Nicola Tesla UNPLUGGED OBJECTIVE

Size: px
Start display at page:

Download "Nicola Tesla UNPLUGGED OBJECTIVE"

Transcription

1 Wireless Energy Transmission Nicola Tesla UNPLUGGED by Nick Simos Ph.D. P.E. Senior Scienis Brookhaven Naional Laboraory OBJECTIVE By saying wihin he framework of he acceped governing physics laws: Aemp o arrive o an undersanding of how Tesla conceived and planned WIRELESS Energy Transmission a his Shoreham Experimenal Saion In paricular ry o undersand he Principles & his Mehods The objecive is NOT o prove or disprove his ideas BUT raher o undersand wha he was afer Aim is o seer clear from convolued conceps which afer all have hur raher han helped N. Tesla s scienific conribuions and repuaion 1

2 Resonance... and N.TESLA a cornersone of his work Heraclius: τα παντα ρει... or everyhing is in moion and Tesla undersood ha everyhing oscillaes earh fields elecric mechanical ec. Finally N. Tesla in he company of pioneers and immoral scieniss Gerhard Krisensson 01 Lund January 30 01

3 Some Background Maxwell Equaions... and TESLA While hese form he basis of our undersanding of elecromagneism we also accep ha inconsisencies boh mahemaical and physical MAY EXIST in hem Semming from Abrup changes or DISCONTINUITIES no everyhing is smooh In an effor o undersand wha Tesla had in mind resoring o some mahemaical formulaions and Maxwell Equaion soluions will unavoidable Kep o a minimum bu necessary as a maer of record In all we will NOT DEVIATE from he Maxwell Equaions Domain no new physics Try o explain everyhing saring every ime from he universally acceped Maxwell governing relaions Maxwell Equaions...? Wha are hey? 3

4 Maxwell s Equaions: Ingenious way of explaining he connecion beween elecric and magneic fields elecric field E and magneic field B B E = μ Faraday' s Law E B = J + ε Ampere Law ρν E = Gauss Law ε B = 0 Gauss Law magneism ρ v is volume elecric charge densiy J is he elecric curren densiy ε is he permiiviy and μ is he permeabiliy All is smooh and easy UNTIL one ges close o abrup elecric and magneic sources Classical Maxwell equaions are supposed o be saisfied poin-wise a any insan of ime. Therefore disconinuous or diverging soluions are no allowed BUT.. When elecromagneic fields vary wih ime we can re-arrange and decouple hese relaions and express hem in forms ha describe propagaion of waves E r 1 J ΔE r εμ = ρ r + μ r ε B r ΔB r εμ =μ J r Transverse waves Herz ype An anenna radiaes high frequency ransverse elecromagneic waves as shown Bu is i all Herz-ype?. No necessarily! Can oher ypes of waves be generaed and propagaed? Longiudinal waves? Tesla be on i will revisi he poin 4

5 To undersand how Tesla while remaining rue o he Maxwell governing principles concepualized and pursued his goals we need o go back and sar a Colorado Springs Tesla a Colorado Springs Pre-cursor o Wardenclyffe Wha did he do here? Wha did he observe? How relevan o his work in Wardenclyffe Shoreham? 5

6 Wha did he do here? A. Wirelessly ransmied elecric pulses o large disances B. Observed he undiminished reurn of an elecric pulse which he speculaed raveled o he anipode and back There has been speculaion ha wha Tesla did he excied was resonances of he Schumann Caviy bu did he? in his words: "This mode of conveying elecrical energy o a disance is no 'wireless' in he popular sense bu a ransmission hrough a conducor and one which is incomparably more perfec han any arificial one. All impedimens of conducion arise from confinemen of he elecric and magneic fluxes o narrow channels. The globe is free of such cramping and impedimens... Some Background on he Caviy Earh and Ionosphere boh conducing capacior-like or a caviy ha can resonae Pleny is happening in he space beween: Elecric field beween his spherical capacior exhibis characerisic modes when excied Elecrical discharges can excie hem lighning is a broadband or whie noise exciaion exciing all he modes in he caviy BUT why is i imporan? I proves ha cerain elecromagneic ypes EXIST i.e. longiudinal ELF and VLF waves Source: Wikipedia 6

7 Schumann Resonances Earh Breahing STANDING waves modes-like are formed in he caviy which funcions like a wave guide Solving he CLASSICAL Maxwell Equaions one can arrive a he conclusion ha boh Longiudinal and Transverse Modes or sanding waves are presen in he caviy Longiudinal ~ Caviy mean radius Transverse ~ Caviy heigh orders of magniude difference beween eigenfrequencies ELF Hz and VLF 0-10 khz waves or resonances develop. These are considered LONGITUDINAL Modes Lighning or man-made discharges can EXCITE hese modes and especially hose considered Exremely Low Frequency ELF including he 7.83 Hz mode Prof. O. Schumann around 195 mahemaically esimaed he 7.83 Hz mode ha was soon afer 1954 confirmed wih measuremens Bu wai a second.. 7

8 According o Wikipedia: The firs documened observaions of global elecromagneic resonance were made by Nikola Tesla a his Colorado Springs laboraory in The observaions led o cerain conclusions abou he elecrical properies of he Earh and which made he basis for his idea of wireless energy ransmission. Tesla researched ways o ransfer power wirelessly over long disances via ransverse and longiudinal waves ransmiing ELF hrough he earh and as well as beween he Earh s surface and he Kennelly-Heaviside layer sanding waves. Making calculaions based on he experimens Tesla discovered ha he resonan frequency of he Earh was ~8 Hz. In he 1950 s researchers confirmed ha he resonan frequency of he Earh s ionospheric caviy was in ha range laer named he Schumann resonance Quoe: Physicis Nikola Tesla back in 1890 s was FIRST o experimen wih he CAVITY powerful discharges emulaing lighning and exciing ELF waves based on which he discovered he resonance frequency of he earh a 8 Hz. Unforunaely Tesla was before his ime and his discoveries were no aken seriously Wireless Transmission wih Schumann Resonances? No quie FEASIBLE here is why: Spherical waves in Caviy or Modes Small Q-facor raio elecric field energy sored in caviy per cycle/average power inpu While Tesla undersood he Caviy effec and assessed is fundamenal resonance he did no ride hese resonances o wirelessly ransfer elecric pulses. So wha did Tesla excie a Colorado Springs? He disurbed he earh s elecric field or blanke wih exreme elecric discharges Elecrically excie receivers a grea disances Observed he undiminished elecric pulses reurn from anipode Deermined a DIFFERENT frequency no he 8 Hz Schumann fundamenal resonance which will guide his wireless ransmission conceps Deermined ha ime required for ransmied pulse o ravel o he anipode and back is seconds fundamenal earh resonance frequency of Hz Elecromagneic waves a hese frequencies!!! ELF & VLF shown in Schumann Caviy 8

9 Tesla quoing: Power would be ransmied by creaing "sanding waves" in he earh by charging he earh wih a gian elecrical oscillaor ha would make he earh vibrae elecrically in he same way a bell vibraes mechanically when i is sruck wih a hammer...." 9

