Sinusoidal Oscillators
|
|
|
- Charles Parsons
- 5 years ago
- Views:
Transcription
1 Sinuoidal Ocillato Signal geneato: inuoidal, ectangula, tiangula, aw-tooth, etc. Obtaining a ine wave: tiangle functional tanf. ine ine wave geneation: fequency elective netwok in a feedback loo of a PF amlifie: inuoidal ocillato - Ocillation fequency: f - Ocillation amlitude: Vˆo - Ocillation citeion - Fequency tability - Amlitude tability - Ditotion coefficient
2 Ocillato feedback loo PF amlifie: x x i a A a x x ; x finite In the comlex domain A( a( a( ( 2f fo a unique a( (
3 Ocillation citeion Bakhauen citeion a ( ( a( a( e a Signal econtuction on the feedback loo ( ( e a( ( ( ( ( a a e module condition: hae condition: Who et Vˆ? o a ( ( a 2 k Nonlineaity of the gain give a give f
4 Ocillato Baic amlifie fequency indeendent o inveting a 8 noninveting a Fequency elective feedback netwok To fulfil the hae condition, thee mut be a unique fequency, f whee the hae hift i: 8, if a, if a 8
5 Baic amlifie fequency indeendent: o inveting a 8 noninveting Ocillato cont. Fequency elective feedback netwok: band-a tye Phae hift of the netwok lie in the ange of [9 o ; -9 o ]. To fulfil the hae condition: only a noninveting amlif can be ued. fecquency (f fo only one It i neceay to get cloe the two ole.
6 o v v ( ( ( out in ( ( v v o ( ( ( ( v v o Z Z Z ( Z Z The WIEN Bidge icuit and comlex tanfe function voltage tanfe
7 out in WIEN Bidge e ( ( 2 2 ( actg Module; Phae ( Module Phae
8 WIEN Bidge ( o ( ( maximum value aymtote aymtote 2 2 ( The module
9 actg WIEN Bidge The hae 9 aymtote 9 aymtote o intemediate value
10 WIEN Bidge Fequency eone Fo an unique fequency f : out in Fo the hae condition: > noninveting amlifie a
11 f 2 ( f 2 3 ( out in If o v v ( ( ( WIEN Bidge Summay
12 O am and WIEN bidge ocillato v ( t Vˆ in 2f o o t a( ( 3 f ( a ˆ? V o Nonlineaity of the gain, cloe to atuation
13 Automatic gain contol (AG a( ( ocillation ae attenuated - zeo a( ( ocillation ae amlified - atuation a ( ( ocillation ae maintained Stability of the ocillation amlitude Automatic gain contol - deending on the outut voltage magnitude Vˆo ˆ V o v Vˆ in 2f o o ( t ct, a(, Vˆ
14 AG fo WIEN bidge ocillato a 4 3 How can an AG be imlemented, o that a i a function on v o? 4 - deendent on v o o 3 - deendent on v o
15 Diode eviited - a vaiable eito Static eitance of a diode in the oeating oint Q 4 D V I D D Q Q 2 Q 3 D D3 VD.495V 4.24k I.279 ma D VD3.6V.263k I ma D3 D2 D4 VD2.555V.599k I.926 ma D2 VD4.645V.5k I 5.64 ma D4 If the voltage do V D inceae, the equivalent tatic eitance D deceae
16 AG uing Diode - how? V D I D D If the voltage do V D inceae, the equivalent tatic eitance D a 4 deceae deendent on v o o 3 - deendent on v o
17 . Uing diode a on ' '' d fo a on ( ( Vˆ o v o (t ' 4 a off a mall, D, D 2 (off 3 '' 4 a off ( v o (t ( inceae, D (on on the oitive half-cycle D 2 (on on the negative half-cycle i given by the value of d 4, ech 3 to maintain ocillation
18 Poblem How doe the voltage v o (t and v (t look like in the teady-tate egime? What i the ocillation fequency? Size 4 o that the cicuit will maintain the ocillation. In conduction aume that the equivalent eitance of the diode D D2.5kΩ. Veify if the ocillation can tat.
19 2. Uing n-channel deletion-tye MOSFET a ' 3 4 DS DS - linea eito contoled by v GS voltage D, 3 negative eak detecto T oeate with v GS <
20 n-channel deletion-tye MOSFET ued in linea egion D G S V Th i D ( v v 2 2 GS Th vds vds DS - linea eito contoled by v GS voltage Fo mall v DS i D 2 ( v GS v Th v DS DS v i DS DS 2 ( v v GS Th
21 a ' 3 4 DS DS 2 ( v V GS Th D, 3 negative eak detecto T oeate with v GS < V Th Vˆ O, v GS, DS, a, Vˆ O
22 O am and ladde netwok ocillato High a band Low a band the hae-hift i in the ange of [ o ; -9 o ] inveting baic amlifie how many identical cell ae neceay to build an ocillato?
