Efficient Simulation for Strongly Coupled Noise- Vibration-Harshness (NVH) R. S. Puri, D. Morrey, Oxford Brooks E. B.

Size: px
Start display at page:

Download "Efficient Simulation for Strongly Coupled Noise- Vibration-Harshness (NVH) R. S. Puri, D. Morrey, Oxford Brooks E. B."

Transcription

1 Efficient Simulation for Strongly Coupled Noie- Vibration-Harhne (NVH) R. S. Puri, D. Morrey, Oxford Brook E. B. Rudnyi, CADFEM

2 Background Joint work 24- Over Available online ModelReduction.com/ contrib/srinivaan.puri/ 1

3 NVH Simulation Low Frequency Mid Frequency High Frequency Structure borne Structure and air borne Air born 1 Hz 1 25 Hz > 25 Hz 2

4 3 Fully Coupled Finite Element Dicretization FLUID29/FLUID3 in ANSYS The element ize hould be maller than wavelength High dimenional model Unymmetric matrice = + + a a f a a f F F p u K K K C C j M M M 2 ω ω

5 Model Order Reduction Relatively new technology Solid mathematical background: Approximation of large cale dynamic ytem Dynamic imulation: Harmonic or tranient imulation Indutry application level: Linear dynamic ytem only 4

6 From Finite Element to Sytem Simulation Phyic & Geometry FEM Sytem of n ODE MOR Reduced Sytem of r << n ODE SCOPE1 + V1 6 - h3 l3 h1 h2 h3 h4 SCOPE2 5Hz h1 l1 h2 l2 h3 l3 h2 l2 h5 h6 h7 h8 h9 h1 h11 h12 h13 h14 h1 l1 h15 h16 h17 h18 h19 h2 h21 h22 h23 h24 h25 h26 h27 h28 h29 h3 Electrothermal Simulation with IGBT: From ANSYS Workbench to Capoc (Euroime 28) FILENAME FILENAME1 D:\capoc23\SomeProject\mor\MOR3Input\mor 5

7 Model Reduction a Projection Projection onto lowdimenional ubpace E x& + Kx = Bu x = Vz + ε E z V T EVz& + V T KVz = V T Bu x = V How to find ubpace? Mode uperpoition i not the bet way to do it. E r 6

8 Implicit Moment Matching Padé approximation Matching firt moment for the tranfer function H ( ) = E x& + Kx = Bu 1 ( E + K ) B H H red = m ( ) i i = m ( i i, red ) m i = m i,red, i =,K,r Implicit Moment Matching: via Krylov Subpace = V = pan{i(k 1 E,K 1 b)} 7

9 MOR for ANSYS: ANSYS Model Simulink, Capoc, Simplorer, VerilogA, FULL file Small dimenional matrice Mx &&+ Ex& + Kx y = Cx = Bu Linear Dynamic Sytem, ODE MOR Algorithm Current verion 2.5 8

10 Electrothermal Simulation of IGBT SCOPE1 Euroime 28, Daimler, imulation with CASPOC + V1 6 - h3 l3 SCOPE2 h1 h1 l1 h2 l2 h3 l3 D D D D D D D D D h2 h3 5Hz VDC + - D D D D D D D D D h2 h4 h5 h6 h7 l2 h8 h9 h1 h11 h12 h13 h14 h1 h15 h16 l1 h17 h18 h19 h2 h21 h22 h23 h24 h25 h26 h27 h28 h29 h3 9 FILENAME FILENAME1 D:\capoc23\SomeProject\mor\MOR3Input\mor

11 HDD actuator and upenion ytem Prof J. S. Han. Tranaction of the KSME, A, Vol. 31, No. 5, pp , 27. 1

12 11 Piezoelectric Angular Rate Senor with Corioli Effect Prof J. S. Han, KSME 28. = + + l f V u K K K K V u E V u M d z T z & & && &&

13 Piezoelectric Angular Rate Senor with Corioli Effect 12

14 Model Reduction a Fat Solver Simulation of the reduced model i a few econd. Arnoldi Proce i fat: Tranient and harmonic repone analyi for the cot comparable with that of a tatic olution. It i advantageou to ue MOR even the reduced model i ued only once: Deign, Geometry optimization. 13

15 NVH Benchmark in Thei The 2D Acid-Tet 3D Plate backed air filled cavity 3D Plate backed Rectangular Water Filled Cavity Cylinder encloing an air-filled cavity Demontrator Structure: Adheive Bonded Joint 14

16 Adheive Bonded Joint Benchmark Mechanical Structure - SHELL181 Adheive SOLID45 Fluid FLUID3 Single excitation point Global and local damping 15

17 Comparion 16

18 Comparion Relative Error 17

19 18 Error Indicator True Error Error Indicator ) ( ) ( ) ( ) ( H H H E r r = ) ( ) ( ) ( ) ( ˆ 1 H H H E r r r r + = ) ( ˆ ) ( E E r r

20 Timing Problem in ANSYS element, node, free DoF Full olution in ANSYS for 2 frequencie hour 83 per frequency Proportional to the number of frequencie MOR for ANSYS Reading ANSYS file 3 Model reduction 17 Proportional to the number of vector Simulation of the reduced model 4 19

21 NVH Optimization 2

22 NVH Vibro-Acoutic Optimization SHELL181 to model the layered compoite Stack of eight layer To find optimal lamination 21

23 Fluid Structure Interaction at Acoutic Level 22 By courtey of Voith Siemen Hydro Power Generation GmbH & Co. KG

24 Concluion Model reduction i an excellent tool to peed up NVH imulation Software for ANSYS i available: MOR for ANSYS More information: 23

Efficient Simulation for Strongly Coupled Noise-Vibration- Harshness (NVH)

