- Critical parts are tested (PS) - The remaining parts are simulated (NS).
|
|
- Gladys Johnston
- 5 years ago
- Views:
Transcription
1
2 Hybrid simulatio of a structural system Loads (Disp.) simulatig deck motio due to earthquake K V T B CBdV Deck modeled aalytically by F.E.M. Piers tested physically - Critical parts are tested (PS) - The remaiig parts are simulated (NS). 1) Physical Substrucutre should move cotiuously, with a costat timescale betwee the seismic evet ad the testig duratio; 2) I the curret applicatio, a refied FE model is itroduced for the Numerical Substructure.
3 Servo-Hydraulic Actuators The implemetatio scheme developed at JRC, Ispra Force trasducers Displacemet Trasducers Referece frame A digital implemetatio of PsD cotrol scheme: Dt s = 1 or 2 msec Substructurig capacity Measuremet of reactio force R... dt Imposed displacemet d.. M d Cd. R d MIa g t Accelerogram x g Numerical itegratio Numerical model
4 The classical moolithic time itegratio:.. M d Cd. Whe the NS is refied, a moolithic itegratio step caot be complete withi the cotrol samplig time. R d MIa g è 1) Use of Partitioed itegratio ad differet time steps betwee the Ns ad the PS. è 2) Explicit scheme is preferable for PS (without iteratio), whereas implicit scheme is suitable to the NS (stability cosideratio). t K. Park, C. Felippa, 1983; T. Hughes, W. Liu, 1978; W. Liu, T. Belytschko, 1982
5 A Multi-time-step Explicit-implicit Method (Gravouil ad Combescure 2001) Steps are sequetial. Steps A 1 ad B 1 are cocurret.
6 Time steppig schemes applied to liear problems ca be recast i a recursive form as where X is the state vector, A is the amplificatio matrix ad L is the load vector. For PM method, X reads with X AX L 1 X ( X, X, X ) A A B T 1 X ( u, u, u, u ), X ( u, u, u ) A A A A A T B B B B T, free X has 11 variables for a partitioed SDoF system. Boelli et.al, 2011
7 Photograph courtesy of JRC Isolator: the physical substructure. The emulated structure. Bridge deck: the umerical substructure.
8 Problems related to umerical dissipatio I FE aalysis, the higher modes are ofte spurious due to the artifacts of the umerical discretizatio process. These spurious modes could be excited due to experimetal errors durig hybrid simulatio. T. Hughes, 1987; Bursi, Shig, 1997; Hulbert, Chag, 1993/1996; C. Farhat, F.-X.Roux,
9 A ovel oe-step four-stage form of the G-alpha method Predictor: Equilibrium equatio (Im.): Corrector: u u tu t u t a 2 f 2 1 D D D ( ) 1 m 2 1 m f u u Dt u Dt(1 ) a 1 1 m m (Ex.): Mu Cu Ku F ( t ) ext Mu Cu Ku F ( t ) ext u u t u u u t u 2 f f 1 D 1; 1 D 1 1 m 1 m The equilibrium equatio is idetical to those of Newmark schemes. The itegratio parameters are chose as those of the origial implicit/explicit G-alpha method, that is, r as the spectral radius at the high frequecy limit for the implicit method ad r b as the spectral radius at the bifurcatio limit for the explicit method. He, 2008; Bursi, He 2012
10 Represetative Numerical Simulatio (I) 0.04 PM m2 u2 (rad) 0.00 m1 la ma u1 Aalytical Part mb time (s) lb Experimetal Part 0.04 PM-alpha (rad) 0.00 Partitioed three-dof system f 1 =0.24 Hz, f 2 =1.6 Hz, f 3 =35 Hz time (s) Rotatioal respose i free vibratio for the Three-DoF system (Dt A =5ms, ss = 100): (a) the PM method; (b) the PM-alpha method, r = r b = 0.5
11 A three-actuator testig setup of the previous 3DOF model Simulatio cosiderig the cotrol errors of the actuators i udershootig type (Mosqueda et.al 2007) ad measured errors of load cells as white oise (0.06%) Respose of partitioed three-dof system (Texp./Ts.e.=50; Dt A =2ms ; Dt B =0.02ms ;ss=100; )
12 This work presets partitioed time itegratio methods for solvig dyamic problems of hybrid structural systems, typical of pseudo-dyamic testig with substructurig or hybrid simulatio, as decomposed by computatioal/physical cosideratios. The methods implemet the iterfield parallel aalysis procedure suitable to maitai a costat time scale betwee the umerical ad physical substructures, by usig the implicit ad explicit schemes of differet time steps. The characteristics of the proposed time schemes are aalyzed with respect to their covergece (stability ad accuracy). High-frequecy umerical dissipatio based o a ew form of the G-alpha methods is itroduced, which is show to be helpful to hybrid simulatio with the presece of both the cotrol errors ad the measuremet errors.