23 ( 5 ( 2 6 ( 3 Low-a ladde with 3 cell ( ( 29 f 6 2 ( 29
24 Sinuoidal ocillato with ladde netwok Why the baic amlifie doe not contain only one inveting o-am amlifie?
25 L Ocillato L aallel eonant cicuit ued fo high fequency domain fequency elective feedback netwok Zech Z Z L Z Z L L Zech L / L eonance fequency: Thomon elation f 2 The aallel L cicuit connected in eie with a load act a a band-to filte having infinite imedance at the eonant fequency of the L cicuit. L
26 How the L cicuit and the baic amlifie will be connected? Thee oint ocillato, one tanito amlifie outut inut v o mall-ignal baic cicuit The baic amlifie i an inveting one (E, o the divide Z 2, Z 3 mut intoduce a -8 o hae hift; Z 2, Z 3 will have ooite ign. Z 3 and Z hould be imila to obtain an L aallel eonant cicuit between collecto and bae.
27 Small-ignal equivalent cicuit fo thee oint ocillato vo vo 3 3 L L L 3 f 2 L 2 f 2 L 2
28 2 8 / Otional 7 V PS V PS olitt Hatley
29 ymbol equivalent cicuit Paallel eonance Quatz-cytal ocillato vey low value f can be neglected Seie eonance 2 L ange: ten of KHz hunded of MHz
30 Otional quatz-cytal inuoidal ocillato V PS advantage: vey table fequency, high quality facto diadvantage: ocillate on a fixed fequency (quatz fequency
31 Quatz i amongt one of the mot common mineal in the Eath' continental cut. It ha a hexagonal cytal tuctue made of tigonal cytallized ilica (ilicon dioxide, SiO2 The cytal ocillato cicuit utain ocillation by taking a voltage ignal fom the quatz eonato, amlifying it, and feeding it back to the eonato. The ate of exanion and contaction of the quatz i the eonant fequency, and i detemined by the cut and ize of the cytal. Duing tatu, the cicuit aound the cytal alie a andom noie (acignal to it, and uely by chance, a tiny faction of the noie will be at the eonant fequency of the cytal. The cytal will theefoe tat ocillating in ynchony with that ignal. A the ocillato amlifie the ignal coming out of the cytal, the cytal' fequency will become tonge, eventually dominating the outut of the ocillato. Natual eitance in the cicuit and in the quatz cytal filte out all the unwanted fequencie.
Oscilatoare sinusoidale
Ocilatoae inuoidale Geneatoae de emnale: inuoidal, detunghiula, tiunghiula, ama, etc. Obtineea unui emnal inuiodal: tiunghi tanf. functional inu geneae emnal inuoidal, etea electia in fecenta in bucla
Time and Frequency Response Analysis of Fuzzy Controller
Ravina Bhat et al,int.j.comute Technology & Alication,Vol 3 (3), 59-68 ISSN:9-6093 Time an Fequency Reone Analyi of Fuzzy Contolle Ravina Bhat Shailena.B IEEE Membe Ao. Pof.,IEEE Membe NMIMS, Mukeh Patel
5. The Slip-Ring Induction Machine
5. Te Sli-ing nduction Macine Souce: Siemen AG TECHNSCHE UNVESTÄT DAMSTADT of. A. Binde : Electical Macine and Dive 5/1 ntitut fü Elektice Enegiewandlung FB 18 Active and eactive owe in conume aow ytem
Analysis of Finite Word-Length Effects
T-6.46 Digital Signal Pocessing and Filteing 8.9.4 Intoduction Analysis of Finite Wod-Length Effects Finite wodlength effects ae caused by: Quantization of the filte coefficients ounding / tuncation of
rectangle, triangle, saw tooth, pulse, etc.