Efficient Simulation for Strongly Coupled Noise-Vibration- Harshness (NVH) Efficient Simulation for Strongly Coupled Noise-Vibration- Harshness (NVH) R. S. Puri, D. Morrey School of Technology, Oxford Brookes University, Wheatley Campus, Wheatley, Oxford OX33 1HX, United Kingdom,

More information

EE 4443/5329. LAB 3: Control of Industrial Systems. Simulation and Hardware Control (PID Design) The Inverted Pendulum. (ECP Systems-Model: 505)

EE 4443/5329. LAB 3: Control of Industrial Systems. Simulation and Hardware Control (PID Design) The Inverted Pendulum. (ECP Systems-Model: 505) EE 4443/5329 LAB 3: Control of Indutrial Sytem Simulation and Hardware Control (PID Deign) The Inverted Pendulum (ECP Sytem-Model: 505) Compiled by: Nitin Swamy Email: nwamy@lakehore.uta.edu Email: okuljaca@lakehore.uta.edu

More information

Fluid-structure coupling analysis and simulation of viscosity effect. on Coriolis mass flowmeter

Fluid-structure coupling analysis and simulation of viscosity effect. on Coriolis mass flowmeter APCOM & ISCM 11-14 th December, 2013, Singapore luid-tructure coupling analyi and imulation of vicoity effect on Corioli ma flowmeter *Luo Rongmo, and Wu Jian National Metrology Centre, A*STAR, 1 Science

More information

Behavioral thermal modeling for quad-core microprocessors

Behavioral thermal modeling for quad-core microprocessors Behavioral thermal modeling for quad-core microproceor Duo Li and Sheldon X.-D. Tan Department of Electrical Engineering Univerity of California, Riveride, CA Murli Tirumala Intel Corporation Outline Introduction

More information

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get Lecture 25 Introduction to Some Matlab c2d Code in Relation to Sampled Sytem here are many way to convert a continuou time function, { h( t) ; t [0, )} into a dicrete time function { h ( k) ; k {0,,, }}

More information

( 1) EE 313 Linear Signals & Systems (Fall 2018) Solution Set for Homework #10 on Laplace Transforms

( 1) EE 313 Linear Signals & Systems (Fall 2018) Solution Set for Homework #10 on Laplace Transforms EE 33 Linear Signal & Sytem (Fall 08) Solution Set for Homework #0 on Laplace Tranform By: Mr. Houhang Salimian & Prof. Brian L. Evan Problem. a) xt () = ut () ut ( ) From lecture Lut { ()} = and { } t

More information

NONLINEAR CONTROLLER DESIGN FOR A SHELL AND TUBE HEAT EXCHANGER AN EXPERIMENTATION APPROACH

NONLINEAR CONTROLLER DESIGN FOR A SHELL AND TUBE HEAT EXCHANGER AN EXPERIMENTATION APPROACH International Journal of Electrical, Electronic and Data Communication, ISSN: 232-284 Volume-3, Iue-8, Aug.-25 NONLINEAR CONTROLLER DESIGN FOR A SHELL AND TUBE HEAT EXCHANGER AN EXPERIMENTATION APPROACH

More information

Lecture 8. PID control. Industrial process control ( today) PID control. Insights about PID actions

Lecture 8. PID control. Industrial process control ( today) PID control. Insights about PID actions Lecture 8. PID control. The role of P, I, and D action 2. PID tuning Indutrial proce control (92... today) Feedback control i ued to improve the proce performance: tatic performance: for contant reference,

More information

S_LOOP: SINGLE-LOOP FEEDBACK CONTROL SYSTEM ANALYSIS

S_LOOP: SINGLE-LOOP FEEDBACK CONTROL SYSTEM ANALYSIS S_LOOP: SINGLE-LOOP FEEDBACK CONTROL SYSTEM ANALYSIS by Michelle Gretzinger, Daniel Zyngier and Thoma Marlin INTRODUCTION One of the challenge to the engineer learning proce control i relating theoretical

More information

A Compensated Acoustic Actuator for Systems with Strong Dynamic Pressure Coupling

A Compensated Acoustic Actuator for Systems with Strong Dynamic Pressure Coupling A Compenated Acoutic Actuator for Sytem with Strong Dynamic Preure Coupling Submitted to ASME Journal of Vibration and Acoutic July.997 Charle Birdong and Clark J. Radcliffe Department of Mechanical Engineering

More information

State Space: Observer Design Lecture 11

State Space: Observer Design Lecture 11 State Space: Oberver Deign Lecture Advanced Control Sytem Dr Eyad Radwan Dr Eyad Radwan/ACS/ State Space-L Controller deign relie upon acce to the tate variable for feedback through adjutable gain. Thi

More information

Non-stationary Random Vibration Analysis of Vehicle with Fractional

Non-stationary Random Vibration Analysis of Vehicle with Fractional 13 th National Conference on Mechanim and Machine (NaCoMM7), IISc, Bangalore, India, December 1-13, 7 NaCoMM-7-77 Non-tationary Random Vibration Analyi of Vehicle with Fractional Damping Yunqing Zhang

More information

ME 375 EXAM #1 Tuesday February 21, 2006

ME 375 EXAM #1 Tuesday February 21, 2006 ME 375 EXAM #1 Tueday February 1, 006 Diviion Adam 11:30 / Savran :30 (circle one) Name Intruction (1) Thi i a cloed book examination, but you are allowed one 8.5x11 crib heet. () You have one hour to

More information

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL 98 CHAPTER DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL INTRODUCTION The deign of ytem uing tate pace model for the deign i called a modern control deign and it i

More information

ME 375 FINAL EXAM Wednesday, May 6, 2009

ME 375 FINAL EXAM Wednesday, May 6, 2009 ME 375 FINAL EXAM Wedneday, May 6, 9 Diviion Meckl :3 / Adam :3 (circle one) Name_ Intruction () Thi i a cloed book examination, but you are allowed three ingle-ided 8.5 crib heet. A calculator i NOT allowed.

