Circuit Synthesizable Guaranteed Passive Modeling for Multiport Structures
|
|
- Martina Matthews
- 5 years ago
- Views:
Transcription
1 Cicuit Synthesizable Guaanteed Passive Modeling fo Multipot Stuctues Zohaib Mahmood, Luca Daniel Massachusetts Institute of Technology BMAS Septembe-23, 2010
2 Outline Motivation fo Compact Dynamical Passive Modeling What is Passivity? Existing Techniques Rational Fitting of Tansfe Functions Results 2
3 Outline Motivation fo Compact Dynamical Passive Modeling What is Passivity? Existing Techniques Rational Fitting of Tansfe Functions Results 3
4 Motivation fo Model Geneation Electomagnetic Field Solve Cicuit Simulato (Time Domain Simulations) 4
5 Motivation fo Model Geneation Step 1: Field Solves OR Measuements Fequency Response Samples (H i ) S/Z-Paametes Step 2 : Samples Tansfe Function Matix Z H ( s) = Z 11 ( s). N1 ( s) Z Z 1N NN ( s). ( s) H (s) must be PASSIVE Cicuit Simulato (Time Domain Simulations) 5
6 Outline Motivation fo Compact Dynamical Passive Modeling What is Passivity? Existing Techniques Rational Fitting of Tansfe Functions Results 6
7 What is a Passive Netwo/Model? DEFINITION Passivity is the inability of a system (o model) to geneate enegy All physical systems dissipate enegy, and ae theefoe passive Fo numeical models of such systems, this is not guaanteed unless enfoced Passivity fo an impedance (o admittance) matix is implied by positive ealness. 7
8 Conditions fo Passivity Conditions fo Passivity (Hybid Paametes) H ˆ ( s) is passive iff: Hˆ( s) = Hˆ() s Condition 1 Conjugate Symmety Condition 2 Stability Condition 3 Non-negativity Hˆ ( s ) is analytic in R { s } > 0 ˆ ˆ Ψ ( jω) = H( jω) + H( jω) ± 0 ω Real impulse esponse All poles in left half plane Ψ( jω) Non-negative eigen values of foall ω 8
9 Conditions fo Passivity Conditions fo Passivity (Hybid Paametes) H ˆ ( s) is passive iff: Hˆ( s) = Hˆ() s Condition 1 Conjugate Symmety Condition 2 Stability Condition 3 Non-negativity Hˆ ( s ) is analytic in R { s } > 0 ˆ ˆ Ψ ( jω) = H( jω) + H( jω) ± 0 ω Real impulse esponse All poles in left half plane Ψ( jω) Non-negative eigen values of foall ω 9
10 Conditions fo Passivity Conditions fo Passivity (Hybid Paametes) H ˆ ( s) is passive iff: Hˆ( s) = Hˆ() s Condition 1 Conjugate Symmety Condition 2 Stability Condition 3 Non-negativity Hˆ ( s ) is analytic in R { s } > 0 ˆ ˆ Ψ ( jω) = H( jω) + H( jω) ± 0 ω Real impulse esponse All poles in left half plane Ψ( jω) Non-negative eigen values of foall ω 10
11 11 Manifestation of Passivity Multi Pot Case n n n n n n s X j s R s Z + = )] ( [ )] ( [ )] ( [ ) ( ) ( ) ( ) (,,1 1, 1,1 s R s R s R s R n n n n
12 Multi Pot Case Manifestation of Passivity [ Z ( s)] = [ R( s)] + j[ X ( s)] n n n n n n R R 1,1 n,1 ( s) ( s) R R 1, n, n( s) ( s) n -Fequency dependent eal matix must be positive semidefinite fo all fequencies -Popety of entie matix, cannot enfoce element-wise 12
13 What if passivity is not peseved -Cicuit simulation may blow-up -Simulato convegence issues -Results may become completely non-physical. o... passive model +... non-passive model (time domain simulation) 13
14 Outline Motivation fo Compact Dynamical Passive Modeling What is Passivity? Existing Techniques Rational Fitting of Tansfe Functions Results 14
15 Designes way aound -- Analytic / Intuitive Appoaches RL/RC Netwos chaacteized at opeating fequency Develop RLC Netwo fom intuition 15
16 Numeical Appoaches Technique Pos Cons Pojection appoaches e.g. PRIMA [Odabasioglu 1997] Vecto Fitting [Gustavsen 1999] Pole discading appoaches [Mosey 2001] Petubation based appoaches [Talocia 2004, Gustavsen 2008] Optimization based appoaches [Suo 2008] Passivity peseved Efficient, Robust Passivity enfoced Passivity enfoced Passivity enfoced Does not wo with fequency esponse data. Passivity not peseved Highly estictive, non-passive pole-esidues ae discaded Two step pocess. Final models may lose accuacy and optimality Computationally expensive, fequency dependent constaints Ou Appoach: Enfoce passivity duing identification, using efficient optimization famewo 16