13 Thak you for your attetio! Ackowledgemets: Prof. O.S. UNITN Dr. P. JRC, Ispra
2C09 Design for seismic and climate changes
2C09 Desig for seismic ad climate chages Lecture 02: Dyamic respose of sigle-degree-of-freedom systems I Daiel Grecea, Politehica Uiversity of Timisoara 10/03/2014 Europea Erasmus Mudus Master Course Sustaiable
More informationMechatronics. Time Response & Frequency Response 2 nd -Order Dynamic System 2-Pole, Low-Pass, Active Filter
Time Respose & Frequecy Respose d -Order Dyamic System -Pole, Low-Pass, Active Filter R 4 R 7 C 5 e i R 1 C R 3 - + R 6 - + e out Assigmet: Perform a Complete Dyamic System Ivestigatio of the Two-Pole,
More informationSpectral Analysis. This week in lab. Next classes: 3/26 and 3/28. Your next experiment Homework is to prepare
Spectral Aalysis This week i lab Your ext experimet Homework is to prepare Next classes: 3/26 ad 3/28 Aero Testig, Fracture Toughess Testig Read the Experimets 5 ad 7 sectios of the course maual Spectral
More informationMONOLITHIC AND PARTITIONED L-STABLE ROSENBROCK METHODS FOR DYNAMIC SUBSTRUCTURE TESTS. Oreste S. Bursi, Chuanguo Jia and Zhen Wang
MONOLITHIC AND PARTITIONED L-STABLE ROSENBROCK METHODS FOR DYNAMIC SUBSTRUCTURE TESTS Oreste S. Bursi, Chuanguo Jia and Zhen Wang University of Trento/ Department of Mechanical and Structural Engineering,
More informationBasics of Dynamics. Amit Prashant. Indian Institute of Technology Gandhinagar. Short Course on. Geotechnical Aspects of Earthquake Engineering
Basics of yamics Amit Prashat Idia Istitute of Techology Gadhiagar Short Course o Geotechical Aspects of Earthquake Egieerig 4 8 March, 213 Our ear Pedulum Revisited g.si g l s Force Equilibrium: Cord
More informationFIXED-FREE AGAINST FREE-FREE BEAMS FOR DYNAMIC YOUNG S MODULUS OF WOOD By: Mehran Roohnia
FIXED-FREE AGAINST FREE-FREE BEAMS FOR DYNAMIC YOUNG S MODULUS OF WOOD By: Mehra Roohia Itroductio: Itroductio: Modulus of Elasticity Hook's Law: s : Stress (e.g. Normal Stress) E: Modulus of Elasticity,
More information2C09 Design for seismic and climate changes
C9 Desig for seismic ad climate chages Lecture 3: Dyamic respose of sigle-degree-of-freedom systems II Daiel Grecea, Politehica Uiversity of Timisoara 11/3/14 Europea Erasmus Mudus Master Course Sustaiable
More informationElastic Plastic Behavior of Geomaterials: Modeling and Simulation Issues
Elastic Plastic Behavior of Geomaterials: Modelig ad Simulatio Issues Boris Zhaohui Yag (UA), Zhao Cheg (EarthMechaics Ic.), Mahdi Taiebat (UBC) Departmet of Civil ad Evirometal Egieerig Uiversity of Califoria,
More informationVibratory Motion. Prof. Zheng-yi Feng NCHU SWC. National CHung Hsing University, Department of Soil and Water Conservation
Vibratory Motio Prof. Zheg-yi Feg NCHU SWC 1 Types of vibratory motio Periodic motio Noperiodic motio See Fig. A1, p.58 Harmoic motio Periodic motio Trasiet motio impact Trasiet motio earthquake A powerful
More information577. Estimation of surface roughness using high frequency vibrations
577. Estimatio of surface roughess usig high frequecy vibratios V. Augutis, M. Sauoris, Kauas Uiversity of Techology Electroics ad Measuremets Systems Departmet Studetu str. 5-443, LT-5368 Kauas, Lithuaia