More information

Exercises for lectures 20 Digital Control

Exercises for lectures 20 Digital Control Exercie for lecture 0 Digital Control Micael Šebek Automatic control 06-4- Sampling: and z relationip for complex pole Continuou ignal Laplace tranform wit pole Dicrete ignal z-tranform, t y( t) e in t,

More information

Quantifying And Specifying The Dynamic Response Of Flowmeters

Quantifying And Specifying The Dynamic Response Of Flowmeters White Paper Quantifying And Specifying The Dynamic Repone Of Flowmeter DP Flow ABSTRACT The dynamic repone characteritic of flowmeter are often incompletely or incorrectly pecified. Thi i often the reult

More information

INTER-NOISE DECEMBER 2006 HONOLULU, HAWAII, USA

INTER-NOISE DECEMBER 2006 HONOLULU, HAWAII, USA INTER-NOISE 2006 3-6 DECEMBER 2006 HONOLULU, HAWAII, USA Krylov Subspace Techniques for Low Frequency Structural Acoustic Analysis and Optimization R Srinivasan Puri a, Denise Morrey a Andrew Bell a, John

More information

Finite Element Analysis of a Fiber Bragg Grating Accelerometer for Performance Optimization

Finite Element Analysis of a Fiber Bragg Grating Accelerometer for Performance Optimization Finite Element Analyi of a Fiber Bragg Grating Accelerometer for Performance Optimization N. Baumallick*, P. Biwa, K. Dagupta and S. Bandyopadhyay Fiber Optic Laboratory, Central Gla and Ceramic Reearch

More information

A new method for the dynamical symulation of mechanical systems using Matlab-Simulink

A new method for the dynamical symulation of mechanical systems using Matlab-Simulink Copyright 2010 ICCES ICCES, vol.14, no.1, pp.23-28 A new method for the dynamical ymulation of mechanical ytem uing Matlab-Simulink Dǎnuţ Receanu 1, Emil Budecu 1 Summary The paper preent a new method

More information

Advanced Digital Signal Processing. Stationary/nonstationary signals. Time-Frequency Analysis... Some nonstationary signals. Time-Frequency Analysis

Advanced Digital Signal Processing. Stationary/nonstationary signals. Time-Frequency Analysis... Some nonstationary signals. Time-Frequency Analysis Advanced Digital ignal Proceing Prof. Nizamettin AYDIN naydin@yildiz.edu.tr Time-Frequency Analyi http://www.yildiz.edu.tr/~naydin 2 tationary/nontationary ignal Time-Frequency Analyi Fourier Tranform

More information

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.1 INTRODUCTION 8.2 REDUCED ORDER MODEL DESIGN FOR LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.3

More information

Control Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax:

Control Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax: Control Sytem Engineering ( Chapter 7. Steady-State Error Prof. Kwang-Chun Ho kwangho@hanung.ac.kr Tel: 0-760-453 Fax:0-760-4435 Introduction In thi leon, you will learn the following : How to find the

More information

LOAD FREQUENCY CONTROL OF MULTI AREA INTERCONNECTED SYSTEM WITH TCPS AND DIVERSE SOURCES OF POWER GENERATION

LOAD FREQUENCY CONTROL OF MULTI AREA INTERCONNECTED SYSTEM WITH TCPS AND DIVERSE SOURCES OF POWER GENERATION G.J. E.D.T.,Vol.(6:93 (NovemberDecember, 03 ISSN: 39 793 LOAD FREQUENCY CONTROL OF MULTI AREA INTERCONNECTED SYSTEM WITH TCPS AND DIVERSE SOURCES OF POWER GENERATION C.Srinivaa Rao Dept. of EEE, G.Pullaiah

More information

Stability. ME 344/144L Prof. R.G. Longoria Dynamic Systems and Controls/Lab. Department of Mechanical Engineering The University of Texas at Austin

Stability. ME 344/144L Prof. R.G. Longoria Dynamic Systems and Controls/Lab. Department of Mechanical Engineering The University of Texas at Austin Stability The tability of a ytem refer to it ability or tendency to eek a condition of tatic equilibrium after it ha been diturbed. If given a mall perturbation from the equilibrium, it i table if it return.

More information

MM1: Basic Concept (I): System and its Variables

MM1: Basic Concept (I): System and its Variables MM1: Baic Concept (I): Sytem and it Variable A ytem i a collection of component which are coordinated together to perform a function Sytem interact with their environment. The interaction i defined in

More information

Automatic Order Reduction for Finite Element Models

Automatic Order Reduction for Finite Element Models Automatic Order Reduction for Finite Element Models Andreas Greiner, Jan Lienemann, Evgenii Rudnyi, and Jan G. Korvink IMTEK, Albert-Ludwigs-Universität Freiburg Geroges-Köhler-Allee 103, D-79110 Freiburg,

More information

Model Order Reduction for Battery Simulation. Xiao Hu, PhD Confidence by Design Detroit June 5, 2012

Model Order Reduction for Battery Simulation. Xiao Hu, PhD Confidence by Design Detroit June 5, 2012 Model Order Reduction for Battery Simulation Xiao Hu, PhD Confidence by Design Detroit June 5, 202 Outline ANSYS model order reduction (MOR) technique Different types of battery simulation Transfer function

More information

Efficient Electrothermal Simulation of Power Electronics for Hybrid Electric Vehicle

