains supplied elecronic

More information

Low-pass filter for UWB system with the circuit for compensation of process induced on-chip capacitor variation

Low-pass filter for UWB system with the circuit for compensation of process induced on-chip capacitor variation Oiginal scienific pape Low-pass file fo UB sysem wih he cicui fo compensaion of pocess induced on-chip capacio vaiaion Banislava Milinković,, Milenko Milićević,, Đođe imić, Goan ojanović, Radivoje Đuić

More information

Voltage Sag-Swell and Harmonics Analysis of UPQC Control Based DFIG- Wind Integration

Voltage Sag-Swell and Harmonics Analysis of UPQC Control Based DFIG- Wind Integration Inenaional Jounal of Engineeing Tends and Technology (IJETT Volume 56 Numbe 1 - Febuay 2018 Volage Sag-Swell and Hamonics Analysis of UPQC Conol Based DFIG- Wind Inegaion Sauabh Gupa #1, S.C. Choube 2,

More information

V L. DT s D T s t. Figure 1: Buck-boost converter: inductor current i(t) in the continuous conduction mode.

V L. DT s D T s t. Figure 1: Buck-boost converter: inductor current i(t) in the continuous conduction mode. ECE 445 Analysis and Design of Power Elecronic Circuis Problem Se 7 Soluions Problem PS7.1 Erickson, Problem 5.1 Soluion (a) Firs, recall he operaion of he buck-boos converer in he coninuous conducion

More information

IMPROVED DESIGN EQUATIONS FOR ASYMMETRIC COPLANAR STRIP FOLDED DIPOLES ON A DIELECTRIC SLAB

IMPROVED DESIGN EQUATIONS FOR ASYMMETRIC COPLANAR STRIP FOLDED DIPOLES ON A DIELECTRIC SLAB IMPROVED DESIGN EQUATIONS FOR ASYMMETRIC COPLANAR STRIP FOLDED DIPOLES ON A DIELECTRIC SLAB H.J. Visse* * Hols Cene TNO P.O. Bo 855 565 N Eindhoven, The Nehelands E-mail: hui.j.visse@no.nl eywods: Coupled

More information

On The Estimation of Two Missing Values in Randomized Complete Block Designs

On The Estimation of Two Missing Values in Randomized Complete Block Designs Mahemaical Theoy and Modeling ISSN 45804 (Pape ISSN 505 (Online Vol.6, No.7, 06 www.iise.og On The Esimaion of Two Missing Values in Randomized Complee Bloc Designs EFFANGA, EFFANGA OKON AND BASSE, E.

More information

Monochromatic Wave over One and Two Bars

Monochromatic Wave over One and Two Bars Applied Mahemaical Sciences, Vol. 8, 204, no. 6, 307-3025 HIKARI Ld, www.m-hikai.com hp://dx.doi.og/0.2988/ams.204.44245 Monochomaic Wave ove One and Two Bas L.H. Wiyano Faculy of Mahemaics and Naual Sciences,

More information

Orthotropic Materials

Orthotropic Materials Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε

More information

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2  P 1 =  #P L L, Lecue 36 Pipe Flow and Low-eynolds numbe hydodynamics 36.1 eading fo Lecues 34-35: PKT Chape 12. Will y fo Monday?: new daa shee and daf fomula shee fo final exam. Ou saing poin fo hydodynamics ae wo equaions:

More information

Control Volume Derivation

Control Volume Derivation School of eospace Engineeing Conol Volume -1 Copyigh 1 by Jey M. Seizman. ll ighs esee. Conol Volume Deiaion How o cone ou elaionships fo a close sysem (conol mass) o an open sysem (conol olume) Fo mass

More information

EE 301 Lab 2 Convolution

EE 301 Lab 2 Convolution EE 301 Lab 2 Convoluion 1 Inroducion In his lab we will gain some more experience wih he convoluion inegral and creae a scrip ha shows he graphical mehod of convoluion. 2 Wha you will learn This lab will

More information

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba THE INTEACTION OF ADIATION AND MATTE: SEMICLASSICAL THEOY PAGE 26 III. EVIEW OF BASIC QUANTUM MECHANICS : TWO -LEVEL QUANTUM SYSTEMS : The lieaue of quanum opics and lase specoscop abounds wih discussions

More information

On Energy-Efficient Node Deployment in Wireless Sesnor Networks

On Energy-Efficient Node Deployment in Wireless Sesnor Networks I J Communicaions, Newok and Sysem Sciences, 008, 3, 07-83 Published Online Augus 008 in Scies (hp://wwwscipog/jounal/ijcns/) On Enegy-Efficien Node Deploymen in Wieless Sesno Newoks Hui WANG 1, KeZhong