17 Numeical Appoaches Technique Pos Cons Pojection appoaches e.g. PRIMA [Odabasioglu 1997] Vecto Fitting [Gustavsen 1999] Pole discading appoaches [Mosey 2001] Petubation based appoaches [Talocia 2004, Gustavsen 2008] Optimization based appoaches [Suo 2008] Passivity peseved Efficient, Robust Passivity enfoced Passivity enfoced Passivity enfoced Does not wo with fequency esponse data. Passivity not peseved Highly estictive, non-passive pole-esidues ae discaded Two step pocess. Final models may lose accuacy and optimality Computationally expensive, fequency dependent constaints Ou Appoach: Enfoce passivity duing identification, using efficient optimization famewo 17
18 Outline Motivation fo Compact Dynamical Passive Modeling What is Passivity? Existing Techniques Rational Fitting of Tansfe Functions Results 18
19 Poblem Statement Given fequency esponse samples { ω i, H i } Seach fo optimal passive ational appoximation in the pole esidue fom Hˆ () s κ = + = 1 s R a D 19
20 Poblem Statement Given fequency esponse samples { ω i, H i } Seach fo optimal passive ational appoximation in the pole esidue fom Hˆ () s κ = + = 1 s R a D Fomulate as optimization poblem L : min H Hˆ ( s) 2 pq, 2 i i pq, L : min max H Hˆ ( s) i i Subject to: H ˆ ( s) PASSIVE 20
21 Poblem Statement Given fequency esponse samples { ω i, H i } Seach fo optimal passive ational appoximation in the pole esidue fom Hˆ () s κ = + = 1 s R a D Fomulate as optimization poblem L : min H Hˆ ( s) 2 pq, 2 i i pq, L : min max H Hˆ ( s) i i Subject to: H ˆ ( s) PASSIVE 21
22 Convex Optimization Poblems Non-convex poblems difficult to solve min H Hˆ ( s) pq, i i 2 Non-convex function (finding global minimum-extemely difficult) Subject to: ˆ ( ) : PASSIVE H s Must efomulate as convex optimization poblem Convex objective function Convex constaints Convex function (finding global minimum-easy) 22
23 Modeling Flow Step 1: Identify a COMMON set of STABLE poles -Vecto Fitting Algoithm [Gustavsen 1999] - Optimization Famewo [Suo 2008] Step 2: Use POLES fom step 1 to identify passive model min H Hˆ ( s) pq, i i 2 Subject to: ˆ ( ) : PASSIVE H s 23
24 Poblem Fomulation Hˆ ( jω ) κ R = + D jω a = 1 κ κc / 2 ˆ ω = 1 = 1 ( ) ˆ c = H j + H ( jω) + D κ κc /2 c c c c R R + ji R ji = R + R R R + c c c c + D = 1 jω a = 1 jω Ra ji a jω Ra + jia 24
25 Poblem Fomulation Hˆ ( jω ) κ R = + D jω a = 1 κ κc / 2 ˆ ω = 1 = 1 ( ) ˆ c = H j + H ( jω) + D κ κc /2 c c c c R R + ji R ji = R + R R R + c c c c + = 1 jω a = 1 jω Ra ji a jω Ra + jia D seies/paallel inteconnection of fist ode netwos seies/paallel inteconnection of second ode netwos esistive/conductive netwo 25
26 Poblem Fomulation Hˆ ( jω ) κ R = + D jω a = 1 κ κc / 2 ˆ ω = 1 = 1 ( ) ˆ c = H j + H ( jω) + D κ κc /2 c c c c R R + ji R ji = R + R R R + c c c c + = 1 jω a = 1 jω Ra ji a jω Ra + jia D seies/paallel inteconnection of fist ode netwos Passivity Conditions: seies/paallel inteconnection of second ode netwos esistive/conductive netwo Condition 1 Conjugate Symmety: Enfoced by constuction Condition 2 Stability: Enfoced duing pole-identification Condition 3 Non-negativity: Enfoced on the building blocs 26
27 Passivity Conditions κ κc / 2 D = 1 = 1 ˆ( ) ˆ ( ) ˆ c H jω = H jω + H ( jω) + A sufficient condition fo passivity: ˆ ( ), ˆ c H jω H ( jω), D passive Hˆ( jω) passive ˆ ( ) 0, ˆ c RH jω ± RH ( jω) ± 0, D ± 0 RHˆ( jω) ± 0 27
28 Real-only poles ˆ H ( jω ) = R jω a ˆ a R H ( j ) j ω = ω + a ω + a a Passivity Conditions ˆ( ) ˆ ( ) ˆ c H jω = H jω + H ( jω) + ωr ˆ a R H ( jω ) 0 R = ± R ± 0 ω κ κc / 2 D = 1 = 1 28
29 Real-only poles ˆ H ( jω ) = R jω a ˆ a R H ( j ) j ω = ω + a ω + a a Passivity Conditions ˆ( ) ˆ ( ) ˆ c H jω = H jω + H ( jω) + ωr ˆ a R H ( jω ) 0 R = ± R ± 0 ω κ κc / 2 D = 1 = 1 - Diect Matix D ± 0 29
30 Passivity Conditions Real-only poles Complex poles ˆ c RH ( jω ) ± 0. ˆ H ( jω ) = ˆ a R H ( j ) j ω = ω + a ω + a ˆ a R H ( jω ) 0 R = ± R ± 0 ω ω 0 c c c c 2 c c c c ( R R) + ω ( R + R). CPR( ω) = Ra R Ia I Ra R Ia I ± 0, ω. c c c c.lim CPR( ω) Ra RR Ia IR ± 0 c c c c. lim CPR( ω) Ra RR + Ia IR ± 0 ω ˆ( ) ˆ ( ) ˆ c H jω = H jω + H ( jω) + R jω a a κ κc / 2 D = 1 = 1 ωr - Diect Matix D ± 0 30
31 Passivity Conditions Real-only poles Complex poles ˆ c RH ( jω ) ± 0. ˆ H ( jω ) = ˆ a R H ( j ) j ω = ω + a ω + a ar H jω R 2 2 ω + a R ˆ ( ) = ± 0 ± 0 ω 0 c c c c 2 c c c c ( R R) + ω ( R + R). CPR( ω) = Ra R Ia I Ra R Ia I ± 0, ω. c c c c.lim CPR( ω) Ra RR Ia IR ± 0 c c c c. lim CPR( ω) Ra RR + Ia IR ± 0 ω ˆ( ) ˆ ( ) ˆ c H jω = H jω + H ( jω) + R jω a κ κc / 2 D = 1 = 1 ωr - Diect Matix D ± 0 Linea Matix Inequalities (Extemely efficient) Unnowns 31