Efficient Electrothermal Simulation of Power Electronics for Hybrid Electric Vehicle Efficient Electrothermal Simulation of Power Electronics for Hybrid Electric Vehicle Anis ehbi, Wolfgang Wondrak, aimler AG, GR & AE Cabin and Powertrain E/E, anis.dehbi@daimler.com Evgenii B. Rudnyi,

More information

Lecture 4. Chapter 11 Nise. Controller Design via Frequency Response. G. Hovland 2004

Lecture 4. Chapter 11 Nise. Controller Design via Frequency Response. G. Hovland 2004 METR4200 Advanced Control Lecture 4 Chapter Nie Controller Deign via Frequency Repone G. Hovland 2004 Deign Goal Tranient repone via imple gain adjutment Cacade compenator to improve teady-tate error Cacade

More information

Lecture 8 - SISO Loop Design

Lecture 8 - SISO Loop Design Lecture 8 - SISO Loop Deign Deign approache, given pec Loophaping: in-band and out-of-band pec Fundamental deign limitation for the loop Gorinevky Control Engineering 8-1 Modern Control Theory Appy reult

More information

Simulation Study on the Shock Properties of the Double-Degree-of-Freedom Cushioning Packaging System

Simulation Study on the Shock Properties of the Double-Degree-of-Freedom Cushioning Packaging System Proceeding of the 7th IAPRI World Conference on Packaging Simulation Study on the Shock Propertie of the Double-Degree-of-Freedom Cuhioning Packaging Sytem Xia Zhu, Qiaoqiao Yan, Xiaoling Yao, Junbin Chen,

More information

Online supplementary information

Online supplementary information Electronic Supplementary Material (ESI) for Soft Matter. Thi journal i The Royal Society of Chemitry 15 Online upplementary information Governing Equation For the vicou flow, we aume that the liquid thickne

More information

University R & D Session. KAIST Activities

University R & D Session. KAIST Activities Univerity R & D Seion KAIST Activitie 016. 3. 30 Jeong IK Lee Aociate Profeor Dept. of Nuclear & Quantum Engineering, KAIST Iue Studied in KAIST Larger power ytem require higher pecific power Advanced

More information

Seismic responses analysis of long continuous rigid-framed bridge subjected to multi-support excitations

Seismic responses analysis of long continuous rigid-framed bridge subjected to multi-support excitations Seimic repone analyi of long continuou rigid-framed ridge ujected to multi-upport excitation Jitao Li 1 and Qinghan Yang 2 1 Potgraduate, School of Civil Engineering, Beijing Jiaotong Univerity, Beijing.

More information

MODERN CONTROL SYSTEMS

MODERN CONTROL SYSTEMS MODERN CONTROL SYSTEMS Lecture 1 Root Locu Emam Fathy Department of Electrical and Control Engineering email: emfmz@aat.edu http://www.aat.edu/cv.php?dip_unit=346&er=68525 1 Introduction What i root locu?

More information

715. Transients in the electromagnetic actuator with the controlled supplier

715. Transients in the electromagnetic actuator with the controlled supplier 75. Tranient in the electromagnetic actuator with the controlled upplier Broniław Tomczuk, Andrzej Waindok, Dawid Wajnert Opole Univerity of Technology, Department of Indutrial Electrical Engineering Prozkowka

More information

Evolutionary Algorithms Based Fixed Order Robust Controller Design and Robustness Performance Analysis

Evolutionary Algorithms Based Fixed Order Robust Controller Design and Robustness Performance Analysis Proceeding of 01 4th International Conference on Machine Learning and Computing IPCSIT vol. 5 (01) (01) IACSIT Pre, Singapore Evolutionary Algorithm Baed Fixed Order Robut Controller Deign and Robutne

More information

Representation of a Group of Three-phase Induction Motors Using Per Unit Aggregation Model A.Kunakorn and T.Banyatnopparat

Representation of a Group of Three-phase Induction Motors Using Per Unit Aggregation Model A.Kunakorn and T.Banyatnopparat epreentation of a Group of Three-phae Induction Motor Uing Per Unit Aggregation Model A.Kunakorn and T.Banyatnopparat Abtract--Thi paper preent a per unit gregation model for repreenting a group of three-phae

More information

THE EXPERIMENTAL PERFORMANCE OF A NONLINEAR DYNAMIC VIBRATION ABSORBER

THE EXPERIMENTAL PERFORMANCE OF A NONLINEAR DYNAMIC VIBRATION ABSORBER Proceeding of IMAC XXXI Conference & Expoition on Structural Dynamic February -4 Garden Grove CA USA THE EXPERIMENTAL PERFORMANCE OF A NONLINEAR DYNAMIC VIBRATION ABSORBER Yung-Sheng Hu Neil S Ferguon

More information

Digital Control System

Digital Control System Digital Control Sytem - A D D A Micro ADC DAC Proceor Correction Element Proce Clock Meaurement A: Analog D: Digital Continuou Controller and Digital Control Rt - c Plant yt Continuou Controller Digital

More information

MM7. PID Control Design

MM7. PID Control Design MM7. PD Control Deign Reading Material: FC: p.79-200, DC: p.66-68. Propertie of PD control 2. uning Method of PD Control 3. Antiwindup echnique 4. A real cae tudy BO9000 0/9/2004 Proce Control . PD Feedback

More information

LOW ORDER MIMO CONTROLLER DESIGN FOR AN ENGINE DISTURBANCE REJECTION PROBLEM. P.Dickinson, A.T.Shenton

LOW ORDER MIMO CONTROLLER DESIGN FOR AN ENGINE DISTURBANCE REJECTION PROBLEM. P.Dickinson, A.T.Shenton LOW ORDER MIMO CONTROLLER DESIGN FOR AN ENGINE DISTURBANCE REJECTION PROBLEM P.Dickinon, A.T.Shenton Department of Engineering, The Univerity of Liverpool, Liverpool L69 3GH, UK Abtract: Thi paper compare