10 Tesla a Shoreham Wireless power ransmission From Colorado Springs o Shoreham Fundamenal principles underlying Tesla's wireless energy ransmission: wha he couned on 1. Low frequency alernaing curren can be ransmied hrough he earh wih low loss ne resisance beween earh s anipodes <1 ohm. Low frequency high volage alernaing curren via elecric displacemens by a elecrosaic inducion b elecrical conducion or a combinaion of he wo 3. Earh s naurally exising elecrosaic poenial elecrosaic field V poenial wih ionosphere Downward direced E-field of abou 100 V/m near surface abiliy o creae disurbances in his charge as annular disorion of he background elecric field AIMED AT TWO Mehods or Circui Types namely OPEN CIRCUIT Earh Resonance CLOSED Circui Amospheric Conducion 10

11 How do his wo conceps work? CENTRAL o Tesla s conceps is he Capacior Principle He is envisioning however a capacior of enormous proporions In a ypical capacior energy indeed ransfers wirelessly across he wo plaes hrough he dielecric AC curren jumps he gap ha is beween 1/6-1/ wavelengh. Because AC frequencies are high wavelenghs are small so GAP is small In Tesla s model he wo disan elevaed erminals are elecrically coupled ogeher in a manner similar o he ransfer of elecrical energy beween wo closely spaced capacior plaes bu a disances grealy exceeding 1/6-1/ wavelengh His concep/model a firs glance considered o be inconsisen wih mainsream physics UNLESS differen ypes of waves beween he plaes can be excied!!!!! Need o have receiving capacior plae o resonae wih is counerpar Capacior plaes TESLA Coil and Sysem: Wha is i? A capacior and some oher suff!!! Medium beween Tesla coils or owers The wireless sysem is comprised of wo sympaheically uned elecrical oscillaors RF power supply conneced o a grounded op-loaded helical resonaor Disance apar many wavelengh's unlike capacior!!! Primary power in and secondary coils Primary coil conneced o power source Secondary pancake coil and connecor o capacior plae: high volage and seleced frequency harmonic of Hz Ionizaion of air beween capacior plaes: exciaion of LF longiudinal modes or waves 11

12 high-volage elevaed erminal Tesla s Earh RESONANCE Mehod 1

13 Open Circui working principle Earh Resonance Mehod A Tesla coil earh resonance ransmier creaes a local disurbance in he earh s charge He is now zooming-in o no simply excie he earh s elecric field wih a broadband source BUT wih a source ha operaes a some harmonic of he earh field-resonance ~11.78Hz Such source is he basis of Tesla's earh resonance mehod. The receiver from he wo Tesla coils is Passive Earh s elecric field resonance will provide he synchronizaion of he receiver!!! Recall ha Tesla esimaed ha he fundamenal earh resonance frequency is of he order Hz. Tha came from his Colorado Springs work! So here is he connecion! Governing Principles in Resonance Mehod Medium beween uning forks ransmier and receiver is AIR Sound compression waves propagae in he medium Medium beween similar coils ransmier and receiver? Types of waves i can suppor VLF ELF Longiudinal waves??? no Herzian debae Energy ransfers beween ransmier and receiver If he characerisic one of fork B is differen han A NOTHING happens!!! 13

14 How will Tesla s Resonance Sysem look like? Receiver will be uned ransmier and will be excied by he field disorion iself excied by he ransmier a he same frequency Same hing only elecrically Open Circui working principle Earh Resonance Mehod coninued Sysem MUST operae a some harmonic of he earh-resonance frequency ~11.78Hz Receiver waiing o be SYMPATHETICALLY acivaed once i does NEEDS o draw load ransfer of energy. Success of he mehod rides on he abiliy of he ransmier o excie and induce waves in he medium beween hem OTHER han of he Herz-ype Le s go back o Maxwell s Equaions and ake a closer look 14

15 Longiudinal and Transverse Waves START from he fac ha any vecor field finie uniform coninuous can spli ino longiudinal and ransverse fields F = F + F F F = 0 = 0 D = ρ r D = longiudinal elecric exciaion E = longiudinal elecric field Maxwell equaion for he long. par of elecric displacemen field Which afer some mahemaical manipulaions leads o: D r = E r = 1 4π 1 4πε r r' ρ r' r r' r r' ρ r' r r' 3 3 d r' 3 3 d r' Source: J. Nisch e al Equivalen Circui Mehod Longiudinal and Transverse Waves 1 r r' E r = r' 4 ρ πε r r' 3 d r 3 ' Above is an ineresing finding which says ha he longiudinal elecric displacemen D and elecric srengh E are fully coupled o he insananeous Coulomb charge!!! Or whaever he SOURCE is doing a r he field is doing a r : Tha is CRUCIAL!!!! E r ρ r' If he source is oscillaing wih a frequency f so will any poin on he domain receiver will oscillae sympaheically a he same frequency which is made o be idenical o ha of he ransmier 15

16 16 Parenhesis Aemp o see if he ypes of waves Tesla was couning on can be generaed 1 r J B r B r r J r E r E r = Δ + = Δ μ εμ μ ρ ε εμ Ineresing soluions due o charge/curren singulariies Consider one of he wave-like equaions z y x E r E r c = Δ τ ζ η δ ξ Laplace ransform on τ In 3-D space r c e E z y x c r re c s re s c r rr = = + /4 ; ; / / ] / [ π ζ η δ ξ r c c r E = ]/4 / [ π δ τ 0 1 { r c c E = τ π c r c r < > τ In -D space

17 Near-field a and wave-zone effecs Herzian Oscillaor Dipole Anenna A poin P wih a saionary posiive charge +e and an oscillaing negaive charge e abou P forming a dipole Herzian Oscillaor generae wha we know as Herzian waves The field produced omi derivaion from Maxwell s equaions E e f[ R1 p&& ] R1 r1 + 4π R 4 π c R = Near-field Wave-zone So even an oscillaing dipole induces a near field!!!! Le s revisi he soluion from a discharge ha Tesla was doing in Colorado Springs E=δ [ τ r/ c]/4π c r From singular discharge Radially expanding hin spherical shell E e f[ R1 p&& ] R1 r1 + 4π R 4 π c R = From oscillaing dipole Well wha is under debae is how far from he source inducing he elecromagneic waves he wo ypes separae I can be said ha i depends on he disurbance or source-ype 17

18 RECEIVER Responding INSTANTLY? I can only happen if he Transmier EXCITES a mode of he field sanding wave ONLY hen he field will be disurbed insanly!!! and Tesla AIMED a exacly ha: Hence RIDE he fundamenal mode of he earh elecric charge field OR a muliple harmonic of i Tesla s ATMOSPHERIC CONDUCTION Mehod Closed Circui Mehod 18

19 Amospheric Conducion elecrosaic inducion insead of rue conducion Elecrical displacemen or he passage of elecrical energy hrough space oher han he applicaion of volage poenial high volage and low curren Wha will he sysem look-like: ionosphere Tesla coil ransmier Ionized pah connecing he ransmier upper amosphere Ionosphere Ionized pah connecing he upper amosphere back down o receiving locaion Tesla Coil receiver Closed circui is compleed wih curren back o he ransmier hrough he earh high curren and low volage DETAILS of he Amospheric Conducion Mehod An oscillaing elecric field is induced by High Poenial RF curren applied o he HELICAL Resonaor of a Tesla coil oscillaing magneic field oscillaing elecric field A plasma sae is formed in he High Volage Terminal capacior plae making i conducive Curren is pushed in he o vols line creaed o he upper sraa high volage will minimize loss due o plasma ransmission-line resisance An ionizing beam of ulraviole radiaion will also form a high-volage plasma ransmission line If a plasma sae is induced in he upper roposphere par of he scheme hen ha becomes a conducor End resul is a flow of rue conducion currens beween ransmier and receiver The process relies on plasma waves developing in he ionized region beween he wo erminals elecrosaic waves or magneo-hydrodynamic waves Curren back hrough he earh One can see a purely conducion mehod and a hybrid one par conducive par inducive 19