More informationNatural frequencies, mode shapes and modal damping values are the most important parameters to
Abstract Natural frequecies, mode shapes ad modal dampig values are the most importat parameters to describe the oise ad vibratio behaviour of a mechaical system. For rotatig machiery, however, the directivity
More informationResearch Article Health Monitoring for a Structure Using Its Nonstationary Vibration
Advaces i Acoustics ad Vibratio Volume 2, Article ID 69652, 5 pages doi:.55/2/69652 Research Article Health Moitorig for a Structure Usig Its Nostatioary Vibratio Yoshimutsu Hirata, Mikio Tohyama, Mitsuo
More informationA PROCEDURE TO MODIFY THE FREQUENCY AND ENVELOPE CHARACTERISTICS OF EMPIRICAL GREEN'S FUNCTION. Lin LU 1 SUMMARY
A POCEDUE TO MODIFY THE FEQUENCY AND ENVELOPE CHAACTEISTICS OF EMPIICAL GEEN'S FUNCTION Li LU SUMMAY Semi-empirical method, which divides the fault plae of large earthquake ito mets ad uses small groud
More informationEXPERIMENT OF SIMPLE VIBRATION
EXPERIMENT OF SIMPLE VIBRATION. PURPOSE The purpose of the experimet is to show free vibratio ad damped vibratio o a system havig oe degree of freedom ad to ivestigate the relatioship betwee the basic
More informationProvläsningsexemplar / Preview TECHNICAL REPORT INTERNATIONAL SPECIAL COMMITTEE ON RADIO INTERFERENCE
TECHNICAL REPORT CISPR 16-4-3 2004 AMENDMENT 1 2006-10 INTERNATIONAL SPECIAL COMMITTEE ON RADIO INTERFERENCE Amedmet 1 Specificatio for radio disturbace ad immuity measurig apparatus ad methods Part 4-3:
More informationResearch Article Health Monitoring for a Structure Using Its Nonstationary Vibration
Hidawi Publishig Corporatio Advaces i Acoustics ad Vibratio Volume 2, Article ID 69652, 5 pages doi:.55/2/69652 Research Article Health Moitorig for a Structure Usig Its Nostatioary Vibratio Yoshimutsu
More information1. Linearization of a nonlinear system given in the form of a system of ordinary differential equations
. Liearizatio of a oliear system give i the form of a system of ordiary differetial equatios We ow show how to determie a liear model which approximates the behavior of a time-ivariat oliear system i a
More informationSchool of Mechanical Engineering Purdue University. ME375 Frequency Response - 1
Case Study ME375 Frequecy Respose - Case Study SUPPORT POWER WIRE DROPPERS Electric trai derives power through a patograph, which cotacts the power wire, which is suspeded from a cateary. Durig high-speed
More informationTHE APPEARANCE OF FIBONACCI AND LUCAS NUMBERS IN THE SIMULATION OF ELECTRICAL POWER LINES SUPPLIED BY TWO SIDES
THE APPEARANCE OF FIBONACCI AND LUCAS NUMBERS IN THE SIMULATION OF ELECTRICAL POWER LINES SUPPLIED BY TWO SIDES Giuseppe Ferri Dipartimeto di Ihgegeria Elettrica-FacoM di Igegeria, Uiversita di L'Aquila
More informationμ are complex parameters. Other
A New Numerical Itegrator for the Solutio of Iitial Value Problems i Ordiary Differetial Equatios. J. Suday * ad M.R. Odekule Departmet of Mathematical Scieces, Adamawa State Uiversity, Mubi, Nigeria.