More information

CALIFORNIA INSTITUTE OF TECHNOLOGY Control and Dynamical Systems

CALIFORNIA INSTITUTE OF TECHNOLOGY Control and Dynamical Systems Control and Dynamical Sytem CDS 0 Problem Set #5 Iued: 3 Nov 08 Due: 0 Nov 08 Note: In the upper left hand corner of the econd page of your homework et, pleae put the number of hour that you pent on thi

More information

Design By Emulation (Indirect Method)

Design By Emulation (Indirect Method) Deign By Emulation (Indirect Method he baic trategy here i, that Given a continuou tranfer function, it i required to find the bet dicrete equivalent uch that the ignal produced by paing an input ignal

More information

The package size and configuration conform to the EIA-535 BAAC standard specification for case size 3528 tantalum capacitors.

The package size and configuration conform to the EIA-535 BAAC standard specification for case size 3528 tantalum capacitors. H Surface Mount LED Indicator Technical Data HSMD-TX HSME-TX HSMG-TX HSMH-TX HSMS-TX HSMY-TX Feature Compatible with Automatic Placement Equipment Compatible with Infrared and Vapor Phae Reflow Solder

More information

Wolfgang Hofle. CERN CAS Darmstadt, October W. Hofle feedback systems

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

More information

A Simple Approach to Synthesizing Naïve Quantized Control for Reference Tracking

A Simple Approach to Synthesizing Naïve Quantized Control for Reference Tracking A Simple Approach to Syntheizing Naïve Quantized Control for Reference Tracking SHIANG-HUA YU Department of Electrical Engineering National Sun Yat-Sen Univerity 70 Lien-Hai Road, Kaohiung 804 TAIAN Abtract:

More information

5.5 Application of Frequency Response: Signal Filters

5.5 Application of Frequency Response: Signal Filters 44 Dynamic Sytem Second order lowpa filter having tranfer function H()=H ()H () u H () H () y Firt order lowpa filter Figure 5.5: Contruction of a econd order low-pa filter by combining two firt order

More information

The application of a multi-domain boundary face method in a steady state heat conduction problem

The application of a multi-domain boundary face method in a steady state heat conduction problem Boundary Element and Other Meh Reduction Method XXXVI 285 The application of a multi-domain boundary face method in a teady tate heat conduction problem Jianming Zhang, Xianghe Li & Yuan Li State Key Laboratory

More information

Analysis of Step Response, Impulse and Ramp Response in the Continuous Stirred Tank Reactor System

Analysis of Step Response, Impulse and Ramp Response in the Continuous Stirred Tank Reactor System ISSN: 454-50 Volume 0 - Iue 05 May 07 PP. 7-78 Analyi of Step Repone, Impule and Ramp Repone in the ontinuou Stirred Tank Reactor Sytem * Zohreh Khohraftar, Pirouz Derakhhi, (Department of hemitry, Science

More information

EE105 - Fall 2005 Microelectronic Devices and Circuits

EE105 - Fall 2005 Microelectronic Devices and Circuits EE5 - Fall 5 Microelectronic Device and ircuit Lecture 9 Second-Order ircuit Amplifier Frequency Repone Announcement Homework 8 due tomorrow noon Lab 7 next week Reading: hapter.,.3. Lecture Material Lat

More information

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

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder R. W. Erickon Department of Electrical, Computer, and Energy Engineering Univerity of Colorado, Boulder ZOH: Sampled Data Sytem Example v T Sampler v* H Zero-order hold H v o e = 1 T 1 v *( ) = v( jkω

More information

Because of their high stiffness, compact size, and effectively

Because of their high stiffness, compact size, and effectively 1630 IEEE Tranaction on Ultraonic, Ferroelectric, and Frequency ontrol, vol. 60, no. 8, Augut 2013 harge Drive With Active D Stabilization for inearization of Piezoelectric Hyterei Andrew J. Fleming, Member,

More information

Chapter 2: Problem Solutions

Chapter 2: Problem Solutions Chapter 2: Solution Dicrete Time Proceing of Continuou Time Signal Sampling à 2.. : Conider a inuoidal ignal and let u ample it at a frequency F 2kHz. xt 3co000t 0. a) Determine and expreion for the ampled

More information

Modelling and Wavelet-Based Identification of 3-DOF Vehicle Suspension System

Modelling and Wavelet-Based Identification of 3-DOF Vehicle Suspension System Journal of Software Engineering and Application, 011, 4, 67-681 doi:10.436/jea.011.41079 Publihed Online December 011 (http://www.scirp.org/journal/jea) Modelling and Wavelet-Baed Identification of 3-DOF

More information

A Study on Simulating Convolutional Codes and Turbo Codes

A Study on Simulating Convolutional Codes and Turbo Codes A Study on Simulating Convolutional Code and Turbo Code Final Report By Daniel Chang July 27, 2001 Advior: Dr. P. Kinman Executive Summary Thi project include the deign of imulation of everal convolutional

More information

Reduced Order Modeling Enables System Level Simulation of a MEMS Piezoelectric Energy Harvester with a Self-Supplied SSHI-Scheme

Reduced Order Modeling Enables System Level Simulation of a MEMS Piezoelectric Energy Harvester with a Self-Supplied SSHI-Scheme Reduced Order Modeling Enables System Level Simulation of a MEMS Piezoelectric Energy Harvester with a Self-Supplied SSHI-Scheme F. Sayed 1, D. Hohlfeld², T. Bechtold 1 1 Institute for Microsystems Engineering,