32 Convex fomulation minimize RH R Hˆ( jω ) + IH IHˆ( jω ) c R, R, D subject to D ± 0 R ± 0 = 1,..., κ 2 2 i i i i i c c c c Ra R R + Ia IR ± 0 = 1,..., κ c c c c Ra RR Ia IR ± 0 = 1,..., κ whee Hˆ ( jω ) i κ κc = 1 ω = 1 c c c R R = + + D j a jω a c Linea Matix Inequalities (Extemely efficient) 32
33 Final Optimization Poblem Samples { ω i, H i }, Desied numbe of poles (N) Find N Stable poles a a minimize RH R Hˆ( jω ) + IH IHˆ( jω ) c R, R, D i 2 2 i i i i i subject to: D± 0, R ± 0 = 1,..., κ c c c c Ra R R + Ia IR ± 0 = 1,..., κ c c c c c Ra RR Ia IR ± 0 = 1,..., κ c Convex Optimization Poblem c c ˆ R R H ( j ) ω = + + c j a jω a a κ κ = 1 ω = 1 c, R, R, D D Cicuit Module (Netlist/ VeilogA Dynamical Model) 33
34 Outline Motivation fo Compact Dynamical Passive Modeling What is Passivity? Existing Techniques Rational Fitting of Tansfe Functions Results 34
35 Results: LINC Powe Amplifie Bloc diagam of the LINC powe amplifie achitectue 35
36 Results: LINC Powe Amplifie Bloc diagam of the LINC powe amplifie achitectue Layout of the Wilinson Combine 36
37 Results: LINC Powe Amplifie Bloc diagam of the LINC powe amplifie achitectue Layout of the Wilinson Combine -Numbe of poles 10 -Time [Matlab] 2 seconds -Eo < 0.7% EM Field Solve (dots) Tansfe Function Matix Z11( s)... Z1N ( s) H() s =... ZN 1( s)... ZNN ( s) Passive Modeling Algoithm (solid lines) Compaing eal and imaginay pats of the impedance paametes fom EM field solve (dots) and ou passive model (solid lines) 37
38 Results: LINC Powe Amplifie Hamiltonian Matix Based Passivity Test Model is passive if the associated Hamiltonian matix has no puely imaginay eigen value Tansfe Function Matix Z11( s)... Z1N ( s) H() s =... ZN 1( s)... ZNN ( s) Zoomed-in eigen values of the associated Hamiltonian matix fo the identified model of Wilinson combine 38
39 Results: LINC Powe Amplifie Bloc diagam of the LINC powe amplifie as simulated inside the cicuit simulato Z11( s)... Z1N ( s) H() s =... ZN 1( s)... ZNN ( s) Passive Tansfe Matix 39
40 Results: LINC Powe Amplifie Bloc diagam of the LINC powe amplifie as simulated inside the cicuit simulato Z11( s)... Z1N ( s) H() s =... ZN 1( s)... ZNN ( s) Passive Tansfe Matix LINC PA Nomalized Input Voltage (v in ) Nomalized Output Voltage (v out ) 40
41 Example: 8-Pot Powe/Gnd Distibution Gid QUALITY CHECK (Impedance matix) - Hamiltonian Matix Based Passivity Test Passed -Numbe of poles 20 -Time [Matlab] 74 seconds 41
42 Example: 4-Pot Inducto Aay QUALITY CHECK (Impedance matix) - Hamiltonian Matix Based Passivity Test Passed -Numbe of poles 23 -Time [Matlab] 72 seconds 42
43 Compaison Stuctue Wilinson Combine Numbe of Pots Numbe of Poles [Suo 2008] Time 1 (seconds) This Wo [Matlab] Powe Distibution Gid Coupled RF inductos NA NA Laptop: Coe2Duo 2.1GHz, 3GB, Windows 7 43
44 Conclusions Summaized how to develop models fom feq. esponse Poposed a Convex Optimization based modeling algoithm Demonstated odes of magnitude impovement ove simila techniques Pesented an example demonstating system level simulation of analog cicuits 44
45 THANK YOU 45
Absolute Specifications: A typical absolute specification of a lowpass filter is shown in figure 1 where:
FIR FILTER DESIGN The design of an digital filte is caied out in thee steps: ) Specification: Befoe we can design a filte we must have some specifications. These ae detemined by the application. ) Appoximations
More informationEEO 401 Digital Signal Processing Prof. Mark Fowler
EEO 41 Digital Signal Pocessing Pof. Mak Fowle Note Set #31 Linea Phase FIR Design Optimum Equiipple (Paks-McClellan) Reading: Sect. 1.2.4 1.2.6 of Poakis & Manolakis 1/2 Motivation The window method and
More informationMulti-Objective Optimization Algorithms for Finite Element Model Updating
Multi-Objective Optimization Algoithms fo Finite Element Model Updating E. Ntotsios, C. Papadimitiou Univesity of Thessaly Geece Outline STRUCTURAL IDENTIFICATION USING MEASURED MODAL DATA Weighted Modal
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.