Nonsinusoidal Signal Geneatos ectangle, tiangle, saw tooth, pulse, etc. Multiibato cicuits: astable no stable states (two quasi-stable states; it emains in each state fo pedetemined times) monostable one
6. The Squirrel-Cage Induction Machine . (6.2)
Electical Machine and Dive 6/1 Squiel-Cage nduction Machine Electical Machine and Dive 6/ Squiel-Cage nduction Machine 6. The Squiel-Cage nduction Machine Sliping-induction machine do not only have advantage
Detailed solution of IES 2014 (ECE) Conventional Paper II. solve I 0 and use same formula again. Saturation region
etailed olution of IS 4 (C) Conventional Pape II qv qv Sol. (a) IC I e Ie K K 4 I =.7 Fo I C = m olve I and ue ame fomula again K IC V ln 5ln 4 q I.7 =.8576 Volt Sol. (b) VGS VS Vupply 5V N MOS channel,
one primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems
CHAPTER 3: One-Dimenional Steady-State Conduction one pimay diection in which heat tanfe (geneally the mallet dimenion) imple model good epeentation fo olving engineeing poblem 3. Plane Wall 3.. hot fluid
Considerations Regarding the Flux Estimation in Induction Generator with Application at the Control of Unconventional Energetic Conversion Systems
Conideation Regading the Flux Etimation in Induction Geneato with Application at the Contol of Unconventional Enegetic Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of
Figure 1 Siemens PSSE Web Site
Stability Analyi of Dynamic Sytem. In the lat few lecture we have een how mall ignal Lalace domain model may be contructed of the dynamic erformance of ower ytem. The tability of uch ytem i a matter of
Analysis of Arithmetic. Analysis of Arithmetic. Analysis of Arithmetic Round-Off Errors. Analysis of Arithmetic. Analysis of Arithmetic
In the fixed-oint imlementation of a digital filte only the esult of the multilication oeation is quantied The eesentation of a actical multilie with the quantie at its outut is shown below u v Q ^v The
γ from B D(Kπ)K and B D(KX)K, X=3π or ππ 0
fom and X, X= o 0 Jim Libby, Andew Powell and Guy Wilkinon Univeity of Oxfod 8th Januay 007 Gamma meeting 1 Outline The AS technique to meaue Uing o 0 : intoducing the coheence facto Meauing the coheence
Chapter 8 Sampling. Contents. Dr. Norrarat Wattanamongkhol. Lecturer. Department of Electrical Engineering, Engineering Faculty, sampling
Content Chate 8 Samling Lectue D Noaat Wattanamongkhol Samling Theoem Samling of Continuou-Time Signal 3 Poceing Continuou-Time Signal 4 Samling of Dicete-Time Signal 5 Multi-ate Samling Deatment of Electical
4. Induction machines. 4.1 Significance and features of induction machines
Moto develoment 4/1 nduction machine 4. nduction machine 4.1 Significance and featue of induction machine a Baic function and diffeent tye of machine: nduction machine ae in the owe ange of 100 W u to
Boise State University Department of Electrical and Computer Engineering ECE470 Electric Machines
Boie State Univeity Depatment of Electical and Compute Engineeing ECE470 Electic Machine Deivation of the Pe-Phae Steady-State Equivalent Cicuit of a hee-phae Induction Machine Nomenclatue θ: oto haft
Above Flux Estimation Issues in Induction Generators with Application at Energy Conversion Systems
Acta Polytechnica Hungaica Vol. 3, No. 3, 2006 Above Flux Etimation Iue in Induction Geneato with Application at Enegy Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of
INFLUENCE OF DESIGN DATA OF INDUCTION MOTOR ON EFFECTS OF CAGE ASYMMETRY
Pace Nauowe Intytutu Mazyn, Naędów i Pomiaów Eletycznych N 66 Politechnii Wocławiej N 66 Studia i Mateiały N 3 1 Alejando FERNANDEZ GOMEZ* Tadeuz J. SOBCZYK* induction moto, oto cage aymmety, cage moto
Experiment I Voltage Variation and Control
ELE303 Electicity Netwoks Expeiment I oltage aiation and ontol Objective To demonstate that the voltage diffeence between the sending end of a tansmission line and the load o eceiving end depends mainly
Determination of Excitation Capacitance of a Three Phase Self Excited Induction Generator