20 Longiudinal Waves and Maxwell Equaions Elecrosaic or magneo-hydrodynamic plasma wave model Elecrosaic Waves K. T. McDonald An Elecrosaic Wave Asserion: A ime-varying purely ELECTRIC field Er can exis and propagae as a longiudinal wave WITHOUT coupling o a ime-varying magneic field B = Bu under he Condiions: Elecric Displacemen D is zero in a plasma medium0 These Longiudinal elecric waves can coexis wih background elecrosaic and magneo-saic fields i E = E xe ˆ x E = V Ex V = i e k ρ = P kxω i kxω E = B E = = 0 c P = volume densiy of elecric momens D = Elecric Displacemen of Long. Wave ρ = charge densiy Maxwell Equaions E = 4πρ E P = 4π Condiion : D = E + 4πP = 0 Furher analysis reveals ha he longiudinal waves can only have he plasma frequencies! We did observe he same in he separaion of ransverse and longiudinal waves of Maxwell s equaions So wha happens a he receiving end...? COUPLED Transmier and Receiver Transmier feels he load in he receiver ENERGY SUCKING ANTENNAS and TESLA Parallelism wih ATOMS 1 Am srongly ineracing wih LIGHT 5000 Am wavelengh Flood he amosphere wih sanding waves ionosphere keeps mos of his EM energy from escaping ino space hen a small resonaor can grab significan waage righ ou of he air effecive disk in figure hp://amasci.com/esla/escv.hml A small resonaor can produce an exensive and inense AC field of is own and can ac as an "EM funnel" simple deskop experimens demonsraed i!!! This is "circuiry" where wavelengh is huge and circuis are small As one said: This is probably he concep ha pu ha "Mona Lisa grin" on phoographs of old Nikola. And ha winkle in his eye... 0

21 How Feasible or Workable is Tesla s Conceps? Resonance or Open Circui Mehod: Tesla s model involves wo very disan elecrically coupled elevaed erminals capacior plaes in a manner similar o he ransfer of elecrical energy beween wo closely spaced capacior plaes in a ypical AC circui bu a disances grealy exceeding 1/6-1/ wavelengh This model considered o be inconsisen wih a basic ene of mainsream physics relaed o he scalar derivaives of he elecromagneic poenials So we hough BUT Wiriciy is proving o be oherwise MIT ess and Resonan Inducive Coupling disances > ¼ wavelengh maybe no he disances Tesla envisioned BUT much greaer han wha was hough as he hreshold of a capacior Amospheric Conducion or Closed Circui Mehod: Model has no inconsisencies I also involves wo very disan elecrically coupled elevaed erminals capacior plaes ha are boh acive and rely on in elecrosaic inducion alone I also involves he ionizaion of he space beween he wo capacior plaes which in urn being in a sae of plasma will permi ELF and VLF waves While consisen i may be impracical for is size. Maybe! 1

22 In his own words... Le he fuure ell he ruh and evaluae each one according o his work and accomplishmens. The presen is heirs; he fuure for which I have really worked is mine. Nikola Tesla I is possible hen ha our fuure already lies in our pas... all we need o do is coninue connecing he dos

23 Links and Resources TESLA Science Cener a Wardenclyffe Tesla Sociey of USA and Canada J. Nisch F. Gronwald G. Wollenberg Equivalen Circui Mehod Wiley 3

A1 K. 12V rms. 230V rms. 2 Full Wave Rectifier. Fig. 2.1: FWR with Transformer. Fig. 2.2: Transformer. Aim: To Design and setup a full wave rectifier.

A1 K. 12V rms. 230V rms. 2 Full Wave Rectifier. Fig. 2.1: FWR with Transformer. Fig. 2.2: Transformer. Aim: To Design and setup a full wave rectifier. 2 Full Wave Recifier Aim: To Design and seup a full wave recifier. Componens Required: Diode(1N4001)(4),Resisor 10k,Capacior 56uF,Breadboard,Power Supplies and CRO and ransformer 230V-12V RMS. + A1 K B1

More information

EE 330 Lecture 24. Amplification with Transistor Circuits Small Signal Modelling

EE 330 Lecture 24. Amplification with Transistor Circuits Small Signal Modelling EE 330 Lecure 24 Amplificaion wih Transisor Circuis Small Signal Modelling Review from las ime Area Comparison beween BJT and MOSFET BJT Area = 3600 l 2 n-channel MOSFET Area = 168 l 2 Area Raio = 21:1

More information

EXPERIMENT #4 AM MODULATOR AND POWER AMPLIFIER

EXPERIMENT #4 AM MODULATOR AND POWER AMPLIFIER EXPERIMENT #4 AM MODULATOR AND POWER AMPLIFIER INTRODUCTION: Being able o ransmi a radio frequency carrier across space is of no use unless we can place informaion or inelligence upon i. This las ransmier

More information

Investigation and Simulation Model Results of High Density Wireless Power Harvesting and Transfer Method

Investigation and Simulation Model Results of High Density Wireless Power Harvesting and Transfer Method Invesigaion and Simulaion Model Resuls of High Densiy Wireless Power Harvesing and Transfer Mehod Jaber A. Abu Qahouq, Senior Member, IEEE, and Zhigang Dang The Universiy of Alabama Deparmen of Elecrical

More information

THE OSCILLOSCOPE AND NOISE. Objectives:

THE OSCILLOSCOPE AND NOISE. Objectives: -26- Preparaory Quesions. Go o he Web page hp://www.ek.com/measuremen/app_noes/xyzs/ and read a leas he firs four subsecions of he secion on Trigger Conrols (which iself is a subsecion of he secion The

More information

4.5 Biasing in BJT Amplifier Circuits

4.5 Biasing in BJT Amplifier Circuits 4/5/011 secion 4_5 Biasing in MOS Amplifier Circuis 1/ 4.5 Biasing in BJT Amplifier Circuis eading Assignmen: 8086 Now le s examine how we C bias MOSFETs amplifiers! f we don bias properly, disorion can

More information

EXPERIMENT #9 FIBER OPTIC COMMUNICATIONS LINK

EXPERIMENT #9 FIBER OPTIC COMMUNICATIONS LINK EXPERIMENT #9 FIBER OPTIC COMMUNICATIONS LINK INTRODUCTION: Much of daa communicaions is concerned wih sending digial informaion hrough sysems ha normally only pass analog signals. A elephone line is such

More information

Lab 3 Acceleration. What You Need To Know: Physics 211 Lab

Lab 3 Acceleration. What You Need To Know: Physics 211 Lab b Lab 3 Acceleraion Wha You Need To Know: The Physics In he previous lab you learned ha he velociy of an objec can be deermined by finding he slope of he objec s posiion vs. ime graph. x v ave. = v ave.