More informationConjugate Gradient Methods. Michael Bader. Summer term 2012
Gadient Methods Outlines Pat I: Quadatic Foms and Steepest Descent Pat II: Gadients Pat III: Summe tem 2012 Pat I: Quadatic Foms and Steepest Descent Outlines Pat I: Quadatic Foms and Steepest Descent
More informationTransverse Wakefield in a Dielectric Tube with Frequency Dependent Dielectric Constant
ARDB-378 Bob Siemann & Alex Chao /4/5 Page of 8 Tansvese Wakefield in a Dielectic Tube with Fequency Dependent Dielectic Constant This note is a continuation of ARDB-368 that is now extended to the tansvese
More informationME 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
More informationAn Electromagnetic Emission Model for Integrated Circuits
An Electomagnetic Emission Model fo Integated Cicuits Pete Kalicek FhG-IZM Padebon/Belin Univesity of Padebon Kalicek@ieee ieee.og 16 Mach 2001 Oveview Motivation/Intoduction Geneal Modeling Poposed Emission
More informationScientific Computing II
Scientific Computing II Conjugate Gadient Methods Michael Bade Summe 2014 Conjugate Gadient Methods, Summe 2014 1 Families of Iteative Solves elaxation methods: Jacobi-, Gauss-Seidel-Relaxation,... Ove-Relaxation-Methods
More informationPearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms
Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two
More informationTemporal-Difference Learning
.997 Decision-Making in Lage-Scale Systems Mach 17 MIT, Sping 004 Handout #17 Lectue Note 13 1 Tempoal-Diffeence Leaning We now conside the poblem of computing an appopiate paamete, so that, given an appoximation
More information1D2G - Numerical solution of the neutron diffusion equation
DG - Numeical solution of the neuton diffusion equation Y. Danon Daft: /6/09 Oveview A simple numeical solution of the neuton diffusion equation in one dimension and two enegy goups was implemented. Both
More informationA Power Method for Computing Square Roots of Complex Matrices
JOURNAL OF MATHEMATICAL ANALYSIS AND APPLICATIONS 13, 39345 1997 ARTICLE NO. AY975517 A Powe Method fo Computing Squae Roots of Complex Matices Mohammed A. Hasan Depatment of Electical Engineeing, Coloado
More informationMany Electron Atoms. Electrons can be put into approximate orbitals and the properties of the many electron systems can be catalogued
Many Electon Atoms The many body poblem cannot be solved analytically. We content ouselves with developing appoximate methods that can yield quite accuate esults (but usually equie a compute). The electons
More informationSwissmetro: design methods for ironless linear transformer
Swissmeto: design methods fo ionless linea tansfome Nicolas Macabey GESTE Engineeing SA Scientific Pak PSE-C, CH-05 Lausanne, Switzeland Tel (+4) 2 693 83 60, Fax. (+4) 2 693 83 6, nicolas.macabey@geste.ch
More informationFE FORMULATIONS FOR PLASTICITY
G These slides ae designed based on the book: Finite Elements in Plasticity Theoy and Pactice, D.R.J. Owen and E. Hinton, 970, Pineidge Pess Ltd., Swansea, UK. Couse Content: A INTRODUCTION AND OVERVIEW
More informationInformation Retrieval Advanced IR models. Luca Bondi
Advanced IR models Luca Bondi Advanced IR models 2 (LSI) Pobabilistic Latent Semantic Analysis (plsa) Vecto Space Model 3 Stating point: Vecto Space Model Documents and queies epesented as vectos in the
More informationStanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012
Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,
More informationGermán Sierra Instituto de Física Teórica CSIC-UAM, Madrid, Spain
Gemán Siea Instituto de Física Teóica CSIC-UAM, Madid, Spain Wo in pogess done in collaboation with J. Lins and S. Y. Zhao (Univ. Queensland, Austalia) and M. Ibañez (IFT, Madid) Taled pesented at the
More informationNumerical Inversion of the Abel Integral Equation using Homotopy Perturbation Method
Numeical Invesion of the Abel Integal Equation using Homotopy Petubation Method Sunil Kuma and Om P Singh Depatment of Applied Mathematics Institute of Technology Banaas Hindu Univesity Vaanasi -15 India
More informationGradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function
Intenational Confeence on Infomation echnology and Management Innovation (ICIMI 05) Gadient-based Neual Netwok fo Online Solution of Lyapunov Matix Equation with Li Activation unction Shiheng Wang, Shidong
More informationJ. Electrical Systems 1-3 (2005): Regular paper
K. Saii D. Rahem S. Saii A Miaoui Regula pape Coupled Analytical-Finite Element Methods fo Linea Electomagnetic Actuato Analysis JES Jounal of Electical Systems In this pape, a linea electomagnetic actuato
More informationModel and Controller Order Reduction for Infinite Dimensional Systems
IT J. Eng. Sci., Vol. 4, No.,, -6 Model and Contolle Ode Reduction fo Infinite Dimensional Systems Fatmawati,*, R. Saagih,. Riyanto 3 & Y. Soehayadi Industial and Financial Mathematics Goup email: fatma47@students.itb.ac.id;
More informationAnalytical calculation of the power dissipated in the LHC liner. Stefano De Santis - LBNL and Andrea Mostacci - CERN
Analytical calculation of the powe dissipated in the LHC line Stefano De Santis - LBNL and Andea Mostacci - CERN Contents What is the Modified Bethe s Diffaction Theoy? Some inteesting consequences of
More informationQuantum Mechanics II
Quantum Mechanics II Pof. Bois Altshule Apil 25, 2 Lectue 25 We have been dicussing the analytic popeties of the S-matix element. Remembe the adial wave function was u kl () = R kl () e ik iπl/2 S l (k)e
More informationHigh precision computer simulation of cyclotrons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D.
High pecision compute simulation of cyclotons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D. Abstact Effective and accuate compute simulations ae highly impotant in acceleatos design and poduction.