More information

A Study on Non-Binary Turbo Codes

A Study on Non-Binary Turbo Codes A Sudy on Non-Binay Tubo Codes Hoia BALTA, Maia KOVACI Univesiy Polyechnic of Timişoaa, Faculy of Eleconics and Telecommunicaions, Posal Addess, 3223 Timişoaa, ROMANIA, E-Mail: hoia.bala@ec.u.o, maia.kovaci@ec.u.o

More information

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens

More information

Chapter 7 Response of First-order RL and RC Circuits

Chapter 7 Response of First-order RL and RC Circuits Chaper 7 Response of Firs-order RL and RC Circuis 7.- The Naural Response of RL and RC Circuis 7.3 The Sep Response of RL and RC Circuis 7.4 A General Soluion for Sep and Naural Responses 7.5 Sequenial

More information

MIMO Cognitive Radio Capacity in. Flat Fading Channel. Mohan Premkumar, Muthappa Perumal Chitra. 1. Introduction

MIMO Cognitive Radio Capacity in. Flat Fading Channel. Mohan Premkumar, Muthappa Perumal Chitra. 1. Introduction Inenaional Jounal of Wieless Communicaions, ewoking and Mobile Compuing 07; 4(6): 44-50 hp://www.aasci.og/jounal/wcnmc ISS: 38-37 (Pin); ISS: 38-45 (Online) MIMO Cogniive adio Capaciy in Fla Fading Channel

More information

ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS

ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS Mem. Fac. Inegaed As and Sci., Hioshima Univ., Se. IV, Vol. 8 9-33, Dec. 00 ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS YOSHIO AGAOKA *, BYUNG HAK KIM ** AND JIN HYUK CHOI ** *Depamen of Mahemaics, Faculy

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

Lab 10: RC, RL, and RLC Circuits

Lab 10: RC, RL, and RLC Circuits Lab 10: RC, RL, and RLC Circuis In his experimen, we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors. We will sudy he way volages and currens change in

More information

Fig. 1S. The antenna construction: (a) main geometrical parameters, (b) the wire support pillar and (c) the console link between wire and coaxial

Fig. 1S. The antenna construction: (a) main geometrical parameters, (b) the wire support pillar and (c) the console link between wire and coaxial a b c Fig. S. The anenna consucion: (a) ain geoeical paaees, (b) he wie suppo pilla and (c) he console link beween wie and coaial pobe. Fig. S. The anenna coss-secion in he y-z plane. Accoding o [], he

More information

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid

More information

Prerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) , PART A PHYSICS

Prerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) ,  PART A PHYSICS Pena Towe, oad No, Conacos Aea, isupu, Jamshedpu 83, Tel (657)89, www.penaclasses.com AIEEE PAT A PHYSICS Physics. Two elecic bulbs maked 5 W V and W V ae conneced in seies o a 44 V supply. () W () 5 W

More information

Voltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response

Voltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response Review Capaciors/Inducors Volage/curren relaionship Sored Energy s Order Circuis RL / RC circuis Seady Sae / Transien response Naural / Sep response EE4 Summer 5: Lecure 5 Insrucor: Ocavian Florescu Lecure

More information

156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2

156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2 156 Thee ae 9 books sacked on a shelf. The hickness of each book is eihe 1 inch o 2 F inches. The heigh of he sack of 9 books is 14 inches. Which sysem of equaions can be used o deemine x, he numbe of

More information

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can. 1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule

More information

(b) (a) (d) (c) (e) Figure 10-N1. (f) Solution:

(b) (a) (d) (c) (e) Figure 10-N1. (f) Solution: Example: The inpu o each of he circuis shown in Figure 10-N1 is he volage source volage. The oupu of each circui is he curren i( ). Deermine he oupu of each of he circuis. (a) (b) (c) (d) (e) Figure 10-N1

More information

A note on characterization related to distributional properties of random translation, contraction and dilation of generalized order statistics

A note on characterization related to distributional properties of random translation, contraction and dilation of generalized order statistics PobSa Foum, Volume 6, July 213, Pages 35 41 ISSN 974-3235 PobSa Foum is an e-jounal. Fo eails please visi www.pobsa.og.in A noe on chaaceizaion elae o isibuional popeies of anom anslaion, conacion an ilaion

More information

Reinforcement learning

Reinforcement learning Lecue 3 Reinfocemen leaning Milos Hauskech milos@cs.pi.edu 539 Senno Squae Reinfocemen leaning We wan o lean he conol policy: : X A We see examples of x (bu oupus a ae no given) Insead of a we ge a feedback

More information

The problem with linear regulators

The problem with linear regulators he problem wih linear regulaors i in P in = i in V REF R a i ref i q i C v CE P o = i o i B ie P = v i o o in R 1 R 2 i o i f η = P o P in iref is small ( 0). iq (quiescen curren) is small (probably).