More information

Experiment 6: Transmission Line Pulse Response

Experiment 6: Transmission Line Pulse Response Eperimen 6: Transmission Line Pulse Response Lossless Disribued Neworks When he ime required for a pulse signal o raverse a circui is on he order of he rise or fall ime of he pulse, i is no longer possible

More information

EE201 Circuit Theory I Fall

EE201 Circuit Theory I Fall EE1 Circui Theory I 17 Fall 1. Basic Conceps Chaper 1 of Nilsson - 3 Hrs. Inroducion, Curren and Volage, Power and Energy. Basic Laws Chaper &3 of Nilsson - 6 Hrs. Volage and Curren Sources, Ohm s Law,

More information

Table of Contents. 3.0 SMPS Topologies. For Further Research. 3.1 Basic Components. 3.2 Buck (Step Down) 3.3 Boost (Step Up) 3.4 Inverter (Buck/Boost)

Table of Contents. 3.0 SMPS Topologies. For Further Research. 3.1 Basic Components. 3.2 Buck (Step Down) 3.3 Boost (Step Up) 3.4 Inverter (Buck/Boost) Table of Conens 3.0 SMPS Topologies 3.1 Basic Componens 3.2 Buck (Sep Down) 3.3 Boos (Sep Up) 3.4 nverer (Buck/Boos) 3.5 Flyback Converer 3.6 Curren Boosed Boos 3.7 Curren Boosed Buck 3.8 Forward Converer

More information

Memorandum on Impulse Winding Tester

Memorandum on Impulse Winding Tester Memorandum on Impulse Winding Teser. Esimaion of Inducance by Impulse Response When he volage response is observed afer connecing an elecric charge sored up in he capaciy C o he coil L (including he inside

More information

Notes on the Fourier Transform

Notes on the Fourier Transform Noes on he Fourier Transform The Fourier ransform is a mahemaical mehod for describing a coninuous funcion as a series of sine and cosine funcions. The Fourier Transform is produced by applying a series

More information

Lecture #7: Discrete-time Signals and Sampling

Lecture #7: Discrete-time Signals and Sampling EEL335: Discree-Time Signals and Sysems Lecure #7: Discree-ime Signals and Sampling. Inroducion Lecure #7: Discree-ime Signals and Sampling Unlike coninuous-ime signals, discree-ime signals have defined

More information

Negative frequency communication

Negative frequency communication Negaive frequency communicaion Fanping DU Email: dufanping@homail.com Qing Huo Liu arxiv:2.43v5 [cs.it] 26 Sep 2 Deparmen of Elecrical and Compuer Engineering Duke Universiy Email: Qing.Liu@duke.edu Absrac

More information

P. Bruschi: Project guidelines PSM Project guidelines.

P. Bruschi: Project guidelines PSM Project guidelines. Projec guidelines. 1. Rules for he execuion of he projecs Projecs are opional. Their aim is o improve he sudens knowledge of he basic full-cusom design flow. The final score of he exam is no affeced by

More information

EE 40 Final Project Basic Circuit

EE 40 Final Project Basic Circuit EE 0 Spring 2006 Final Projec EE 0 Final Projec Basic Circui Par I: General insrucion 1. The final projec will coun 0% of he lab grading, since i s going o ake lab sessions. All oher individual labs will

More information

Diodes. Diodes, Page 1

Diodes. Diodes, Page 1 Diodes, Page 1 Diodes V-I Characerisics signal diode Measure he volage-curren characerisic of a sandard signal diode, he 1N914, using he circui shown below. The purpose of he back-o-back power supplies

More information

(This lesson plan assumes the students are using an air-powered rocket as described in the Materials section.)

(This lesson plan assumes the students are using an air-powered rocket as described in the Materials section.) The Mah Projecs Journal Page 1 PROJECT MISSION o MArs inroducion Many sae mah sandards and mos curricula involving quadraic equaions require sudens o solve "falling objec" or "projecile" problems, which

More information

ECE3204 Microelectronics II Bitar / McNeill. ECE 3204 / Term D-2017 Problem Set 7

ECE3204 Microelectronics II Bitar / McNeill. ECE 3204 / Term D-2017 Problem Set 7 EE3204 Microelecronics II Biar / McNeill Due: Monday, May 1, 2017 EE 3204 / Term D-2017 Problem Se 7 All ex problems from Sedra and Smih, Microelecronic ircuis, 7h ediion. NOTES: Be sure your NAME and

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 301 s & Sysems Prof. Mark Fowler Noe Se #1 Wha is s & Sysems all abou??? 1/9 Do All EE s & CoE s Design Circuis? No!!!! Someone has o figure ou wha funcion hose circuis need o do Someone also needs

More information

Pulse Train Controlled PCCM Buck-Boost Converter Ming Qina, Fangfang Lib

Pulse Train Controlled PCCM Buck-Boost Converter Ming Qina, Fangfang Lib 5h Inernaional Conference on Environmen, Maerials, Chemisry and Power Elecronics (EMCPE 016 Pulse Train Conrolled PCCM Buck-Boos Converer Ming Qina, Fangfang ib School of Elecrical Engineering, Zhengzhou

More information

Pointwise Image Operations

Pointwise Image Operations Poinwise Image Operaions Binary Image Analysis Jana Kosecka hp://cs.gmu.edu/~kosecka/cs482.hml - Lookup able mach image inensiy o he displayed brighness values Manipulaion of he lookup able differen Visual

More information

Phase-Shifting Control of Double Pulse in Harmonic Elimination Wei Peng1, a*, Junhong Zhang1, Jianxin gao1, b, Guangyi Li1, c

Phase-Shifting Control of Double Pulse in Harmonic Elimination Wei Peng1, a*, Junhong Zhang1, Jianxin gao1, b, Guangyi Li1, c Inernaional Symposium on Mechanical Engineering and Maerial Science (ISMEMS 016 Phase-Shifing Conrol of Double Pulse in Harmonic Eliminaion Wei Peng1, a*, Junhong Zhang1, Jianxin gao1, b, Guangyi i1, c

More information

Multipath. Introduction. Theory. Multipath 7.1

Multipath. Introduction. Theory. Multipath 7.1 Mulipa 7. Mulipa Inroducion Tere are wo caracerisics o radio cannels a presen serious diiculies or elecommunicaion sysems. One is e remendous dynamic range a mus be accommodaed due o e large cange in pa

More information

Sound so far: 10/13/2013. Sound and stringed instruments

Sound so far: 10/13/2013. Sound and stringed instruments 0/3/203 Sound and ed insrumens Sound so far: Sound is a pressure or densiy flucuaion carried (usually) by air molecules sound wae is longdiudinal Wha is he difference beween a hud and a musical noe? ecure

More information

Control and Protection Strategies for Matrix Converters. Control and Protection Strategies for Matrix Converters

Control and Protection Strategies for Matrix Converters. Control and Protection Strategies for Matrix Converters Conrol and Proecion Sraegies for Marix Converers Dr. Olaf Simon, Siemens AG, A&D SD E 6, Erlangen Manfred Bruckmann, Siemens AG, A&D SD E 6, Erlangen Conrol and Proecion Sraegies for Marix Converers To

More information

Lecture 4. EITN Chapter 12, 13 Modulation and diversity. Antenna noise is usually given as a noise temperature!