More information

Electromechanical Dynamics for Micro Film

Electromechanical Dynamics for Micro Film Senor & Tranducer, Vol. 76, Iue 8, Augut 04, pp. 99-06 Senor & Tranducer 04 by IFSA Publihing, S. L. http://www.enorportal.com Electromechanical Dynamic for Micro Film Lizhong Xu, Xiaorui Fu Mechanical

More information

Minimal state space realization of MIMO systems in the max algebra

Minimal state space realization of MIMO systems in the max algebra KULeuven Department of Electrical Engineering (ESAT) SISTA Technical report 94-54 Minimal tate pace realization of MIMO ytem in the max algebra B De Schutter and B De Moor If you want to cite thi report

More information

Radiation Heat Transfer

Radiation Heat Transfer CM30 ranport I Part II: Heat ranfer Radiation Heat ranfer Profeor Faith Morrion Department of Chemical Engineering Michigan echnological Univerity CM30 ranport Procee and Unit Operation I Part : Heat ranfer

More information

Sliding Mode Control of a Dual-Fuel System Internal Combustion Engine

Sliding Mode Control of a Dual-Fuel System Internal Combustion Engine Proceeding of the ASME 9 Dynamic Sytem and Control Conference DSCC9 October -4, 9, Hollywood, California, USA DSCC9-59 Control of a Dual-Fuel Sytem Internal Combution Engine Stephen Pace Department of

More information

Singular Value Analysis of Linear- Quadratic Systems!

Singular Value Analysis of Linear- Quadratic Systems! Singular Value Analyi of Linear- Quadratic Sytem! Robert Stengel! Optimal Control and Etimation MAE 546! Princeton Univerity, 2017!! Multivariable Nyquit Stability Criterion!! Matrix Norm and Singular

More information

Fractional-Order PI Speed Control of a Two-Mass Drive System with Elastic Coupling

Fractional-Order PI Speed Control of a Two-Mass Drive System with Elastic Coupling Fractional-Order PI Speed Control of a Two-Ma Drive Sytem with Elatic Coupling Mohammad Amin Rahimian, Mohammad Saleh Tavazoei, and Farzad Tahami Electrical Engineering Department, Sharif Univerity of

More information

Experimental Study and Analysis of Flow Induced Vibration in a pipeline

Experimental Study and Analysis of Flow Induced Vibration in a pipeline Experimental Study and Analysis of Flow Induced Vibration in a pipeline R.Veerapandi a G. Karthikeyan b Dr. G. R.Jinu c R. Kannaiah d a Final Year M.E(CAD),Regional Centre of Anna University,Tirunelveli-629004

More information

Introduction to Laplace Transform Techniques in Circuit Analysis

Introduction to Laplace Transform Techniques in Circuit Analysis Unit 6 Introduction to Laplace Tranform Technique in Circuit Analyi In thi unit we conider the application of Laplace Tranform to circuit analyi. A relevant dicuion of the one-ided Laplace tranform i found

More information

Typical Process Control System. Lecture 8. ExampleMIMO-system: ADistillation Column. Multivariable transfer functions

Typical Process Control System. Lecture 8. ExampleMIMO-system: ADistillation Column. Multivariable transfer functions Lecture 8 Typical Proce Control Sytem Today lecture: Multivariable ytem... Tranfer function for MIMO-ytem vehicle power network proce control indutry Limitation due to untable multivariable zero Decentralized/decoupled

More information

AEIJST June Vol 2 Issue 6 ISSN

AEIJST June Vol 2 Issue 6 ISSN Theoretical Invetigation Performance of Proportional Directional Control Value Uing Matlab /Simulink *Sudhindra R. Kulkarni **S.H.Kulkarni ***Sudhindra R. Kulkarni *Department of Mechanical Engineering,

More information

POWER SYSTEM SMALL SIGNAL STABILITY ANALYSIS BASED ON TEST SIGNAL

POWER SYSTEM SMALL SIGNAL STABILITY ANALYSIS BASED ON TEST SIGNAL POWE YEM MALL INAL ABILIY ANALYI BAE ON E INAL Zheng Xu, Wei hao, Changchun Zhou Zheang Univerity, Hangzhou, 37 PChina Email: hvdc@ceezueducn Abtract - In thi paper, a method baed on ome tet ignal (et

More information

MODELING OF NEGATIVE INFLUENCES AT THE SIGNAL TRANSMISSION IN THE OPTICAL MEDIUM. Rastislav Róka, Filip Čertík

MODELING OF NEGATIVE INFLUENCES AT THE SIGNAL TRANSMISSION IN THE OPTICAL MEDIUM. Rastislav Róka, Filip Čertík MODELING OF NEGATIVE INFLUENCES AT THE SIGNAL TRANSMISSION IN THE OPTICAL MEDIUM Ratilav Róka, Filip Čertík Intitute of Telecommunication, FEEIT, Slovak Univerity of Technology in Bratilava E-mail: ratilav.roka@tuba.k,

More information

A New Method For Simultaneously Measuring And Analyzing PLL Transfer Function And Noise Processes

A New Method For Simultaneously Measuring And Analyzing PLL Transfer Function And Noise Processes A New Method For Simultaneouly Meauring And Analyzing PLL Tranfer Function And Noie Procee Mike Li CTO, Ph.D. Jan Wiltrup Corporate Conultant 1 Outline Introduction Phae Locked-Loop (PLL) and Noie Procee

More information

Lecture #9 Continuous time filter

Lecture #9 Continuous time filter Lecture #9 Continuou time filter Oliver Faut December 5, 2006 Content Review. Motivation......................................... 2 2 Filter pecification 2 2. Low pa..........................................