More informationIntroduction to Signals and Systems, Part V: Lecture Summary
EEL33: Discrete-Time Sigals ad Systems Itroductio to Sigals ad Systems, Part V: Lecture Summary Itroductio to Sigals ad Systems, Part V: Lecture Summary So far we have oly looked at examples of o-recursive
More informationAN OPEN-PLUS-CLOSED-LOOP APPROACH TO SYNCHRONIZATION OF CHAOTIC AND HYPERCHAOTIC MAPS
http://www.paper.edu.c Iteratioal Joural of Bifurcatio ad Chaos, Vol. 1, No. 5 () 119 15 c World Scietific Publishig Compay AN OPEN-PLUS-CLOSED-LOOP APPROACH TO SYNCHRONIZATION OF CHAOTIC AND HYPERCHAOTIC
More informationCUMULATIVE DAMAGE ESTIMATION USING WAVELET TRANSFORM OF STRUCTURAL RESPONSE
CUMULATIVE DAMAGE ESTIMATION USING WAVELET TRANSFORM OF STRUCTURAL RESPONSE Ryutaro SEGAWA 1, Shizuo YAMAMOTO, Akira SONE 3 Ad Arata MASUDA 4 SUMMARY Durig a strog earthquake, the respose of a structure
More informationSample Size Estimation in the Proportional Hazards Model for K-sample or Regression Settings Scott S. Emerson, M.D., Ph.D.
ample ie Estimatio i the Proportioal Haards Model for K-sample or Regressio ettigs cott. Emerso, M.D., Ph.D. ample ie Formula for a Normally Distributed tatistic uppose a statistic is kow to be ormally
More informationAdded mass estimation of open flat membranes vibrating in still air
Added mass estimatio of ope flat membraes vibratig i still air *Yua-qi Li 1),Yi Zhou ), Akihito YOHIDA 3) ad Yukio TAMURA 4) 1), ) Departmet of Buildig Egieerig, Togji Uiversity, haghai, 9, Chia 1) liyq@togji.edu.c
More informationDynamic Response of Linear Systems
Dyamic Respose of Liear Systems Liear System Respose Superpositio Priciple Resposes to Specific Iputs Dyamic Respose of st Order Systems Characteristic Equatio - Free Respose Stable st Order System Respose
More informationDynamic Response of Second Order Mechanical Systems with Viscous Dissipation forces
Hadout #b (pp. 4-55) Dyamic Respose o Secod Order Mechaical Systems with Viscous Dissipatio orces M X + DX + K X = F t () Periodic Forced Respose to F (t) = F o si( t) ad F (t) = M u si(t) Frequecy Respose
More informationCS284A: Representations and Algorithms in Molecular Biology
CS284A: Represetatios ad Algorithms i Molecular Biology Scribe Notes o Lectures 3 & 4: Motif Discovery via Eumeratio & Motif Represetatio Usig Positio Weight Matrix Joshua Gervi Based o presetatios by
More information567. Research of Dynamics of a Vibration Isolation Platform
567. Research of Dyamics of a Vibratio Isolatio Platform A. Kilikevičius, M. Jurevičius 2, M. Berba 3 Vilius Gedimias Techical Uiversity, Departmet of Machie buildig, J. Basaavičiaus str. 28, LT-03224
More informationTR Use of the Implicit HHT-I3 and the Explicit ADAMS Methods with the Absolute Nodal Coordinate Formulation
R-007-05 Use of the Implicit HH-I3 ad the Explicit ADAMS Methods with the Absolute Nodal Coordiate Formulatio Bassam Hussei, Da Negrut, Ahmed A. Shabaa August 007 Abstract his ivestigatio is cocered with
More informationLecture 2: Monte Carlo Simulation
STAT/Q SCI 43: Itroductio to Resamplig ethods Sprig 27 Istructor: Ye-Chi Che Lecture 2: ote Carlo Simulatio 2 ote Carlo Itegratio Assume we wat to evaluate the followig itegratio: e x3 dx What ca we do?