Lecture 4. EITN Chapter 12, 13 Modulation and diversity. Antenna noise is usually given as a noise temperature! Lecure 4 EITN75 2018 Chaper 12, 13 Modulaion and diversiy Receiver noise: repeiion Anenna noise is usually given as a noise emperaure! Noise facors or noise figures of differen sysem componens are deermined

More information

Signals and the frequency domain ENGR 40M lecture notes July 31, 2017 Chuan-Zheng Lee, Stanford University

Signals and the frequency domain ENGR 40M lecture notes July 31, 2017 Chuan-Zheng Lee, Stanford University Signals and he requency domain ENGR 40M lecure noes July 3, 07 Chuan-Zheng Lee, Sanord Universiy signal is a uncion, in he mahemaical sense, normally a uncion o ime. We oen reer o uncions as signals o

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 3 Signals & Sysems Prof. Mark Fowler Noe Se #8 C-T Sysems: Frequency-Domain Analysis of Sysems Reading Assignmen: Secion 5.2 of Kamen and Heck /2 Course Flow Diagram The arrows here show concepual

More information

Lecture 11. Digital Transmission Fundamentals

Lecture 11. Digital Transmission Fundamentals CS4/MSc Compuer Neworking Lecure 11 Digial Transmission Fundamenals Compuer Neworking, Copyrigh Universiy of Edinburgh 2005 Digial Transmission Fundamenals Neworks consruced ou of Links or ransmission

More information

Microwave Transistor Oscillator Design

Microwave Transistor Oscillator Design Tuorial on Modern Ulra Low Noise Microwave Transisor Oscillaor Design olumbia Universiy Sepember, 9 Ulrich L. Rohde, Ph.D.* hairman Synergy Microwave orp. *Prof. of RF ircui and Microwave ircui Design

More information

Explanation of Maximum Ratings and Characteristics for Thyristors

Explanation of Maximum Ratings and Characteristics for Thyristors 8 Explanaion of Maximum Raings and Characerisics for Thyrisors Inroducion Daa shees for s and riacs give vial informaion regarding maximum raings and characerisics of hyrisors. If he maximum raings of

More information

Solution of ECE 342 Test 2 S12

Solution of ECE 342 Test 2 S12 Soluion of ECE 342 Tes 2 S2. All quesions regarding superheerodyne receivers refer o his diagram. x c () Anenna B T < B RF < 2 f B = B T Oher Signals f c Mixer f Baseband x RFi RF () x RFo () () () x i

More information

Parameters Affecting Lightning Backflash Over Pattern at 132kV Double Circuit Transmission Lines

Parameters Affecting Lightning Backflash Over Pattern at 132kV Double Circuit Transmission Lines Parameers Affecing Lighning Backflash Over Paern a 132kV Double Circui Transmission Lines Dian Najihah Abu Talib 1,a, Ab. Halim Abu Bakar 2,b, Hazlie Mokhlis 1 1 Deparmen of Elecrical Engineering, Faculy

More information

OpenStax-CNX module: m Elemental Signals. Don Johnson. Perhaps the most common real-valued signal is the sinusoid.

OpenStax-CNX module: m Elemental Signals. Don Johnson. Perhaps the most common real-valued signal is the sinusoid. OpenSax-CNX module: m0004 Elemenal Signals Don Johnson This work is produced by OpenSax-CNX and licensed under he Creaive Commons Aribuion License.0 Absrac Complex signals can be buil from elemenal signals,

More information

Communication Systems. Communication Systems

Communication Systems. Communication Systems Communicaion Sysems Analog communicaion Transmi and receive analog waveforms Ampliude Modulaion (AM Phase Modulaion (PM Freq. Modulaion (FM Quadraure Ampliude Modulaion (QAM Pulse Ampliude Modulaion (PAM

More information

A NEW DUAL-POLARIZED HORN ANTENNA EXCITED BY A GAP-FED SQUARE PATCH

A NEW DUAL-POLARIZED HORN ANTENNA EXCITED BY A GAP-FED SQUARE PATCH Progress In Elecromagneics Research Leers, Vol. 21, 129 137, 2011 A NEW DUAL-POLARIZED HORN ANTENNA EXCITED BY A GAP-FED SQUARE PATCH S. Ononchimeg, G. Ogonbaaar, J.-H. Bang, and B.-C. Ahn Applied Elecromagneics

More information

A New Voltage Sag and Swell Compensator Switched by Hysteresis Voltage Control Method

A New Voltage Sag and Swell Compensator Switched by Hysteresis Voltage Control Method Proceedings of he 8h WSEAS Inernaional Conference on ELECTRIC POWER SYSTEMS, HIGH VOLTAGES, ELECTRIC MACHINES (POWER '8) A New Volage Sag and Swell Compensaor Swiched by Hyseresis Volage Conrol Mehod AMIR

More information

Acquisition of Rotor Anisotropy Signals in Sensorless Position Control Systems

Acquisition of Rotor Anisotropy Signals in Sensorless Position Control Systems IEEE Transacions on Indusry Applicaions, Vol. 4, 24 aaa Acquisiion of Roor Anisoropy Signals in Sensorless Posiion Conrol Sysems Joachim Holz, Fellow, IEEE, and Hangwen Pan Elecrical Machines and Drives

More information

Study on the Wide Gap Dielectric Barrier Discharge Device Gaofeng Wang

Study on the Wide Gap Dielectric Barrier Discharge Device Gaofeng Wang Sudy on he Wide Gap Dielecric Barrier Discharge Device Gaofeng Wang School of Informaion Engineering, Zhengzhou Universiy, Zhengzhou 450001, China 932167312@qq.com Keywords: DBD; Wide air gap; Plasma body;

More information

ELEG 3124 SYSTEMS AND SIGNALS Ch. 1 Continuous-Time Signals

ELEG 3124 SYSTEMS AND SIGNALS Ch. 1 Continuous-Time Signals Deparmen of Elecrical Engineering Universiy of Arkansas ELEG 3124 SYSTEMS AND SIGNALS Ch. 1 Coninuous-Time Signals Dr. Jingxian Wu wuj@uark.edu OUTLINE 2 Inroducion: wha are signals and sysems? Signals

More information

GG6005. General Description. Features. Applications DIP-8A Primary Side Control SMPS with Integrated MOSFET

GG6005. General Description. Features. Applications DIP-8A Primary Side Control SMPS with Integrated MOSFET General Descripion GG65 is a primary side conrol PSR SMPS wih an inegraed MOSFET. I feaures a programmable cable drop compensaion funcion, PFM echnology, and a CV/CC conrol loop wih high reliabiliy and

More information

Primary Side Control SMPS with Integrated MOSFET

Primary Side Control SMPS with Integrated MOSFET General Descripion GG64 is a primary side conrol SMPS wih an inegraed MOSFET. I feaures programmable cable drop compensaion and a peak curren compensaion funcion, PFM echnology, and a CV/CC conrol loop

More information

TESTING CREEPING DISCHARGE BEHAVIOUR OF INSULATORS FOR ISOLATED LIGHTNING PROTECTION SYSTEMS

TESTING CREEPING DISCHARGE BEHAVIOUR OF INSULATORS FOR ISOLATED LIGHTNING PROTECTION SYSTEMS IX Inernaional Symposium on Lighning Proecion 26 h -3 h November 27 Foz do Iguaçu, Brazil TESTING CREEPING DISCHARGE BEHAVIOUR OF INSULATORS FOR ISOLATED LIGHTNING PROTECTION SYSTEMS Beierl, Omar Brocke,