More information

A FAMILY OF THREE-LEVEL DC-DC CONVERTERS

A FAMILY OF THREE-LEVEL DC-DC CONVERTERS A FAMIY OF THREE-EVE DC-DC CONVERTERS Anonio José Beno Boion, Ivo Barbi Federal Universiy of Sana Caarina - UFSC, Power Elecronics Insiue - INEP PO box 5119, ZIP code 88040-970, Florianópolis, SC, BRAZI

More information

Effect of Wall Absorption on dispersion of a solute in a Herschel Bulkley Fluid through an annulus

Effect of Wall Absorption on dispersion of a solute in a Herschel Bulkley Fluid through an annulus Available online a www.pelagiaeseachlibay.com Advances in Applied Science Reseach,, 3 (6):3878-3889 ISSN: 976-86 CODEN (USA): AASRFC Effec of Wall Absopion on dispesion of a solue in a Heschel Bulley Fluid

More information

An Electrostatic Analogue for the Novel Temporary Magnetic Remanence Thermodynamic Cycles

An Electrostatic Analogue for the Novel Temporary Magnetic Remanence Thermodynamic Cycles -1- An Elecosaic Analogue fo he Novel Tempoay Magneic emanence Themodynamic Cycles Absac emi Conwall Fuue Enegy eseach Goup Queen May, Univesiy of London, Mile End oad, London E1 4NS hp://webspace.qmul.ac.uk/oconwall

More information

FINITE DIFFERENCE APPROACH TO WAVE GUIDE MODES COMPUTATION

FINITE DIFFERENCE APPROACH TO WAVE GUIDE MODES COMPUTATION FINITE DIFFERENCE ROCH TO WVE GUIDE MODES COMUTTION Ing.lessando Fani Elecomagneic Gou Deamen of Elecical and Eleconic Engineeing Univesiy of Cagliai iazza d mi, 93 Cagliai, Ialy SUMMRY Inoducion Finie

More information

Topic Astable Circuits. Recall that an astable circuit has two unstable states;

Topic Astable Circuits. Recall that an astable circuit has two unstable states; Topic 2.2. Asable Circuis. Learning Objecives: A he end o his opic you will be able o; Recall ha an asable circui has wo unsable saes; Explain he operaion o a circui based on a Schmi inverer, and esimae

More information

Risk tolerance and optimal portfolio choice

Risk tolerance and optimal portfolio choice Risk oleance and opimal pofolio choice Maek Musiela BNP Paibas London Copoae and Invesmen Join wok wih T. Zaiphopoulou (UT usin) Invesmens and fowad uiliies Pepin 6 Backwad and fowad dynamic uiliies and

More information

Sharif University of Technology - CEDRA By: Professor Ali Meghdari

Sharif University of Technology - CEDRA By: Professor Ali Meghdari Shaif Univesiy of echnology - CEDRA By: Pofesso Ali Meghai Pupose: o exen he Enegy appoach in eiving euaions of oion i.e. Lagange s Meho fo Mechanical Syses. opics: Genealize Cooinaes Lagangian Euaion

More information

Pseudosteady-State Flow Relations for a Radial System from Department of Petroleum Engineering Course Notes (1997)

Pseudosteady-State Flow Relations for a Radial System from Department of Petroleum Engineering Course Notes (1997) Pseudoseady-Sae Flow Relaions fo a Radial Sysem fom Deamen of Peoleum Engineeing Couse Noes (1997) (Deivaion of he Pseudoseady-Sae Flow Relaions fo a Radial Sysem) (Deivaion of he Pseudoseady-Sae Flow

More information

MECHANICS OF MATERIALS Poisson s Ratio

MECHANICS OF MATERIALS Poisson s Ratio Fouh diion MCHANICS OF MATRIALS Poisson s Raio Bee Johnson DeWolf Fo a slende ba subjeced o aial loading: 0 The elongaion in he -diecion is accompanied b a conacion in he ohe diecions. Assuming ha he maeial

More information

Chapter 4 DC converter and DC switch

Chapter 4 DC converter and DC switch haper 4 D converer and D swich 4.1 Applicaion - Assumpion Applicaion: D swich: Replace mechanic swiches D converer: in racion drives Assumions: Ideal D sources Ideal Power emiconducor Devices 4.2 D swich