More informationModeling and Calculation of Optical Amplification in One Dimensional Case of Laser Medium Using Finite Difference Time Domain Method
Jounal of Physics: Confeence Seies PAPER OPEN ACCESS Modeling and Calculation of Optical Amplification in One Dimensional Case of Lase Medium Using Finite Diffeence Time Domain Method To cite this aticle:
More informationMethod for Approximating Irrational Numbers
Method fo Appoximating Iational Numbes Eic Reichwein Depatment of Physics Univesity of Califonia, Santa Cuz June 6, 0 Abstact I will put foth an algoithm fo poducing inceasingly accuate ational appoximations
More informationA Personal Perspective on Parameterized and Nonlinear MOR
A Pesonal Pespective on Paameteized and Nonlinea MOR J. White Slides thanks to D. Luca, M. Reichelt, M. Rewienski, D. Vasilyev Inteconnect Focus Cente e e e e A Multitechnology Phase-Locked Loop CN FE
More informationEquilibrium Reconstruction with Grad-Shafranov Equation
Equilibium Reconstuction with Gad-Shafanov Equation Qian Peng (qp215) Apil 14, 211 1 Gad-Shafanov equation [1]Fo axial symmetic case, the tooidal B eld is B to = F φ. Whee 2π F (, θ) is the total poloidal
More informationHammerstein Model Identification Based On Instrumental Variable and Least Square Methods
Intenational Jounal of Emeging Tends & Technology in Compute Science (IJETTCS) Volume 2, Issue, Januay Febuay 23 ISSN 2278-6856 Hammestein Model Identification Based On Instumental Vaiable and Least Squae
More informationNumerical Solution of Boundary Value Problems for the Laplacian in R 3 in the Case of Complex Boundary Surface
Computational Applied Mathematics Jounal 5; (: 9-5 Published online Febuay 5 (http://www.aascit.og/jounal/camj Numeical Solution of Bounday Value Poblems fo the Laplacian in R in the Case of Complex Bounday
More informationWeb-based Supplementary Materials for. Controlling False Discoveries in Multidimensional Directional Decisions, with
Web-based Supplementay Mateials fo Contolling False Discoveies in Multidimensional Diectional Decisions, with Applications to Gene Expession Data on Odeed Categoies Wenge Guo Biostatistics Banch, National
More informationContribution to the cavity model for analysis of microstrip patch antennas
JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS Vol. 8, No. 1, Febauy 006, p. 339-344 Contibution to the cavity model fo analysis of micostip patch antennas D. D. SANDU *, O. G. AVADANEI, A. IOACHIM
More informationDiscrete LQ optimal control with integral action: A simple controller on incremental form for MIMO systems
Modeling, Identification and Contol, Vol., No., 1, pp. 5, ISSN 189 18 Discete LQ optimal contol with integal action: A simple contolle on incemental fom fo MIMO systems David Di Ruscio Telemak Univesity
More informationInteraction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r)
Supplementay mateial fo Inteaction of Feedfowad and Feedback Steams in Visual Cotex in a Fiing-Rate Model of Columna Computations Tobias Bosch and Heiko Neumann Institute fo Neual Infomation Pocessing
More informationIntroduction to Orbital-Free Density-Functional Theory. Ralf Gehrke FHI Berlin, February 8th 2005
Intoduction to Obital-Fee Density-Functional heoy Ralf Gehke FHI Belin, Febuay 8th 005 Outline Basics of functional deivatives I Pinciples of Obital-fee Density-Functional heoy basics of Density-Functional
More information1 Spherical multipole moments
Jackson notes 9 Spheical multipole moments Suppose we have a chage distibution ρ (x) wheeallofthechageiscontained within a spheical egion of adius R, as shown in the diagam. Then thee is no chage in the
More informationAalborg Universitet. Load Estimation from Natural input Modal Analysis Aenlle, Manuel López; Brincker, Rune; Canteli, Alfonso Fernández
Aalbog Univesitet Load Estimation fom atual input Modal Analysis Aenlle, Manuel López; Bincke, Rune; Canteli, Alfonso Fenández Published in: Confeence Poceedings Publication date: 005 Document Vesion Publishe's
More informationA FURTHER SUBSPACE METHOD OPTIMIZATION FOR TRACKING REAL VALUED SINUSOIDS IN NOISE
Électonique et tansmission de l infomation A FURHER SUBSPACE MEHOD OPIMIZAION FOR RACKING REAL VALUED SINUSOIDS IN NOISE ŞEFAN SLAVNICU, SILVIU CIOCHINĂ Key wods: Subspace tacking, Fequency estimation,
More informationLocalization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matrix
Jounal of Sciences, Islamic Republic of Ian (): - () Univesity of Tehan, ISSN - http://sciencesutaci Localization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matix H Ahsani
More informationEKT 356 MICROWAVE COMMUNICATIONS CHAPTER 2: PLANAR TRANSMISSION LINES
EKT 356 MICROWAVE COMMUNICATIONS 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
More informationCoupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials
Coupled Electomagnetic and Heat Tansfe Simulations fo RF Applicato Design fo Efficient Heating of Mateials Jeni Anto 1 and Raj C Thiagaajan 2 * 1 Reseache, Anna Univesity, Chennai, 2 ATOA Scientific Technologies
More informationElectron Density Distribution in HSX
Electon Density Distibution in HSX C. Deng, D.L. Bowe Electical Engineeing Depatment Univesity of Califonia, Los Angeles J. Canik, S.P. Gehadt, D.T. Andeson, P. Pobet, F.S.B. Andeson The HSX Plasma Laboatoy