More information

10. The Series Resistor and Inductor Circuit

10. The Series Resistor and Inductor Circuit Elecronicsab.nb 1. he Series esisor and Inducor Circui Inroducion he las laboraory involved a resisor, and capacior, C in series wih a baery swich on or off. I was simpler, as a pracical maer, o replace

More information

Simulation Series Termination

Simulation Series Termination ESE370: Circui-Level Modeling, Design, and Opimizaion for Digial Sysems Day 35: December 5, 2012 Transmission Lines Implicaions 1 Transmission Line Agenda Where arise? General wire formulaion Lossless

More information

Power losses in pulsed voltage source inverters/rectifiers with sinusoidal currents

Power losses in pulsed voltage source inverters/rectifiers with sinusoidal currents ree-wheeling diode Turn-off power dissipaion: off/d = f s * E off/d (v d, i LL, T j/d ) orward power dissipaion: fw/t = 1 T T 1 v () i () d Neglecing he load curren ripple will resul in: fw/d = i Lavg

More information

Installation and Operating Instructions for ROBA -brake-checker Typ

Installation and Operating Instructions for ROBA -brake-checker Typ (B.018102.EN) Guidelines on he Declaraion of Conformiy A conformiy evaluaion has been carried ou for he produc in erms of he EC Low Volage Direcive 2006/95/ EC and EMC Direcive 2004/108/EC. The Declaraion

More information

Solid-state Multi-functional Timer

Solid-state Multi-functional Timer Solid-sae Muli-funcional Timer Eigh operaing modes (H3DE-M) and four operaing modes (H3DE-S) cover a wide range of applicaions. Programmable conac enables he building of a self-holding relay circui (-

More information

MODELING OF CROSS-REGULATION IN MULTIPLE-OUTPUT FLYBACK CONVERTERS

MODELING OF CROSS-REGULATION IN MULTIPLE-OUTPUT FLYBACK CONVERTERS MODELING OF CROSS-REGULATION IN MULTIPLE-OUTPUT FLYBACK CONVERTERS Dragan Maksimovićand Rober Erickson Colorado Power Elecronics Cener Deparmen of Elecrical and Compuer Engineering Universiy of Colorado,

More information

5 Spatial Relations on Lines

5 Spatial Relations on Lines 5 Spaial Relaions on Lines There are number of useful problems ha can be solved wih he basic consrucion echniques developed hus far. We now look a cerain problems, which involve spaial relaionships beween

More information

4 20mA Interface-IC AM462 for industrial µ-processor applications

4 20mA Interface-IC AM462 for industrial µ-processor applications Because of he grea number of indusrial buses now available he majoriy of indusrial measuremen echnology applicaions sill calls for he sandard analog curren nework. The reason for his lies in he fac ha

More information

Dimensions. Model Number. Electrical connection emitter. Features. Electrical connection receiver. Product information. Indicators/operating means

Dimensions. Model Number. Electrical connection emitter. Features. Electrical connection receiver. Product information. Indicators/operating means OBE-R-SE Dimensions.8.8 ø..75 7.5 6. 5 6.7 4.9 4. 5.9 ø.6 Model Number OBE-R-SE Elecrical connecion emier Thru-beam sensor wih m fixed cable Feaures 45 cable oule for maximum mouning freedom under exremely

More information

Electrical connection

Electrical connection Reference scanner Dimensioned drawing en 02-2014/06 50117040-01 200 500mm Disance on background/reference 10-30 V DC We reserve he righ o make changes DS_HRTR46Bref_en_50117040_01.fm Robus objec deecion

More information

Chapter 1: Introduction

Chapter 1: Introduction Second ediion ober W. Erickson Dragan Maksimovic Universiy of Colorado, Boulder.. Inroducion o power processing.. Some applicaions of power elecronics.3. Elemens of power elecronics Summary of he course.

More information

Synchronization of single-channel stepper motor drivers reduces noise and interference

Synchronization of single-channel stepper motor drivers reduces noise and interference hronizaion of single-channel sepper moor drivers reduces noise and inerference n mos applicaions, a non-synchronized operaion causes no problems. However, in some cases he swiching of he wo channels inerfere,

More information

Revision: June 11, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: June 11, E Main Suite D Pullman, WA (509) Voice and Fax 2.5.3: Sinusoidal Signals and Complex Exponenials Revision: June 11, 2010 215 E Main Suie D Pullman, W 99163 (509) 334 6306 Voice and Fax Overview Sinusoidal signals and complex exponenials are exremely

More information

Universal microprocessor-based ON/OFF and P programmable controller MS8122A MS8122B

Universal microprocessor-based ON/OFF and P programmable controller MS8122A MS8122B COMPETENCE IN MEASUREMENT Universal microprocessor-based ON/OFF and P programmable conroller MS8122A MS8122B TECHNICAL DESCRIPTION AND INSTRUCTION FOR USE PLOVDIV 2003 1 I. TECHNICAL DATA Analog inpus

More information

Mobile Communications Chapter 3 : Media Access

Mobile Communications Chapter 3 : Media Access Moivaion Can we apply media access mehods from fixed neworks? Mobile Communicaions Chaper 3 : Media Access Moivaion SDMA, FDMA, TDMA Aloha Reservaion schemes Collision avoidance, MACA Polling CDMA SAMA

More information

Automatic Power Factor Control Using Pic Microcontroller

Automatic Power Factor Control Using Pic Microcontroller IDL - Inernaional Digial Library Of Available a:www.dbpublicaions.org 8 h Naional Conference on Advanced Techniques in Elecrical and Elecronics Engineering Inernaional e-journal For Technology And Research-2017

More information

The student will create simulations of vertical components of circular and harmonic motion on GX.

The student will create simulations of vertical components of circular and harmonic motion on GX. Learning Objecives Circular and Harmonic Moion (Verical Transformaions: Sine curve) Algebra ; Pre-Calculus Time required: 10 150 min. The sudens will apply combined verical ranslaions and dilaions in he

More information

Key Issue. 3. Media Access. Hidden and Exposed Terminals. Near and Far Terminals. FDD/FDMA General Scheme, Example GSM. Access Methods SDMA/FDMA/TDMA

Key Issue. 3. Media Access. Hidden and Exposed Terminals. Near and Far Terminals. FDD/FDMA General Scheme, Example GSM. Access Methods SDMA/FDMA/TDMA Key Issue Can we apply media access mehods from fixed neworks? 3. Media Access SDMA, FDMA, TDMA Aloha and Reservaion Schemes Avoidance and Polling MACA, CDMA, SAMA Example CSMA/CD: Carrier Sense Muliple

More information

Examination Mobile & Wireless Networking ( ) April 12,

Examination Mobile & Wireless Networking ( ) April 12, Page 1 of 5 Examinaion Mobile & Wireless Neworking (192620010) April 12, 2017 13.45 16.45 Noes: Only he overhead shees used in he course, 2 double-sided shees of noes (any fon size/densiy!), and a dicionary