More informationPROPOSING INPUT-DEPENDENT MODE CONTRIBUTION FACTORS FOR SIMPLIFIED SEISMIC RESPONSE ANALYSIS OF BUILDING SYSTEMS
he 4 th World Coferece o Earthquake Egieerig October -7, 008, Beiig, Chia PROPOSING INPU-DEPENDEN ODE CONRIBUION FACORS FOR SIPLIFIED SEISIC RESPONSE ANALYSIS OF BUILDING SYSES ahmood Hosseii ad Laya Abbasi
More informationDYNAMIC ANALYSIS OF BEAM-LIKE STRUCTURES SUBJECT TO MOVING LOADS
DYNAMIC ANALYSIS OF BEAM-LIKE STRUCTURES SUBJECT TO MOVING LOADS Ivaa Štimac 1, Ivica Kožar 1 M.Sc,Assistat, Ph.D. Professor 1, Faculty of Civil Egieerig, Uiverity of Rieka, Croatia INTRODUCTION The vehicle-iduced
More informationCorrelation. Two variables: Which test? Relationship Between Two Numerical Variables. Two variables: Which test? Contingency table Grouped bar graph
Correlatio Y Two variables: Which test? X Explaatory variable Respose variable Categorical Numerical Categorical Cotigecy table Cotigecy Logistic Grouped bar graph aalysis regressio Mosaic plot Numerical
More informationDETERMINATION OF MECHANICAL PROPERTIES OF A NON- UNIFORM BEAM USING THE MEASUREMENT OF THE EXCITED LONGITUDINAL ELASTIC VIBRATIONS.
ICSV4 Cairs Australia 9- July 7 DTRMINATION OF MCHANICAL PROPRTIS OF A NON- UNIFORM BAM USING TH MASURMNT OF TH XCITD LONGITUDINAL LASTIC VIBRATIONS Pavel Aokhi ad Vladimir Gordo Departmet of the mathematics
More informationEECE 301 Signals & Systems
EECE 301 Sigals & Systems Prof. Mark Fowler Note Set #8 D-T Covolutio: The Tool for Fidig the Zero-State Respose Readig Assigmet: Sectio 2.1-2.2 of Kame ad Heck 1/14 Course Flow Diagram The arrows here
More information(all terms are scalars).the minimization is clearer in sum notation:
7 Multiple liear regressio: with predictors) Depedet data set: y i i = 1, oe predictad, predictors x i,k i = 1,, k = 1, ' The forecast equatio is ŷ i = b + Use matrix otatio: k =1 b k x ik Y = y 1 y 1
More information3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense,
3. Z Trasform Referece: Etire Chapter 3 of text. Recall that the Fourier trasform (FT) of a DT sigal x [ ] is ω ( ) [ ] X e = j jω k = xe I order for the FT to exist i the fiite magitude sese, S = x [
More informationApplication of an Innovative Precise Integration Method in Solving Equilibrium Equations of Motion for Structural Dynamic Problems
Applicatio of a Iovative Precise Itegratio Method i Solvig Equilibrium Equatios of Motio for Structural Dyamic Problems Chiu-li Wu Natioal Ceter for Research o Earthquake Egieerig,Taipei City, Taiwa Chig-Chiag
More informationChapter 6 Sampling Distributions
Chapter 6 Samplig Distributios 1 I most experimets, we have more tha oe measuremet for ay give variable, each measuremet beig associated with oe radomly selected a member of a populatio. Hece we eed to
More informationNonlinear Vibrations of Aerospace Structures
Noliear Vibratios of Aerospace Structures Uiversity of Liège, Belgium L Itroductio Course objectives Review of liear theory Istructors: G. Kersche, J.P. Noel, T. Detroux Cotact details: Space Structures
More informationProceedings of the 2nd International Conference on Computer Science and Electronics Engineering (ICCSEE 2013)
Proceedigs of the 2d Iteratioal Coferece o Computer Sciece ad Electroics Egieerig (ICCE 20) GPU Implemetatio of the Electric Power System Model for Real-Time Simulatio of Electromagetic Trasiets Slawomir
More informationMicroscopic traffic flow modeling
Chapter 34 Microscopic traffic flow modelig 34.1 Overview Macroscopic modelig looks at traffic flow from a global perspective, whereas microscopic modelig, as the term suggests, gives attetio to the details
More informationExponential Moving Average Pieter P