More information

International Journal of Pure and Applied Sciences and Technology

International Journal of Pure and Applied Sciences and Technology In. J. Pue Appl. Sci. Technol., 4 (211, pp. 23-29 Inenaional Jounal of Pue and Applied Sciences and Technology ISS 2229-617 Available online a www.ijopaasa.in eseach Pape Opizaion of he Uiliy of a Sucual

More information

Physics 2001/2051 Moments of Inertia Experiment 1

Physics 2001/2051 Moments of Inertia Experiment 1 Physics 001/051 Momens o Ineia Expeimen 1 Pelab 1 Read he ollowing backgound/seup and ensue you ae amilia wih he heoy equied o he expeimen. Please also ill in he missing equaions 5, 7 and 9. Backgound/Seup

More information

ECE 2100 Circuit Analysis

ECE 2100 Circuit Analysis ECE 1 Circui Analysis Lesson 35 Chaper 8: Second Order Circuis Daniel M. Liynski, Ph.D. ECE 1 Circui Analysis Lesson 3-34 Chaper 7: Firs Order Circuis (Naural response RC & RL circuis, Singulariy funcions,

More information

A Numerical Hydration Model of Portland Cement

A Numerical Hydration Model of Portland Cement A Numeical Hydaion Model of Poland Cemen Ippei Mauyama, Tesuo Masushia and Takafumi Noguchi ABSTRACT : A compue-based numeical model is pesened, wih which hydaion and micosucual developmen in Poland cemen-based

More information

Chapter 5: Discontinuous conduction mode. Introduction to Discontinuous Conduction Mode (DCM)

Chapter 5: Discontinuous conduction mode. Introduction to Discontinuous Conduction Mode (DCM) haper 5. The isconinuous onducion Mode 5.. Origin of he disconinuous conducion mode, and mode boundary 5.. Analysis of he conversion raio M(,K) 5.3. Boos converer example 5.4. Summary of resuls and key

More information

(a) Unde zeo-bias conditions, thee ae no lled states on one side of the junction which ae at the same enegy as the empty allowed states on the othe si

(a) Unde zeo-bias conditions, thee ae no lled states on one side of the junction which ae at the same enegy as the empty allowed states on the othe si 1 Esaki Diode hen the concentation of impuity atoms in a pn-diode is vey high, the depletion laye width is educed to about 1 nm. Classically, a caie must have an enegy at least equal to the potential-baie

More information

Silicon Controlled Rectifiers UNIT-1

Silicon Controlled Rectifiers UNIT-1 Silicon Conrolled Recifiers UNIT-1 Silicon Conrolled Recifier A Silicon Conrolled Recifier (or Semiconducor Conrolled Recifier) is a four layer solid sae device ha conrols curren flow The name silicon

More information

Projection of geometric models

Projection of geometric models ojecion of geomeic moels Eie: Yeh-Liang Hsu (998-9-2); ecommene: Yeh-Liang Hsu (2-9-26); las upae: Yeh-Liang Hsu (29--3). Noe: This is he couse maeial fo ME55 Geomeic moeling an compue gaphics, Yuan Ze

More information

Range Migration Techniques for Short-Range MIMO Array Imaging

Range Migration Techniques for Short-Range MIMO Array Imaging Pogess In Elecomagneics Reseach Lees, Vol. 64, 111 117, 2016 Range Migaion Techniques fo Sho-Range MIMO Aay Imaging Jing Yang, Xiaozhou Shang, and Zhi-Ping Li * Absac This pape pesens a sho-ange imaging

More information

EFFECT OF PERMISSIBLE DELAY ON TWO-WAREHOUSE INVENTORY MODEL FOR DETERIORATING ITEMS WITH SHORTAGES

EFFECT OF PERMISSIBLE DELAY ON TWO-WAREHOUSE INVENTORY MODEL FOR DETERIORATING ITEMS WITH SHORTAGES Volume, ssue 3, Mach 03 SSN 39-4847 EFFEC OF PERMSSBLE DELAY ON WO-WAREHOUSE NVENORY MODEL FOR DEERORANG EMS WH SHORAGES D. Ajay Singh Yadav, Ms. Anupam Swami Assisan Pofesso, Depamen of Mahemaics, SRM

More information

Investigation of Flexible Multi-Mode Harmonic Vibration for the Automatic Washing Process