More informationHow to Obtain Desirable Transfer Functions in MIMO Systems Under Internal Stability Using Open and Closed Loop Control
How to Obtain Desiable ansfe Functions in MIMO Sstems Unde Intenal Stabilit Using Open and losed Loop ontol echnical Repot of the ISIS Goup at the Univesit of Note Dame ISIS-03-006 June, 03 Panos J. Antsaklis
More informationA Relativistic Electron in a Coulomb Potential
A Relativistic Electon in a Coulomb Potential Alfed Whitehead Physics 518, Fall 009 The Poblem Solve the Diac Equation fo an electon in a Coulomb potential. Identify the conseved quantum numbes. Specify
More informationCalculating Frequency-Dependent Inductance of VLSI Interconnect by Complete Multiple Reciprocity Boundary Element Method
Calculating Fequency-Dependent Inductance of VLSI Inteconnect by Complete Multiple Recipocity Bounday Element Method Changhao Yan Wenjian Yu Zeyi Wang Dept. of Comp. Sci. & Tech. Dept. of Comp. Sci. &
More information{ } ( ) ( ) ( 1 ( ) π 2. Trapezoidal rule: a ( ) ( ) Simpson rule: 3/8 Simpson rule: Boole's rule a ( ) ( ) ( ) ( + ) 45 Weddle's Rule Hardy's rule:
L. Yaoslavsy. Selected Topics in Image Pocessing Pat. Fast tansfom methods fo image esampling Lect. 5. Pecise numeical integation and eentiation Conventional numeical integation methods: T T T = S S S
More informationMAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS
The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD
More informationHQuad: Statistics of Hamiltonian Cycles in Wireless Rechargeable Sensor Networks
HQuad: Statistics of Hamiltonian Cycles in Wieless Rechageable Senso Netwoks Yanmao Man Dept. of ECE Univesity of Aizona Tucson, AZ, U.S.A. yman@email.aizona.edu Jing Deng Dept. of CS UNC at Geensboo Geensboo,
More informationCourse Outline. ECE 178: Image Processing REVIEW. Relationship between pixels. Connected components. Distance Measures. Linear systems-review
ECE 78: Image Pocessing REVIEW Lectue #2 Mach 3, 23 Couse Outline! Intoduction! Digital Images! Image Tansfoms! Sampling and Quantization! Image Enhancement! Image/Video Coding JPEG MPEG Mach 3, 23 Mach
More informationDirected Regression. Benjamin Van Roy Stanford University Stanford, CA Abstract
Diected Regession Yi-hao Kao Stanfod Univesity Stanfod, CA 94305 yihaoao@stanfod.edu Benjamin Van Roy Stanfod Univesity Stanfod, CA 94305 bv@stanfod.edu Xiang Yan Stanfod Univesity Stanfod, CA 94305 xyan@stanfod.edu
More informationAn Adaptive Neural-Network Model-Following Speed Control of PMSM Drives for Electric Vehicle Applications
Poceedings of the 9th WSEAS Intenational Confeence on Applied Mathematics, Istanbul, Tuey, May 27-29, 2006 (pp412-417) An Adaptive Neual-Netwo Model-Following Speed Contol of PMSM Dives fo Electic Vehicle
More informationCoarse Mesh Radiation Transport Code COMET Radiation Therapy Application*
Coase Mesh Radiation Tanspot Code COMT Radiation Theapy Application* Fazad Rahnema Nuclea & Radiological ngineeing and Medical Physics Pogams Geogia Institute of Technology Computational Medical Physics
More informationsinγ(h y > ) exp(iωt iqx)dωdq
Lectue 9/28/5 Can we ecove a ay pictue fom the above G fo a membane stip? Such a pictue would be complementay to the above expansion in a seies of integals along the many banches of the dispesion elation.
More informationIn the previous section we considered problems where the
5.4 Hydodynamically Fully Developed and Themally Developing Lamina Flow In the pevious section we consideed poblems whee the velocity and tempeatue pofile wee fully developed, so that the heat tansfe coefficient
More informationGENLOG Multinomial Loglinear and Logit Models
GENLOG Multinomial Loglinea and Logit Models Notation This chapte descibes the algoithms used to calculate maximum-likelihood estimates fo the multinomial loglinea model and the multinomial logit model.
More informationEKT 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
More informationHydroelastic Analysis of a 1900 TEU Container Ship Using Finite Element and Boundary Element Methods
TEAM 2007, Sept. 10-13, 2007,Yokohama, Japan Hydoelastic Analysis of a 1900 TEU Containe Ship Using Finite Element and Bounday Element Methods Ahmet Egin 1)*, Levent Kaydıhan 2) and Bahadı Uğulu 3) 1)
More informationCOUPLED MODELS OF ROLLING, SLIDING AND WHIRLING FRICTION
ENOC 008 Saint Petesbug Russia June 30-July 4 008 COUPLED MODELS OF ROLLING SLIDING AND WHIRLING FRICTION Alexey Kieenkov Ins ti tu te fo P ob le ms in Me ch an ic s Ru ss ia n Ac ad em y of Sc ie nc es
More informationExperiment 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
More informationASTR415: Problem Set #6
ASTR45: Poblem Set #6 Cuan D. Muhlbege Univesity of Mayland (Dated: May 7, 27) Using existing implementations of the leapfog and Runge-Kutta methods fo solving coupled odinay diffeential equations, seveal
More informationGoodness-of-fit for composite hypotheses.
Section 11 Goodness-of-fit fo composite hypotheses. Example. Let us conside a Matlab example. Let us geneate 50 obsevations fom N(1, 2): X=nomnd(1,2,50,1); Then, unning a chi-squaed goodness-of-fit test
More informationIdentification of the degradation of railway ballast under a concrete sleeper
Identification of the degadation of ailway ballast unde a concete sleepe Qin Hu 1) and Heung Fai Lam ) 1), ) Depatment of Civil and Achitectual Engineeing, City Univesity of Hong Kong, Hong Kong SAR, China.