ISSN (Online): 78 8875 (An ISO 397: 007 Cetified Oganization) Detemination of Excitation Capacitance of a Thee Phae Self Excited Induction Geneato Anamika Kumai, D. A. G. Thoa, S. S. Mopai 3 PG Student
Electromagnetism Physics 15b
lectomagnetism Physics 15b Lectue #20 Dielectics lectic Dipoles Pucell 10.1 10.6 What We Did Last Time Plane wave solutions of Maxwell s equations = 0 sin(k ωt) B = B 0 sin(k ωt) ω = kc, 0 = B, 0 ˆk =
Chapter 5 Part 2. AC Bridges. Comparison Bridges. Capacitance. Measurements. Dr. Wael Salah
Chater 5 Part 2 AC Bridge Comarion Bridge Caacitance Meaurement 5.5 AC - BIDGES AC - Bridge enable u to erform recie meaurement for the following : eactance (caacitance and inductance) meaurement. Determining
c( 1) c(0) c(1) Note z 1 represents a unit interval delay Figure 85 3 Transmit equalizer functional model
Relace 85.8.3.2 with the following: 85.8.3.2 Tansmitted outut wavefom The 40GBASE-CR4 and 100GBASE-CR10 tansmit function includes ogammable equalization to comensate fo the fequency-deendent loss of the
AC DRIVES. There are two type of AC motor Drives : 1. Induction Motor Drives 2. Synchronous Motor Drives
AC DRIVES AC moto Dive ae ued in many indutial and dometic application, uch a in conveye, lift, mixe, ecalato etc. The AC moto have a numbe of advantage : Lightweight (0% to 40% lighte than equivalent
6. The squirrel cage induction machine
6. The quiel cage induction achine TECHSCHE VERSTÄT Pof. A. Binde : Electical Machine and Dive 6/1 ntitut f Eletiche Enegieandlung FB 18 Squiel cage induction achine Coe quiel cage: fo big oe achine >
Online-routing on the butterfly network: probabilistic analysis
Online-outing on the buttefly netwok: obabilistic analysis Andey Gubichev 19.09.008 Contents 1 Intoduction: definitions 1 Aveage case behavio of the geedy algoithm 3.1 Bounds on congestion................................
Simulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements
Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model Paamete fom PER ZETTERBERG Stockholm Septembe 8 TRITA EE 8:49 Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model
Multivariable Control Systems
Multivaiable Contol Sytem Ali Kaimpou Aociate ofeo Fedowi Univeity of Mahhad Refeence ae appeaed in the lat lide. Stability of Multivaiable Feedback Contol Sytem Topic to be coveed include: Well - oedne
Gravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003
avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive
CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES
44 CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES 3.1 INTRODUCTION The contolle equied fo AC dive can be divided into two majo type: cala contol and vecto contol (Boe 1976). In cala contol, which
TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the
Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection
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,
RESONANCE SERIES RESONANT CIRCUITS. 5/2007 Enzo Paterno 1
ESONANCE SEIES ESONANT CICUITS 5/007 Enzo Pateno ESONANT CICUITS A vey impotant cicuit, used in a wide vaiety o electical and electonic systems today (i.e. adio & television tunes), is called the esonant
Mon , (.12) Rotational + Translational RE 11.b Tues.
Mon..-.3, (.) Rotational + Tanlational RE.b Tue. EP0 Mon..4-.6, (.3) Angula Momentum & Toque RE.c Tue. Wed..7 -.9, (.) Toque EP RE.d ab Fi. Rotation Coue Eval.0 Quantization, Quiz RE.e Mon. Review fo Final
Portal del coneixement obert de la UPC
UPCommon Potal del coneixement obet de la UPC htt://ucommon.uc.edu/e-int Taaó, Andé; Candela, Joé Ignacio; Rocabet, Joan; Rodíguez, Pedo (017) Pootional-eonant cuent contolle with othogonal decouling on
22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 18
.65, MHD Theoy of Fuion Sytem Pof. Feidbeg Lectue 8. Deive δw fo geneal cew pinch. Deive Suydam citeion Scew Pinch Equilibia μ p + + ( ) = μ J = μ J= Stability ( ) m k ξ=ξ e ι +ι ξ=ξ e +ξ e +ξ e =ξ +ξ
Solutions. V in = ρ 0. r 2 + a r 2 + b, where a and b are constants. The potential at the center of the atom has to be finite, so a = 0. r 2 + b.