Investigation of Flexible Multi-Mode Harmonic Vibration for the Automatic Washing Process Inesigaion of Flexible Muli-Mode Hamonic Vibaion fo he Auomaic Washing Pocess JIAN-LONG KUO a, TSUNG-YU WANG b, a Depamen of Mechanical and Auomaion Engineeing, Naional Kaohsiung Fis Uniesiy of Science

More information

Homework-8(1) P8.3-1, 3, 8, 10, 17, 21, 24, 28,29 P8.4-1, 2, 5

Homework-8(1) P8.3-1, 3, 8, 10, 17, 21, 24, 28,29 P8.4-1, 2, 5 Homework-8() P8.3-, 3, 8, 0, 7, 2, 24, 28,29 P8.4-, 2, 5 Secion 8.3: The Response of a Firs Order Circui o a Consan Inpu P 8.3- The circui shown in Figure P 8.3- is a seady sae before he swich closes a

More information

6.003 Homework #9 Solutions

6.003 Homework #9 Solutions 6.00 Homework #9 Soluions Problems. Fourier varieies a. Deermine he Fourier series coefficiens of he following signal, which is periodic in 0. x () 0 0 a 0 5 a k sin πk 5 sin πk 5 πk for k 0 a k 0 πk j

More information

The sudden release of a large amount of energy E into a background fluid of density

The sudden release of a large amount of energy E into a background fluid of density 10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy

More information

A DETAILED STUDY OF THE HIGH ORDER SERIAL RESONANT INVERTER FOR INDUCTION HEATING

A DETAILED STUDY OF THE HIGH ORDER SERIAL RESONANT INVERTER FOR INDUCTION HEATING ELECTRONICS 005 1 3 Septembe, Sozopol, BULGARIA A DETAILED STUDY OF THE HIGH ORDER SERIAL RESONANT INVERTER FOR INDUCTION HEATING Evgeniy Ivanov Popov, Liliya Ivanova Pindeva, Elisaveta Histova Mileva,

More information

PARAMETER IDENTIFICATION IN DYNAMIC ECONOMIC MODELS*

PARAMETER IDENTIFICATION IN DYNAMIC ECONOMIC MODELS* Aicles Auumn PARAMETER IDENTIFICATION IN DYNAMIC ECONOMIC MODELS Nikolay Iskev. INTRODUCTION Paamee idenifi caion is a concep which evey suden of economics leans in hei inoducoy economeics class. The usual

More information

Design Guideline for Buried Hume Pipe Subject to Coupling Forces

Design Guideline for Buried Hume Pipe Subject to Coupling Forces Design Guideline fo Buied Hume Pipe Sujec o Coupling Foces Won Pyo Hong 1), *Seongwon Hong 2), and Thomas Kang 3) 1) Depamen of Civil, nvionmenal and Plan ngineeing, Chang-Ang Univesiy, Seoul 06974, Koea

More information

Energy dispersion relation for negative refraction (NR) materials

Energy dispersion relation for negative refraction (NR) materials Enegy dispesion elaion fo negaive efacion (NR) maeials Y.Ben-Ayeh Physics Depamen, Technion Isael of Technology, Haifa 3, Isael E-mail addess: ph65yb@physics.echnion,ac.il; Fax:97 4 895755 Keywods: Negaive-efacion,

More information

6.003 Homework #9 Solutions

6.003 Homework #9 Solutions 6.003 Homework #9 Soluions Problems. Fourier varieies a. Deermine he Fourier series coefficiens of he following signal, which is periodic in 0. x () 0 3 0 a 0 5 a k a k 0 πk j3 e 0 e j πk 0 jπk πk e 0

More information

More Digital Logic. t p output. Low-to-high and high-to-low transitions could have different t p. V in (t)

More Digital Logic. t p output. Low-to-high and high-to-low transitions could have different t p. V in (t) EECS 4 Spring 23 Lecure 2 EECS 4 Spring 23 Lecure 2 More igial Logic Gae delay and signal propagaion Clocked circui elemens (flip-flop) Wriing a word o memory Simplifying digial circuis: Karnaugh maps

More information

Kalman Filter: an instance of Bayes Filter. Kalman Filter: an instance of Bayes Filter. Kalman Filter. Linear dynamics with Gaussian noise

Kalman Filter: an instance of Bayes Filter. Kalman Filter: an instance of Bayes Filter. Kalman Filter. Linear dynamics with Gaussian noise COM47 Inoducion o Roboics and Inelligen ysems he alman File alman File: an insance of Bayes File alman File: an insance of Bayes File Linea dynamics wih Gaussian noise alman File Linea dynamics wih Gaussian

More information