More information

Jens Otto CADFEM GmbH

Jens Otto CADFEM GmbH Titelmasterformat Simulation of Electric durch Machines Klicken with bearbeiten ANSYS Jens Otto CADFEM GmbH 1 Why Simulation with ANSYS? Challenges for electric machines Electromagnetic Design: Rated power/

More information

Extremum seeking (ES) was invented in

Extremum seeking (ES) was invented in EXTREMUM SEEKING FOR WIND AND SOLAR ENERGY by Azad Ghaffari, Mirolav Krtic and Sridhar Sehagiri APPLICATIONS Extremum eeking (ES) wa invented in 1922 and i one of the oldet feedback method Rather than

More information

The Skeldar V-150 flight control system. Modeling, identification and control of an unmanned helicopter. Saab AB. Saab Aerosystems.

The Skeldar V-150 flight control system. Modeling, identification and control of an unmanned helicopter. Saab AB. Saab Aerosystems. The Skeldar V-5 flight ontrol ytem Modeling, identifiation and ontrol of an unmanned heliopter Ola Härkegård LiTH, November 8, 27 Organization Saab AB Saab Aeroytem Aeronauti Flight Control Sytem Aerodynami

More information

Titelmasterformat durch Klicken bearbeiten

Titelmasterformat durch Klicken bearbeiten Titelmasterformat durch Klicken bearbeiten Vibration and Acoustics for Electric Drive Development Presenter: Jens Otto, CADFEM GmbH Developer: Dr. Jürgen Wibbeler, Dr. Martin Hanke, CADFEM GmbH 4th CADFEM

More information

FLEXOELECTRIC SIGNALS ON RINGS IN TRANSVERSE MOTIONS

FLEXOELECTRIC SIGNALS ON RINGS IN TRANSVERSE MOTIONS Proceeding of the ASME 011 International Deign Engineering Technical Conference & Computer and Information in Engineering Conference IDETC/CIE 011 Augut 8-31, 011, Wahington, DC, USA DETC011-4819 FLEXOELECTRIC

More information

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment Journal of Multidiciplinary Engineering Science and Technology (JMEST) ISSN: 59- Vol. Iue, January - 5 Advanced D-Partitioning Analyi and it Comparion with the haritonov Theorem Aement amen M. Yanev Profeor,

More information

EE 4343/ Control System Design Project

EE 4343/ Control System Design Project Copyright F.L. Lewi 2004 All right reerved EE 4343/5320 - Control Sytem Deign Project Updated: Sunday, February 08, 2004 Background: Analyi of Linear ytem, MATLAB Review of Baic Concept LTI Sytem LT I

More information

Module 4: Time Response of discrete time systems Lecture Note 1

Module 4: Time Response of discrete time systems Lecture Note 1 Digital Control Module 4 Lecture Module 4: ime Repone of dicrete time ytem Lecture Note ime Repone of dicrete time ytem Abolute tability i a baic requirement of all control ytem. Apart from that, good

More information

Modeling the scalar wave equation with Nyström methods

Modeling the scalar wave equation with Nyström methods GEOPHYSICS, VOL. 71, NO. 5 SEPTEMBER-OCTOBER 200 ; P. T151 T158, 7 FIGS. 10.1190/1.2335505 Modeling the calar wave equation with Nytröm method Jing-Bo Chen 1 ABSTRACT High-accuracy numerical cheme for

More information

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. R 4 := 100 kohm

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. R 4 := 100 kohm SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuit II Solution to Aignment 3 February 2003. Cacaded Op Amp [DC&L, problem 4.29] An ideal op amp ha an output impedance of zero,

More information

Journal of Advanced Mechanical Design, Systems, and Manufacturing

Journal of Advanced Mechanical Design, Systems, and Manufacturing Vol., No. 4, 8 Mathematical Model of Linear Motor Stage with Non-Linear Friction Characteritic * Satohi KANEKO **, Ryuta SATO *** and Maaomi TSUTSUMI **** **Pot graduate, Tokyo Univerity of Agriculture

More information

Experimental Modal Analysis of a Flat Plate Subjected To Vibration

Experimental Modal Analysis of a Flat Plate Subjected To Vibration American Journal of Engineering Research (AJER) 2016 American Journal of Engineering Research (AJER) e-issn: 2320-0847 p-issn : 2320-0936 Volume-5, Issue-6, pp-30-37 www.ajer.org Research Paper Open Access

More information

Lecture 6: Resonance II. Announcements

Lecture 6: Resonance II. Announcements EES 5 Spring 4, Lecture 6 Lecture 6: Reonance II EES 5 Spring 4, Lecture 6 Announcement The lab tart thi week You mut how up for lab to tay enrolled in the coure. The firt lab i available on the web ite,

More information

Linearteam tech paper. The analysis of fourth-order state variable filter and it s application to Linkwitz- Riley filters

Linearteam tech paper. The analysis of fourth-order state variable filter and it s application to Linkwitz- Riley filters Linearteam tech paper The analyi of fourth-order tate variable filter and it application to Linkwitz- iley filter Janne honen 5.. TBLE OF CONTENTS. NTOCTON.... FOTH-OE LNWTZ-LEY (L TNSFE FNCTON.... TNSFE

More information

Solutions. Digital Control Systems ( ) 120 minutes examination time + 15 minutes reading time at the beginning of the exam

Solutions. Digital Control Systems ( ) 120 minutes examination time + 15 minutes reading time at the beginning of the exam BSc - Sample Examination Digital Control Sytem (5-588-) Prof. L. Guzzella Solution Exam Duration: Number of Quetion: Rating: Permitted aid: minute examination time + 5 minute reading time at the beginning