More informationINVESTIGATION OF THE OPERATIONAL MODAL ANALYSIS APPLICABILITY IN COMBUSTION ENGINE DIAGNOSTICS
INVESTIGATION OF THE OPERATIONAL MODAL ANALYSIS APPLICABILITY IN COMBUSTION ENGINE DIAGNOSTICS Macin Łukasiewicz Univesity of Technology and Life Science ul. S. Kaliskiego 7, 85-789 Bydgoszcz, Poland tel.:
More informationPhysics 221 Lecture 41 Nonlinear Absorption and Refraction
Physics 221 Lectue 41 Nonlinea Absoption and Refaction Refeences Meye-Aendt, pp. 97-98. Boyd, Nonlinea Optics, 1.4 Yaiv, Optical Waves in Cystals, p. 22 (Table of cystal symmeties) 1. Intoductoy Remaks.
More informationAnalysis and Optimization of a Special Type of Dielectric Loaded Resonant Cavity for Mobile Communication Filters
328 Analysis and Optimization of a Special Type of Dielectic Loaded Resonant Cavity fo Mobile Communication Filtes Haold S. Showes, Banmali S. Rawat *, Syam S. Challa Depatment of Electical and Biomedical
More informationAPPLICATION OF MAC IN THE FREQUENCY DOMAIN
PPLICION OF MC IN HE FREQUENCY DOMIN D. Fotsch and D. J. Ewins Dynamics Section, Mechanical Engineeing Depatment Impeial College of Science, echnology and Medicine London SW7 2B, United Kingdom BSRC he
More informationImplicit Constraint Enforcement for Rigid Body Dynamic Simulation
Implicit Constaint Enfocement fo Rigid Body Dynamic Simulation Min Hong 1, Samuel Welch, John app, and Min-Hyung Choi 3 1 Division of Compute Science and Engineeing, Soonchunhyang Univesity, 646 Eupnae-i
More informationMultiple Experts with Binary Features
Multiple Expets with Binay Featues Ye Jin & Lingen Zhang Decembe 9, 2010 1 Intoduction Ou intuition fo the poect comes fom the pape Supevised Leaning fom Multiple Expets: Whom to tust when eveyone lies
More informationResidual Modes on Non-linear Resonant Decay Method
Residual Modes on Non-linea Resonant Decay Method D Mehdi Samast, Pofesso Jan R. Wight ABSRAC Non-linea Resonant Decay method (NL-RDM) addesses the identification of multi-degee of feedom non-linea systems.
More informationConventional 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
More informationTECHNICAL SIMULATIONS AND MEASUREMENTS OF CAGE-SWITCHING AT THE INDUCTION MACHINE. Tulbure Adrian*, Risteiu Mircea**
TECHNICAL SIMULATIONS AND MEASUREMENTS OF CAGE-SWITCHING AT THE INDUCTION MACHINE Tulbue Adian*, Risteiu Micea** * Univesity of Petosani ** Univesity 1 Decembie 1918 Alba-Iulia Abstact: In the pesent pape
More informationValidation of Closed Loop Degaussing System for Double Hull Submarines
Validation of Closed Loop Degaussing System fo Double Hull Submaines L. Demilie 1, G. Cauffet 2, O. Chadebec 2, J.L. Coulomb 2, L.L. Rouve 2 1 DCNS, 2 ue Sextius Michel, 75732 Pais cedex 15, Fance. lauent.demilie@dcnsgoup.com
More informationDescription of TEAM Workshop Problem 33.b: Experimental Validation of Electric Local Force Formulations.
1 Desciption of TEAM Wokshop Poblem 33.b: Expeimental Validation of Electic Local Foce Fomulations. Olivie Baé, Pascal Bochet, Membe, IEEE Abstact Unde extenal stesses, the esponse of any mateial is a
More informationDymore User s Manual Two- and three dimensional dynamic inflow models
Dymoe Use s Manual Two- and thee dimensional dynamic inflow models Contents 1 Two-dimensional finite-state genealized dynamic wake theoy 1 Thee-dimensional finite-state genealized dynamic wake theoy 1
More informationPROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.
POBLM S # SOLUIONS by obet A. DiStasio J. Q. he Bon-Oppenheime appoximation is the standad way of appoximating the gound state of a molecula system. Wite down the conditions that detemine the tonic and
More informationAN EMBEDDED SEMI-ANALYTICAL BENCHMARK VIA ITERATIVE INTERPOLATION FOR NEUTRON TRANSPORT METHODS VERIFICATION
AN EMBEDDED SEMI-ANAYTICA BENCHMARK VIA ITERATIVE INTERPOATION FOR NEUTRON TRANSPORT METHODS VERIFICATION B. D. Ganapol Depatment of Aeospace and Mechanical Engineeing Univesity of Aizona Ganapol@cowboy.ame.aizona
More informationState tracking control for Takagi-Sugeno models
State tacing contol fo Taagi-Sugeno models Souad Bezzaoucha, Benoît Max,3,DidieMaquin,3 and José Ragot,3 Abstact This wo addesses the model efeence tacing contol poblem It aims to highlight the encouteed
More informationDIMENSIONALITY LOSS IN MIMO COMMUNICATION SYSTEMS
DIMENSIONALITY LOSS IN MIMO COMMUNICATION SYSTEMS Segey Loya, Amma Koui School of Infomation Technology and Engineeing (SITE) Univesity of Ottawa, 6 Louis Pasteu, Ottawa, Ontaio, Canada, KN 6N5 Email:
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electical and Compute Engineeing, Conell Univesity ECE 33: Electomagnetic Fields and Waves Fall 7 Homewok 6 Due on Oct. 5, 7 by 5: PM Reading Assignments: i) Review the lectue notes. ii) Review
More information11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.