More information

Technology Trends & Issues in High-Speed Digital Systems

Technology Trends & Issues in High-Speed Digital Systems Deailed comparison of dynamic range beween a vecor nework analyzer and sampling oscilloscope based ime domain reflecomeer by normalizing measuremen ime Sho Okuyama Technology Trends & Issues in High-Speed

More information

Chapter 2 Summary: Continuous-Wave Modulation. Belkacem Derras

Chapter 2 Summary: Continuous-Wave Modulation. Belkacem Derras ECEN 44 Communicaion Theory Chaper Summary: Coninuous-Wave Modulaion.1 Modulaion Modulaion is a process in which a parameer of a carrier waveform is varied in accordance wih a given message (baseband)

More information

ECE-517 Reinforcement Learning in Artificial Intelligence

ECE-517 Reinforcement Learning in Artificial Intelligence ECE-517 Reinforcemen Learning in Arificial Inelligence Lecure 11: Temporal Difference Learning (con.), Eligibiliy Traces Ocober 8, 2015 Dr. Iamar Arel College of Engineering Deparmen of Elecrical Engineering

More information

Design of Power Factor Correction Circuit Using AP1662

Design of Power Factor Correction Circuit Using AP1662 Applicaion Noe 075 Design of Power Facor Correcion Circui Using AP66 Prepared by Wang Zhao Kun ysem Engineering Deparmen. nroducion. Produc Feaures The AP66 is an acive power facor conrol C which is designed

More information

ORDER INFORMATION TO pin 320 ~ 340mV AMC7150DLF

ORDER INFORMATION TO pin 320 ~ 340mV AMC7150DLF www.addmek.com DESCRIPTI is a PWM power ED driver IC. The driving curren from few milliamps up o 1.5A. I allows high brighness power ED operaing a high efficiency from 4Vdc o 40Vdc. Up o 200KHz exernal

More information

Dimensions. Transmitter Receiver ø2.6. Electrical connection. Transmitter +UB 0 V. Emitter selection. = Light on = Dark on

Dimensions. Transmitter Receiver ø2.6. Electrical connection. Transmitter +UB 0 V. Emitter selection. = Light on = Dark on OBE-R-SE Dimensions Transmier.. 7.5 9..5.8 4.9 4 5 M 8.9 7.5 9..5.8 4 5 M 8.9 ø.6 ø.6 Model Number OBE-R-SE Thru-beam sensor wih m fixed cable Elecrical connecion Transmier Feaures BN +UB WH IN Ulra-small

More information

Dimensions. Transmitter Receiver ø2.6. Electrical connection. Transmitter +UB 0 V. Emitter selection. = Light on = Dark on

Dimensions. Transmitter Receiver ø2.6. Electrical connection. Transmitter +UB 0 V. Emitter selection. = Light on = Dark on OBE-R-SE Dimensions Transmier.. 7.5 9..5.8 4.9 4 5 M 8.9 7.5 9..5.8 4 5 M 8.9 ø.6 ø.6 Model Number OBE-R-SE Thru-beam sensor wih m fixed cable Elecrical connecion Transmier Feaures BN +UB WH IN Ulra-small

More information

ECE ANALOG COMMUNICATIONS - INVESTIGATION 7 INTRODUCTION TO AMPLITUDE MODULATION - PART II

ECE ANALOG COMMUNICATIONS - INVESTIGATION 7 INTRODUCTION TO AMPLITUDE MODULATION - PART II ECE 405 - ANALOG COMMUNICATIONS - INVESTIGATION 7 INTRODUCTION TO AMPLITUDE MODULATION - PART II FALL 2005 A.P. FELZER To do "well" on his invesigaion you mus no only ge he righ answers bu mus also do

More information

An Improved Zero-Voltage-Transition Technique in a Single-Phase Active Power Factor Correction Circuit

An Improved Zero-Voltage-Transition Technique in a Single-Phase Active Power Factor Correction Circuit An Improved Zero-lage-Transiion Technique in a Single-Phase Acive Power Facor Correcion Circui Suriya Kaewarsa School of Elecrical Engineering, Rajamangala Universiy of Technology Isan Sakon Nakhon Campus,

More information

Transmission Lines. Transmission Lines :: Topics. Introduction Wave Propagation Termination Reflections Summary. Introduction.

Transmission Lines. Transmission Lines :: Topics. Introduction Wave Propagation Termination Reflections Summary. Introduction. Transmission Lines Digial Design and Compuer Archiecure David Money Harris and Sarah L. Harris Transmission Lines :: Topics Inroducion Wave Propagaion Terminaion Reflecions Summary TL- TL- Inroducion

More information

BOUNCER CIRCUIT FOR A 120 MW/370 KV SOLID STATE MODULATOR

BOUNCER CIRCUIT FOR A 120 MW/370 KV SOLID STATE MODULATOR BOUNCER CIRCUIT FOR A 120 MW/370 KV SOLID STATE MODULATOR D. Gerber, J. Biela Laboraory for High Power Elecronic Sysems ETH Zurich, Physiksrasse 3, CH-8092 Zurich, Swizerland Email: gerberdo@ehz.ch This

More information

Digital Communications - Overview

Digital Communications - Overview EE573 : Advanced Digial Communicaions Digial Communicaions - Overview Lecurer: Assoc. Prof. Dr Noor M Khan Deparmen of Elecronic Engineering, Muhammad Ali Jinnah Universiy, Islamabad Campus, Islamabad,

More information

MEASUREMENTS OF VARYING VOLTAGES

MEASUREMENTS OF VARYING VOLTAGES MEASUREMENTS OF ARYING OLTAGES Measuremens of varying volages are commonly done wih an oscilloscope. The oscilloscope displays a plo (graph) of volage versus imes. This is done by deflecing a sream of

More information

AN303 APPLICATION NOTE

AN303 APPLICATION NOTE AN303 APPLICATION NOTE LATCHING CURRENT INTRODUCTION An imporan problem concerning he uilizaion of componens such as hyrisors or riacs is he holding of he componen in he conducing sae afer he rigger curren

More information

Communication Systems. Department of Electronics and Electrical Engineering

Communication Systems. Department of Electronics and Electrical Engineering COMM 704: Communicaion Lecure : Analog Mulipliers Dr Mohamed Abd El Ghany Dr. Mohamed Abd El Ghany, Mohamed.abdel-ghany@guc.edu.eg nroducion Nonlinear operaions on coninuous-valued analog signals are ofen

More information

Anomalous oscillations with an IMP ATT diode

Anomalous oscillations with an IMP ATT diode Philips ech. Rev. 32, 361-369,1971, No. 9/10/11/12 361 Anomalous oscillaions wih an IMP ATT diode P. J. de Waard Inrodueion In 1967 i was discovered ha an IMPATT-diode oscillaor can have a mode of oscillaion

More information

Chapter 2 Introduction: From Phase-Locked Loop to Costas Loop

Chapter 2 Introduction: From Phase-Locked Loop to Costas Loop Chaper 2 Inroducion: From Phase-Locked Loop o Cosas Loop The Cosas loop can be considered an exended version of he phase-locked loop (PLL). The PLL has been invened in 932 by French engineer Henri de Belleszice

More information

f t 2cos 2 Modulator Figure 21: DSB-SC modulation.