More information

Real Sources (Secondary Sources) Phantom Source (Primary source) LS P. h rl. h rr. h ll. h lr. h pl. h pr

Real Sources (Secondary Sources) Phantom Source (Primary source) LS P. h rl. h rr. h ll. h lr. h pl. h pr Ecient frequency domain ltered-x realization of phantom ource iet C.W. ommen, Ronald M. Aart, Alexander W.M. Mathijen, John Gara, Haiyan He Abtract A phantom ound ource i a virtual ound image which can

More information

Vibro-acoustic Analysis for Noise Reduction of Electric Machines

Vibro-acoustic Analysis for Noise Reduction of Electric Machines Vibro-acoustic Analysis for Noise Reduction of Electric Machines From Flux to OptiStruct Example : Synchronous Machine Flux 2D coupling to OptiStruct Patrick LOMBARD Application Team Manager Patrick.Lombard@cedrat.com

More information

MEEN 673: NONLINEAR FINITE ELEMENT ANALYSIS. Time-Dependent Problems

MEEN 673: NONLINEAR FINITE ELEMENT ANALYSIS. Time-Dependent Problems JN Reddy - 1 MEEN 673: NONLINEAR FINITE ELEMENT ANALYSIS Time-Dependent Problem ONTENTS Tranient problem Semi-dicretization Time approimation Ma lumping Stability and accuracy omputer implementation Numerical

More information

Resonance investigation of pump-turbine during startup process

Resonance investigation of pump-turbine during startup process IOP Conference Serie: Earth and Environmental Science OPEN ACCESS Reonance invetigation of pump-turbine during tartup proce To cite thi article: L Y He et al 2014 IOP Conf. Ser.: Earth Environ. Sci. 22

More information

MODELING OF A SYSTEM WITH HYBRID DYNAMICS

MODELING OF A SYSTEM WITH HYBRID DYNAMICS 4 Acta Electrotechnica et Informatica, Vol., No., 0, 4 9, DOI: 0.478/v098-0-000- MODELING OF A SYSTEM WITH HYBRID DYNAMICS Vratilav HLADKÝ, Ľuboš POPOVIČ, Ján SARNOVSKÝ Department of Cybernetic and Artificial

More information

The Analysis of Aluminium Cantilever Beam with Piezoelectric Material by changing Position of piezo patch over Length of Beam

The Analysis of Aluminium Cantilever Beam with Piezoelectric Material by changing Position of piezo patch over Length of Beam The Analysis of Aluminium Cantilever Beam with Piezoelectric Material by changing Position of piezo patch over Length of Beam Mr. Lalit R. Shendre 1, Prof. Bhamare V.G. 2 1PG Student, Department of Mechanical

More information

MINIATURIZATION OF INERTIAL MAGNETOELECTRIC VIBRATION VELOCITY SENSOR WITH HIGH FREQUENCY RESPONSE AT LOW FREQUENCY BAND

MINIATURIZATION OF INERTIAL MAGNETOELECTRIC VIBRATION VELOCITY SENSOR WITH HIGH FREQUENCY RESPONSE AT LOW FREQUENCY BAND th February 3. Vol. 48 No. 5-3 JATIT & LLS. All right reerved. ISSN: 99-8645 www.jatit.org E-ISSN: 87-395 MINIATURIZATION OF INERTIAL MAGNETOELECTRIC VIBRATION VELOCITY SENSOR WITH HIGH FREQUENCY RESPONSE

More information

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

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder R. W. Erickon Department of Electrical, Computer, and Energy Engineering Univerity of Colorado, Boulder Cloed-loop buck converter example: Section 9.5.4 In ECEN 5797, we ued the CCM mall ignal model to

More information

Chapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog

Chapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog Chapter Sampling and Quantization.1 Analog and Digital Signal In order to invetigate ampling and quantization, the difference between analog and digital ignal mut be undertood. Analog ignal conit of continuou

More information

Massachusetts Institute of Technology Dynamics and Control II

Massachusetts Institute of Technology Dynamics and Control II I E Maachuett Intitute of Technology Department of Mechanical Engineering 2.004 Dynamic and Control II Laboratory Seion 5: Elimination of Steady-State Error Uing Integral Control Action 1 Laboratory Objective:

More information

RESEARCH ON THE THEORIES OF BEM BASED CYCLOSTATIONARY NEAR FIELD ACOUSTIC HOLOGRAPHY. Haibin Zhang, Weikang Jiang and Quan Wan

RESEARCH ON THE THEORIES OF BEM BASED CYCLOSTATIONARY NEAR FIELD ACOUSTIC HOLOGRAPHY. Haibin Zhang, Weikang Jiang and Quan Wan ICV14 Cairn Autralia 9-12 July, 2007 REEARCH ON THE THEORIE OF BEM BAED CYCLOTATIONARY NEAR FIELD ACOUTIC HOLOGRAPHY Haibin Zhang, Weikang Jiang and Quan Wan tate Key Laboratory of Mechanical ytem and

More information

The stabilization interval system of a tethered descent underwater vehicle

The stabilization interval system of a tethered descent underwater vehicle IOP Conference Serie: Material Science and Engineering PAPER OPEN ACCESS The tabilization interval ytem of a tethered decent underwater vehicle To cite thi article: S A Gayvoronkiy et al 016 IOP Conf.

More information

Sensorless speed control including zero speed of non salient PM synchronous drives

Sensorless speed control including zero speed of non salient PM synchronous drives BULLETIN OF THE POLISH ACADEMY OF SCIENCES TECHNICAL SCIENCES Vol. 54, No. 3, 2006 Senorle peed control including zero peed of non alient PM ynchronou drive H. RASMUSSEN Aalborg Univerity, Fredrik Bajer

More information