Fall 2007 Qualifie Pat II 12 minute questions 11) A thin, unifom od of mass M is suppoted by two vetical stings, as shown below. Find the tension in the emaining sting immediately afte one of the stings
More informationReconstruction of 3D Anisotropic Objects by VIE and Model-Based Inversion Methods
Pogess In Electomagnetics Reseach C, Vol. 8, 97, 08 Reconstuction of D Anisotopic Objects by VIE and Model-Based Invesion Methods Lin E. Sun, * and Mei Song Tong Abstact A model-based invesion algoithm
More informationSEARCH-BASED DYNAMIC IDENTIFICATION OF INDUCTION MOTORS
SEARCH-BASED DYNAMIC IDENTIFICATION OF INDUCTION MOTORS Alexande Vladimiovich Nesteovskiy Veniamin Geogievich ashiskikh Valey Mihailovich Zavyalov and Iina Yuyevna Semykina uzbass State Technical Univesity
More informationSolutions. 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
More informationImplementation of RCWA
Instucto D. Ramond Rumpf (915) 747 6958 cumpf@utep.edu EE 5337 Computational Electomagnetics Lectue # Implementation of RCWA Lectue These notes ma contain copighted mateial obtained unde fai use ules.
More informationCOMP Parallel Computing SMM (3) OpenMP Case Study: The Barnes-Hut N-body Algorithm
COMP 633 - Paallel Computing Lectue 8 Septembe 14, 2017 SMM (3) OpenMP Case Study: The Banes-Hut N-body Algoithm Topics Case study: the Banes-Hut algoithm Study an impotant algoithm in scientific computing»
More informationMutual impedance between linear elements: The induced EMF method. Persa Kyritsi September 29th, 2005 FRB7, A1-104
Mutual impedance between linea elements: The induced EMF method Septembe 9th, 5 FRB7, A-4 Outline Septembe 9, 5 Reminde: self impedance nduced EMF method Nea-field of a dipole Self impedance vs. Mutual
More informationGreen s function Monte Carlo algorithms for elliptic problems
Mathematics and Computes in Simulation 63 (2003) 587 604 Geen s function Monte Calo algoithms fo elliptic poblems I.T. Dimov, R.Y. Papancheva Cental Laboatoy fo Paallel Pocessing, Depatment of Paallel
More informationSimulation and Discretization of Fractional Order Systems
Simulation and Discetization of Factional Ode Systems Mohamad Adnan Depatment of Electical and Compute Engineeing, Ameican Univesity of Beiut, Beiut, Lebanon Abstact - This wok deals with the simulation
More informationChapter 3 Optical Systems with Annular Pupils
Chapte 3 Optical Systems with Annula Pupils 3 INTRODUCTION In this chapte, we discuss the imaging popeties of a system with an annula pupil in a manne simila to those fo a system with a cicula pupil The
More informationCENTER FOR MULTIMODAL SOLUTIONS FOR CONGESTION MITIGATION (CMS)
Final Repot to the CENTER FOR MULTIMODAL SOLUTIONS FOR CONGESTION MITIGATION (CMS) CMS Poect Numbe: _8-4_ Title: Chaacteizing the Tadeoffs and Costs Associated with Tanspotation Congestion in Supply Chains
More informationSupporting Information Wedge Dyakonov Waves and Dyakonov Plasmons in Topological Insulator Bi 2 Se 3 Probed by Electron Beams
Suppoting Infomation Wedge Dyakonov Waves and Dyakonov Plasmons in Topological Insulato Bi 2 Se 3 Pobed by Electon Beams Nahid Talebi, Cigdem Osoy-Keskinboa, Hadj M. Benia, Klaus Ken, Chistoph T. Koch,
More informationIN SITU SOUND ABSORPTION COEFFICIENT MEASUREMENT OF VARIOUS SURFACES
IN SITU SOUND ABSORPTION COEFFICIENT MEASUREMENT OF VARIOUS SURFACES PACS REFERENCES : 43.20.El, 43.20.Ye, 43.55.Ev, 43.58.Bh Michel Béengie 1 ; Massimo Gaai 2 1 Laboatoie Cental des Ponts et Chaussées
More informationA NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM
Poceedings of the ASME 2010 Intenational Design Engineeing Technical Confeences & Computes and Infomation in Engineeing Confeence IDETC/CIE 2010 August 15-18, 2010, Monteal, Quebec, Canada DETC2010-28496
More informationA Simulator for High-Speed Backplane Transceivers
UKSim 29: th Intenational Confeence on Compute Modelling and Simulation A Simulato fo High-Speed Backplane Tansceives Dianyong Chen, Bo Wang, Bangli Liang, and Tad Kwasniewski Depatment of Electonics,
More informationBasic Bridge Circuits
AN7 Datafoth Copoation Page of 6 DID YOU KNOW? Samuel Hunte Chistie (784-865) was bon in London the son of James Chistie, who founded Chistie's Fine At Auctionees. Samuel studied mathematics at Tinity
More informationPower efficiency and optimum load formulas on RF rectifiers featuring flow-angle equations
LETTE IEICE Electonics Expess, Vol.10, No.11, 1 9 Powe efficiency and optimum load fomulas on F ectifies featuing flow-angle equations Takashi Ohia a) Toyohashi Univesity of Technology, 1 1 Hibaigaoka,
More informationSecret Exponent Attacks on RSA-type Schemes with Moduli N = p r q
Secet Exponent Attacks on RSA-type Schemes with Moduli N = p q Alexande May Faculty of Compute Science, Electical Engineeing and Mathematics Univesity of Padebon 33102 Padebon, Gemany alexx@uni-padebon.de
More informationChapter Introduction to Finite Element Methods
Chapte 1.4 Intoduction to Finite Element Methods Afte eading this chapte, you should e ale to: 1. Undestand the asics of finite element methods using a one-dimensional polem. In the last fifty yeas, the
More information