Solutions. Plum Pudding Model (a) Find the coesponding electostatic potential inside and outside the atom. Fo R The solution can be found by integating twice, 2 V in = ρ 0 ε 0. V in = ρ 0 6ε 0 2 + a 2
CHAPTER 14 SIGNAL GENERATORS AND WAVEFORM-SHAPING CIRCUITS
CHAPTE 4 SIGNA GENEATS AN WAEFM-SHAPING CICUITS Chapter utline 4. Baic Principle o Sinuoidal cillator 4. p Amp-C cillator 4. C and Crytal cillator 4.4 Bitable Multiibrator 4.5 Generation o Square and Triangular
Histogram Processing
Hitogam Poceing Lectue 4 (Chapte 3) Hitogam Poceing The hitogam of a digital image with gay level fom to L- i a dicete function h( )=n, whee: i the th gay level n i the numbe of pixel in the image with
55:041 Electronic Circuits
55:04 Electronic ircuit Frequency eone hater 7 A. Kruger Frequency eone- ee age 4-5 o the Prologue in the text Imortant eview v = M co ωt + θ m = M e e j ωt+θ m = e M e jθ me jωt Thi lead to the concet
ME 3600 Control Systems Frequency Domain Analysis
ME 3600 Contol Systems Fequency Domain Analysis The fequency esponse of a system is defined as the steady-state esponse of the system to a sinusoidal (hamonic) input. Fo linea systems, the esulting steady-state
Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law
Faaday s Law Faaday s Epeiments Chapte 3 Law of nduction (emf( emf) Faaday s Law Magnetic Flu Lenz s Law Geneatos nduced Electic fields Michael Faaday discoeed induction in 83 Moing the magnet induces
Conventional Paper-I (a) Explain the concept of gradient. Determine the gradient of the given field: ( )
EE-Conventional Pape-I IES-013 www.gatefoum.com Conventional Pape-I-013 1. (a) Eplain the concept of gadient. Detemine the gadient of the given field: V ρzsin φ+ z cos φ+ρ What is polaization? In a dielectic
V V The circumflex (^) tells us this is a unit vector
Vecto Vecto have Diection and Magnitude Mike ailey mjb@c.oegontate.edu Magnitude: V V V V x y z vecto.pptx Vecto Can lo e Defined a the oitional Diffeence etween Two oint 3 Unit Vecto have a Magnitude
Designing Control Loops for Linear and Switching Power Supplies: A Tutorial Guide Christophe Basso October 2012 Last update March 3 rd 2014
Deigning Control Loo for Linear and Switching Power Sulie: A Tutorial Guide Chritohe Bao October Lat udate March 3 rd 4 Correction of tyo, mitake and error found by reader or by the author himelf. Secial
3. Electromagnetic Waves II
Lectue 3 - Electomagnetic Waves II 9 3. Electomagnetic Waves II Last time, we discussed the following. 1. The popagation of an EM wave though a macoscopic media: We discussed how the wave inteacts with
LC transfer of energy between the driving source and the circuit will be a maximum.
The Q of oscillatos efeences: L.. Fotney Pinciples of Electonics: Analog and Digital, Hacout Bace Jovanovich 987, Chapte (AC Cicuits) H. J. Pain The Physics of Vibations and Waves, 5 th edition, Wiley
Simulink Model of Direct Torque Control of Induction Machine
Ameican Jounal of Applied Science 5 (8): 1083-1090, 2008 ISSN 1546-9239 2008 Science Publication Simulink Model of Diect Toque Contol of Induction Machine H.F. Abdul Wahab and H. Sanui Faculty of Engineeing,
Development of Model Reduction using Stability Equation and Cauer Continued Fraction Method
Intenational Jounal of Electical and Compute Engineeing. ISSN 0974-90 Volume 5, Numbe (03), pp. -7 Intenational Reeach Publication Houe http://www.iphoue.com Development of Model Reduction uing Stability
55:041 Electronic Circuits
55:041 Electonic icuits BJT eview Sections in hapte 5 & 6 in Textbook A. Kuge BJT eview, Page- 1 npn Output Family of uves A. Kuge BJT eview, Page- 2 npn BJT dc Equivalent evese biased Fowad biased i B
MAC Module 12 Eigenvalues and Eigenvectors
MAC 23 Module 2 Eigenvalues and Eigenvectos Leaning Objectives Upon completing this module, you should be able to:. Solve the eigenvalue poblem by finding the eigenvalues and the coesponding eigenvectos
ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson Dept. Of ECE. Notes 20 Dielectrics
ECE 3318 Applied Electicity and Magnetism Sping 218 Pof. David R. Jackson Dept. Of ECE Notes 2 Dielectics 1 Dielectics Single H 2 O molecule: H H Wate ε= εε O 2 Dielectics (cont.) H H Wate ε= εε O Vecto
ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D.