f t 2cos 2 Modulator Figure 21: DSB-SC modulation. 4.5 Ampliude modulaion: AM 4.55. DSB-SC ampliude modulaion (which is summarized in Figure 21) is easy o undersand and analyze in boh ime and frequency domains. However, analyical simpliciy is no always

More information

16.5 ADDITIONAL EXAMPLES

16.5 ADDITIONAL EXAMPLES 16.5 ADDITIONAL EXAMPLES For reiew purposes, more examples of boh piecewise linear and incremenal analysis are gien in he following subsecions. No new maerial is presened, so readers who do no need addiional

More information

Integrated Forward Half-Bridge Resonant Inverter as a High-Power-Factor Electronic Ballast

Integrated Forward Half-Bridge Resonant Inverter as a High-Power-Factor Electronic Ballast Inegraed Forward Half-Bridge Resonan Inverer as a High-Power-Facor Elecronic Ballas Absrac.- A novel single-sage high-power-facor elecronic ballas obained from he inegraion of a forward dc-o-dc converer

More information

Lecture 5: DC-DC Conversion

Lecture 5: DC-DC Conversion 1 / 31 Lecure 5: DC-DC Conversion ELEC-E845 Elecric Drives (5 ECTS) Mikko Rouimo (lecurer), Marko Hinkkanen (slides) Auumn 217 2 / 31 Learning Oucomes Afer his lecure and exercises you will be able o:

More information

White paper. RC223 (type B) residual-current release

White paper. RC223 (type B) residual-current release Whie paper (ype B) residual-curren release (ype B) residual curren release Index 1. Generals... 2 2. Applicaion descripion... 3 2.1 Applicaions...3 2.2 Applicaion examples...4 2.3 How does an operae?...6

More information

The Relationship Between Creation and Innovation

The Relationship Between Creation and Innovation The Relaionship Beween Creaion and DONG Zhenyu, ZHAO Jingsong Inner Mongolia Universiy of Science and Technology, Baoou, Inner Mongolia, P.R.China, 014010 Absrac:Based on he compleion of Difference and

More information

LECTURE 1 CMOS PHASE LOCKED LOOPS

LECTURE 1 CMOS PHASE LOCKED LOOPS Lecure 01 (8/9/18) Page 1-1 Objecive LECTURE 1 CMOS PHASE LOCKED LOOPS OVERVIEW Undersand he principles and applicaions of phase locked loops using inegraed circui echnology wih emphasis on CMOS echnology.

More information

Multiple Load-Source Integration in a Multilevel Modular Capacitor Clamped DC-DC Converter Featuring Fault Tolerant Capability

Multiple Load-Source Integration in a Multilevel Modular Capacitor Clamped DC-DC Converter Featuring Fault Tolerant Capability Muliple Load-Source Inegraion in a Mulilevel Modular Capacior Clamped DC-DC Converer Feauring Faul Toleran Capabiliy Faisal H. Khan, Leon M. Tolber The Universiy of Tennessee Elecrical and Compuer Engineering

More information

Variation Aware Cross-Talk Aggressor Alignment by Mixed Integer Linear Programming

Variation Aware Cross-Talk Aggressor Alignment by Mixed Integer Linear Programming ariaion Aware Cross-alk Aggressor Alignmen by Mixed Ineger Linear Programming ladimir Zoloov IBM. J. Wason Research Cener, Yorkown Heighs, NY zoloov@us.ibm.com Peer Feldmann D. E. Shaw Research, New York,

More information

HF Transformer Based Grid-Connected Inverter Topology for Photovoltaic Systems

HF Transformer Based Grid-Connected Inverter Topology for Photovoltaic Systems 1 HF Transformer Based Grid-Conneced Inverer Topology for Phoovolaic Sysems Abhiji Kulkarni and Vinod John Deparmen of Elecrical Engineering, IISc Bangalore, India. (abhijik@ee.iisc.erne.in, vjohn@ee.iisc.erne.in)

More information

Optical fibres. Optical fibres made from high-density glass can carry light signals long distances without losing any light through their sides.

Optical fibres. Optical fibres made from high-density glass can carry light signals long distances without losing any light through their sides. Nearly here Nailed i! Uni 1 Conen Opical fibres Opical fibres made from high-densiy glass can carry ligh signals long disances wihou losing any ligh hrough heir sides. Criical angle The criical angle,

More information

ICT 5305 Mobile Communications

ICT 5305 Mobile Communications ICT 5305 Mobile Communicaions Lecure - 2 April 2016 Dr. Hossen Asiful Musafa 2.1 Frequencies for communicaion VLF = Very Low Frequency LF = Low Frequency MF = Medium Frequency HF = High Frequency VHF =

More information

UNIT IV DIGITAL MODULATION SCHEME

UNIT IV DIGITAL MODULATION SCHEME UNI IV DIGIAL MODULAION SCHEME Geomeric Represenaion of Signals Ojecive: o represen any se of M energy signals {s i (} as linear cominaions of N orhogonal asis funcions, where N M Real value energy signals

More information

Connection. Input II EEx ia IIC without SC red. Composition

Connection. Input II EEx ia IIC without SC red. Composition Sandsill conroller Oupu: relay Connecion Inpu I EEx ia IIC Inpu II EEx ia IIC 1-channel Conrol circui EEx ia IIC Addiional inpu or roaion direcion deecion or sar-up override 2 relay oupus Inpu requency

More information

AM Demodulation (peak detect.)

AM Demodulation (peak detect.) AM Deodulaion (peak deec.) Deodulaion is abou recovering he original signal--crysal Radio Exaple Anenna = Long Wire FM AM Tuning Circui A siple Diode! Deodulaion Circui (envelop of AM Signal) Filer (Mechanical)

More information

Special Insert. Everything you wanted to know about Type B residual current circuit breakers but never dared to ask

Special Insert. Everything you wanted to know about Type B residual current circuit breakers but never dared to ask Special Inser Everyhing you waned o know abou Type B residual curren circui breakers bu never dared o ask Claudio Amadori: R&D ABB 1 Figure 1 - Marking of he Type B residual curren circui breakers Type

More information

PF Coils 2-6 Supply Scope of the project and main technical aspects

PF Coils 2-6 Supply Scope of the project and main technical aspects PF Coils 2-6 Supply Scope of he projec and main echnical aspecs PF Coils formaion Meeing Barcelona - 15 h Ocober 2012 This presenaion is inended for reference purposes only and is no a legally binding

More information

An off-line multiprocessor real-time scheduling algorithm to reduce static energy consumption

An off-line multiprocessor real-time scheduling algorithm to reduce static energy consumption An off-line muliprocessor real-ime scheduling algorihm o reduce saic energy consumpion Firs Workshop on Highly-Reliable Power-Efficien Embedded Designs Shenzhen, China Vincen Legou, Mahieu Jan, Lauren

More information

The University of Melbourne Department of Mathematics and Statistics School Mathematics Competition, 2013 JUNIOR DIVISION Time allowed: Two hours

The University of Melbourne Department of Mathematics and Statistics School Mathematics Competition, 2013 JUNIOR DIVISION Time allowed: Two hours The Universiy of Melbourne Deparmen of Mahemaics and Saisics School Mahemaics Compeiion, 203 JUNIOR DIVISION Time allowed: Two hours These quesions are designed o es your abiliy o analyse a problem and

More information