Expoetial Movig Average Pieter P Differece equatio The Differece equatio of a expoetial movig average lter is very simple: y[] x[] + (1 )y[ 1] I this equatio, y[] is the curret output, y[ 1] is the previous
More informationComputational Fluid Dynamics. Lecture 5
Time differecig cotiued. Three level schemes. B. Modified L-F schemes. C. Higher order methods. Three level schemes Computatioal Fluid Dyamics Lecture 5 ψ = α α β tf β cosistet schemes if α α = ad β β
More informationDifference Equation Construction (1) ENGG 1203 Tutorial. Difference Equation Construction (2) Grow, baby, grow (1)
ENGG 03 Tutorial Differece Equatio Costructio () Systems ad Cotrol April Learig Objectives Differece Equatios Z-trasform Poles Ack.: MIT OCW 6.0, 6.003 Newto s law of coolig states that: The chage i a
More informationSolution of Differential Equation from the Transform Technique
Iteratioal Joural of Computatioal Sciece ad Mathematics ISSN 0974-3189 Volume 3, Number 1 (2011), pp 121-125 Iteratioal Research Publicatio House http://wwwirphousecom Solutio of Differetial Equatio from
More informationSystem Diagnostics using Kalman Filter Estimation Error
System Diagostics usig Kalma Filter Estimatio Error Prof. Seugchul Lee, Seugtae Park, Heechag Kim, Hyusuk Huh ICMR2015 (11/25/2015) Machie Health Diagostics Desig Desig DNA + + Blue Prit phagocytes lymphocytes
More informationREAL-TIME MONITORING OF POWER AND NEUTRON CAPTURE CROSS SECTION IN NUCLEAR RESEARCH REACTOR
D5 REAL-TIME MONITORING OF POWER AND NEUTRON CAPTURE CROSS SECTION IN NUCLEAR RESEARCH REACTOR D.A.P. PALMA Brazilia Nuclear Eergy Commissio (CNEN), Rio de Jaeiro, Brazil A.Z. MESQUITA, R.M.G.P. SOUZA
More informationDynamic System Response
Solutio of Liear, Costat-Coefficiet, Ordiary Differetial Equatios Classical Operator Method Laplace Trasform Method Laplace Trasform Properties 1 st -Order Dyamic System Time ad Frequecy Respose d -Order
More informationFREE VIBRATION RESPONSE OF A SYSTEM WITH COULOMB DAMPING
Mechaical Vibratios FREE VIBRATION RESPONSE OF A SYSTEM WITH COULOMB DAMPING A commo dampig mechaism occurrig i machies is caused by slidig frictio or dry frictio ad is called Coulomb dampig. Coulomb dampig
More informationFinite Element Analysis of Cable-Stayed Bridges with Appropriate Initial Shapes Under Seismic Excitations Focusing on Deck-Stay Interaction
Chapter 9 Fiite Elemet Aalysis of Cable-Stayed Bridges with Appropriate Iitial Shapes Uder Seismic Excitatios Focusig o Deck-Stay Iteractio Mig-Yi Liu ad Pao-Hsii Wag Additioal iformatio is available at
More informationVibration Absorbers/Neutralisers. Professor Mike Brennan
Vibratio Absorbers/Neutralisers Professor Mike Brea Vibratio absorbers/eutralisers m k c Vibratio absorber/eutraliser What does it do? Absorber or eutraliser Mobility approach effectiveess of the device
More informationAPPLICATION OF NETSLAB FOR REMOTE TESTING OF BRIDGE SYSTEMS ABSTRACT
APPLICATION OF NETSLAB FOR REMOTE TESTING OF BRIDGE SYSTEMS Yulei Fa, Ya Xiao, ad Yurog Guo ABSTRACT A Iteret based remote hybrid testig platform was developed for bridge systems. The testig platform,
More informationCALCULATION OF STIFFNESS AND MASS ORTHOGONAL VECTORS
14. CALCULATION OF STIFFNESS AND MASS ORTHOGONAL VECTORS LDR Vectors are Always More Accurate tha Usig the Exact Eigevectors i a Mode Superpositio Aalysis 14.1 INTRODUCTION The major reaso to calculate
More informationMicroscopic Theory of Transport (Fall 2003) Lecture 6 (9/19/03) Static and Short Time Properties of Time Correlation Functions
.03 Microscopic Theory of Trasport (Fall 003) Lecture 6 (9/9/03) Static ad Short Time Properties of Time Correlatio Fuctios Refereces -- Boo ad Yip, Chap There are a umber of properties of time correlatio
More informationMOST PEOPLE WOULD RATHER LIVE WITH A PROBLEM THEY CAN'T SOLVE, THAN ACCEPT A SOLUTION THEY CAN'T UNDERSTAND.