ELETROSTATIS::BHSE 9-4 MQ. A moving electic chage poduces A. electic field only. B. magnetic field only.. both electic field and magnetic field. D. neithe of these two fields.. both electic field and magnetic
Chapter 3 Problem Solutions
Chate Poblem Solutions Poblem A Equation (5) gives P P G G log h log h L 4 log d t t t sys Substituting gives P log 6 log log 4 log 875 m B The wavelength is given by 8 The fee-sace ath loss is then 9
Lecture 10. Erbium-doped fiber amplifier (EDFA) Raman amplifiers Have replaced semiconductor optical amplifiers in the course
ecture 1 Two tye of otical amlifier: Erbium-doed fiber amlifier (EDFA) Raman amlifier Have relaced emiconductor otical amlifier in the coure Fiber Otical Communication ecture 1, Slide 1 Benefit and requirement
Chapter 33 Alternating Current
hapte 33 Altenating uent icuits Most of the electical enegy is poduced by electical geneatos in the fom of sinusoidal altenating cuent. Why do we use the sinusoidal electic potential but neithe the tiangula
Look over Chapter 22 sections 1-8 Examples 2, 4, 5, Look over Chapter 16 sections 7-9 examples 6, 7, 8, 9. Things To Know 1/22/2008 PHYS 2212
PHYS 1 Look ove Chapte sections 1-8 xamples, 4, 5, PHYS 111 Look ove Chapte 16 sections 7-9 examples 6, 7, 8, 9 Things To Know 1) What is an lectic field. ) How to calculate the electic field fo a point
Wolfgang Hofle. CERN CAS Darmstadt, October W. Hofle feedback systems
Wolfgang Hofle Wolfgang.Hofle@cern.ch CERN CAS Darmtadt, October 9 Feedback i a mechanim that influence a ytem by looping back an output to the input a concept which i found in abundance in nature and
NODIA AND COMPANY. GATE SOLVED PAPER Electronics & Communication Control System. Copyright By NODIA & COMPANY
No art of thi ublication may be reroduced ditributed in any fm any mean, electronic, mechanical, hotocoying, otherwie without the ri ermiion of the auth. ATE OLVED PAPER Electronic & Communication Control
rad rev 60sec p sec 2 rad min 2 2
NAME: EE 459/559, Exa 1, Fall 2016, D. McCalley, 75 inute allowed (unle othewie diected) Cloed Book, Cloed Note, Calculato Peitted, No Counication Device. The following infoation ay o ay not be ueful fo
Image Enhancement: Histogram-based methods
Image Enhancement: Hitogam-baed method The hitogam of a digital image with gayvalue, i the dicete function,, L n n # ixel with value Total # ixel image The function eeent the faction of the total numbe
Inference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo
Infeence fo A One Way Factoial Expeiment By Ed Stanek and Elaine Puleo. Intoduction We develop etimating equation fo Facto Level mean in a completely andomized one way factoial expeiment. Thi development
Theory. Single Soil Layer. ProShake User s Manual
PoShake Ue Manual Theoy PoShake ue a fequency domain appoach to olve the gound epone poblem. In imple tem, the input motion i epeented a the um of a eie of ine wave of diffeent amplitude, fequencie, and
Systems Analysis. Prof. Cesar de Prada ISA-UVA
Sytem Analyi Prof. Cear de Prada ISAUVA rada@autom.uva.e Aim Learn how to infer the dynamic behaviour of a cloed loo ytem from it model. Learn how to infer the change in the dynamic of a cloed loo ytem
ROOT LOCUS. Poles and Zeros
Automatic Control Sytem, 343 Deartment of Mechatronic Engineering, German Jordanian Univerity ROOT LOCUS The Root Locu i the ath of the root of the characteritic equation traced out in the - lane a a ytem
Rotational Kinetic Energy
Add Impotant Rotational Kinetic Enegy Page: 353 NGSS Standad: N/A Rotational Kinetic Enegy MA Cuiculum Famewok (006):.1,.,.3 AP Phyic 1 Leaning Objective: N/A, but olling poblem have appeaed on peviou
6.641 Electromagnetic Fields, Forces, and Motion Spring 2005
MIT OpenouseWae http://ocw.mit.edu 6.641 Electomagnetic Fields, Foces, and Motion Sping 2005 Fo infomation about citing these mateials o ou Tems of Use, visit: http://ocw.mit.edu/tems. 6.641 Electomagnetic
MULTILAYER PERCEPTRONS
Last updated: Nov 26, 2012 MULTILAYER PERCEPTRONS Outline 2 Combining Linea Classifies Leaning Paametes Outline 3 Combining Linea Classifies Leaning Paametes Implementing Logical Relations 4 AND and OR
17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other
Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system
Sensorless Control of Induction Motor Drives
Poceeding of the IEEE, Vol. 9, No. 8, Aug., pp. 359-394 Senole Contol of Induction Moto Dive Joachim Holtz, Fellow, IEEE Electical Machine and Dive Goup, Univeity of Wuppetal 497 Wuppetal Gemany Abtact
Article : 8 Article : 8 Stress Field. and. Singularity Problem
Aticle : 8 Aticle : 8 Stess Field and Singulaity Poblem (fatigue cack gowth) Repeated load cycles cack development Time (cycles) Cack length 3 Weakening due to gowing cacks Cack length stess concentation
CHAPTER 5. The Operational Amplifier 1
EECE22 NETWORK ANALYSIS I Dr. Charle J. Kim Cla Note 9: Oerational Amlifier (OP Am) CHAPTER. The Oerational Amlifier A. INTRODUCTION. The oerational amlifier or o am for hort, i a eratile circuit building
Lecture 12 - Non-isolated DC-DC Buck Converter
ecture 12 - Non-iolated DC-DC Buck Converter Step-Down or Buck converter deliver DC power from a higher voltage DC level ( d ) to a lower load voltage o. d o ene ref + o v c Controller Figure 12.1 The
Thermodynamic Properties of Ammonia-Water Mixture
ppendix hemodynamic opetie of mmonia-wate Mixtue. INROUION mmonia-wate mixtue i a woking fluid ued in Kalina cycle ytem (KS) and apo aboption efigeation (VR) plant. Unlike fo pue component, binay mixtue
x 1 b 1 Consider the midpoint x 0 = 1 2
1 chapte 2 : oot-finding def : Given a function f(), a oot is a numbe satisfying f() = 0. e : f() = 2 3 = ± 3 question : How can we find the oots of a geneal function f()? 2.1 bisection method idea : Find
CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS
17 CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS 2.1 DESCRIPTION The development of wind enegy ytem and advance in powe electonic have enabled an efficient futue fo wind enegy. Ou imulation tudy
Review: Electrostatics and Magnetostatics
Review: Electostatics and Magnetostatics In the static egime, electomagnetic quantities do not vay as a function of time. We have two main cases: ELECTROSTATICS The electic chages do not change postion
Circular Motion & Torque Test Review. The period is the amount of time it takes for an object to travel around a circular path once.
Honos Physics Fall, 2016 Cicula Motion & Toque Test Review Name: M. Leonad Instuctions: Complete the following woksheet. SHOW ALL OF YOUR WORK ON A SEPARATE SHEET OF PAPER. 1. Detemine whethe each statement
CMSC 425: Lecture 5 More on Geometry and Geometric Programming
CMSC 425: Lectue 5 Moe on Geomety and Geometic Pogamming Moe Geometic Pogamming: In this lectue we continue the discussion of basic geometic ogamming fom the eious lectue. We will discuss coodinate systems
Design of CMOS Analog Integrated Circuits. Basic Building Block
Desin of CMOS Analo Inteated Cicuits Fanco Malobeti Basic Buildin Block F. Malobeti : Desin of CMOS Analo Inteated Cicuits - Basic Buildin Block INERTER WITH ACTIE LOAD The simplest fom of ain stae, the
Control Systems. Root locus.
Control Sytem Root locu chibum@eoultech.ac.kr Outline Concet of Root Locu Contructing root locu Control Sytem Root Locu Stability and tranient reone i cloely related with the location of ole in -lane How
EKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES
EKT 345 MICROWAVE ENGINEERING CHAPTER : PLANAR TRANSMISSION LINES 1 Tansmission Lines A device used to tansfe enegy fom one point to anothe point efficiently Efficiently minimum loss, eflection and close
Then the number of elements of S of weight n is exactly the number of compositions of n into k parts.
Geneating Function In a geneal combinatoial poblem, we have a univee S of object, and we want to count the numbe of object with a cetain popety. Fo example, if S i the et of all gaph, we might want to
Lecture 14. Static Analysis. RF MEMS Switches. Agenda: Different Configurations of RF MEMS Devices
EEL695 vance MEMS (Sin 5) Intucto: D. Huikai Xie Diffeent onfiuation of RF MEMS Device ena: Lectue 14 Eectotatic otae () -8 ctuation Mechanim uent (m) owe (mw) Size Sma Switchin time (µ) 1- ontact foce
On a proper definition of spin current
On a pope definition of pin cuent Qian Niu Univeity of Texa at Autin P. Zhang, Shi, Xiao, and Niu (cond-mat 0503505) P. Zhang and Niu (cond-mat/0406436) Culce, Sinova, Sintyn, Jungwith, MacDonald, and
MAGNETIC FIELD INTRODUCTION
MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),
Edge Cover Time for Regular Graphs
1 2 3 47 6 23 11 Jounal of Intege Sequences, Vol. 11 (28, Aticle 8.4.4 Edge Cove Time fo Regula Gahs Robeto Tauaso Diatimento di Matematica Univesità di Roma To Vegata via della Riceca Scientifica 133
Operational transconductance amplifier based voltage-mode universal filter
Indian Journal of Pure & Alied Phyic ol. 4, etember 005,. 74-79 Oerational tranconductance amlifier baed voltage-mode univeral filter Naeem Ahmad & M R Khan Deartment of Electronic and Communication Engineering,
Physics 107 HOMEWORK ASSIGNMENT #15
Physics 7 HOMEWORK SSIGNMENT #5 Cutnell & Johnson, 7 th eition Chapte 8: Poblem 4 Chapte 9: Poblems,, 5, 54 **4 small plastic with a mass of 6.5 x - kg an with a chage of.5 µc is suspene fom an insulating
Waves and Polarization in General
Waves and Polaization in Geneal Wave means a distubance in a medium that tavels. Fo light, the medium is the electomagnetic field, which can exist in vacuum. The tavel pat defines a diection. The distubance
Computing Electromagnetic Fields in Inhomogeneous Media Using Lattice Gas Automata. I. Introduction
Comuting Electomagnetic Fields in Inhomogeneous Media Using Lattice Gas Automata M.Zhang, D. Cule, L. Shafai, G. Bidges and N.Simons Deatment of Electical and Comute Engineeing Univesity of Manitoba Winnieg,
Lecture 6. Erbium-doped fiber amplifier (EDFA) Raman amplifiers Have replaced semiconductor optical amplifiers in the course
Lecture 6 wo tye of otical amlifier: Erbium-doed fiber amlifier (EDFA) Raman amlifier Have relaced emiconductor otical amlifier in the coure Fiber Otical Communication Lecture 6, Slide 1 Benefit and requirement
you of a spring. The potential energy for a spring is given by the parabola U( x)
Small oscillations The theoy of small oscillations is an extemely impotant topic in mechanics. Conside a system that has a potential enegy diagam as below: U B C A x Thee ae thee points of stable equilibium,
x with A given by (6.2.1). The control ( ) ( )
Homework 5 Sring 9 AerE33 Due 4/(F) SOLUTION PROBLEM (3t) In thi roblem we will invetigate the longitudinal dynamic of the B747 airlane a decribed in Etkin 66 The tate model i x Ax Bu where the tate vector
Control Systems. Root locus.
Control Sytem Root locu chibum@eoultech.ac.kr Outline Concet of Root Locu Contructing root locu Control Sytem Root Locu Stability and tranient reone i cloely related with the location of ole in -lane How
Original Method for Stability Analysis of Mechatronic Systems with Asynchronous Machines
Soin Enache, Auel Campeanu, Oiginal Method fo Stability Analyi of Mechatonic Sytem with Aynchonou Machine SORIN ENACHE, AUREL CAMPEANU, ION VLAD, MONICA ADELA ENACHE Electomechanical Faculty Univeity of
Physics 122, Fall September 2012
Physics 1, Fall 1 7 Septembe 1 Today in Physics 1: getting V fom E When it s best to get V fom E, athe than vice vesa V within continuous chage distibutions Potential enegy of continuous chage distibutions
Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!
Ch 30 - Souces of Magnetic Field 1.) Example 1 Detemine the magnitude and diection of the magnetic field at the point O in the diagam. (Cuent flows fom top to bottom, adius of cuvatue.) Fo staight segments,
Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits
Phys-7 ectue 8 Mutual nductance Self-nductance - Cicuits Mutual nductance f we have a constant cuent i in coil, a constant magnetic field is ceated and this poduces a constant magnetic flux in coil. Since
18 Problem 1. 7 d Sketch a cross section of a switched reluctance machine and explain the principle of operation.
Exam Electrical Machine and Drive (ET4117) 9 November 01 from 14.00 to 17.00. Thi exam conit of 3 roblem on 3 age. Page 5 can be ued to anwer roblem 4 quetion a. The number before a quetion indicate how
ANALYSIS AND DESIGN OF ONE-BIT NOISE-SHAPING QUANTIZER USING VARIABLE STRUCTURE CONTROL APPROACH
266 Aian Jounal of Contol, Vol. 7, No. 3, pp. 266-274, Septembe 2005 ANALYSIS AND DESIGN OF ONE-BI NOISE-SHAPING QUANIZER USING VARIABLE SRUCURE CONROL APPROACH Jwuheng Hu and Shiang-Hwua Yu ABSRAC hi