XI-1 (1074) MOST PEOPLE WOULD RATHER LIVE WITH A PROBLEM THEY CAN'T SOLVE, THAN ACCEPT A SOLUTION THEY CAN'T UNDERSTAND. R. E. D. WOOLSEY AND H. S. SWANSON XI-2 (1075) STATISTICAL DECISION MAKING Advaced
More informationComplex Algorithms for Lattice Adaptive IIR Notch Filter
4th Iteratioal Coferece o Sigal Processig Systems (ICSPS ) IPCSIT vol. 58 () () IACSIT Press, Sigapore DOI:.7763/IPCSIT..V58. Complex Algorithms for Lattice Adaptive IIR Notch Filter Hog Liag +, Nig Jia
More informationLoad Dependent Ritz Vector Algorithm and Error Analysis
Load Depedet Ritz Vector Algorithm ad Error Aalysis Writte by Ed Wilso i 006. he Complete eigealue subspace I the aalysis of structures subected to three base acceleratios there is a requiremet that oe
More informationThe Phi Power Series
The Phi Power Series I did this work i about 0 years while poderig the relatioship betwee the golde mea ad the Madelbrot set. I have fially decided to make it available from my blog at http://semresearch.wordpress.com/.
More informationFinite Element Modeling of Seismic Response of Field Fabricated Liquefied Natural Gas (LNG) Spherical Storage Vessels
Egieerig, 013, 5, 543-550 doi:10.436/eg.013.56065 Published Olie Jue 013 (http://www.scirp.org/joural/eg) Fiite Elemet Modelig of Seismic Respose of Field Fabricated Liquefied Natural Gas (LNG) Spherical
More informationLecture 6 Chi Square Distribution (χ 2 ) and Least Squares Fitting
Lecture 6 Chi Square Distributio (χ ) ad Least Squares Fittig Chi Square Distributio (χ ) Suppose: We have a set of measuremets {x 1, x, x }. We kow the true value of each x i (x t1, x t, x t ). We would
More informationApplication of Dynamic Relaxation in Thermo-Elastic Structural Analysis of Highway Pavement Structures
9 th Iteratioal LS-DYNA Users Coferece Simulatio Techology () Applicatio of Dyamic Relaxatio i Thermo-Elastic Structural Aalysis of Highway Pavemet Structures Samir N. Shoukry, Gergis W. William, Mourad
More informationPrinciple Of Superposition
ecture 5: PREIMINRY CONCEP O RUCUR NYI Priciple Of uperpositio Mathematically, the priciple of superpositio is stated as ( a ) G( a ) G( ) G a a or for a liear structural system, the respose at a give
More informationDynamic Programming. Sequence Of Decisions
Dyamic Programmig Sequece of decisios. Problem state. Priciple of optimality. Dyamic Programmig Recurrece Equatios. Solutio of recurrece equatios. Sequece Of Decisios As i the greedy method, the solutio
More informationDynamic Programming. Sequence Of Decisions. 0/1 Knapsack Problem. Sequence Of Decisions
Dyamic Programmig Sequece Of Decisios Sequece of decisios. Problem state. Priciple of optimality. Dyamic Programmig Recurrece Equatios. Solutio of recurrece equatios. As i the greedy method, the solutio
More informationADVANCED DIGITAL SIGNAL PROCESSING
ADVANCED DIGITAL SIGNAL PROCESSING PROF. S. C. CHAN (email : sccha@eee.hku.hk, Rm. CYC-702) DISCRETE-TIME SIGNALS AND SYSTEMS MULTI-DIMENSIONAL SIGNALS AND SYSTEMS RANDOM PROCESSES AND APPLICATIONS ADAPTIVE
More informationModification of Arrhenius Model for Numerical Modelling of Turbulent Flames
J. Basic. Appl. Sci. Res., (5)480-486, 01 01, TextRoad Publicatio ISSN 090-4304 Joural of Basic ad Applied Scietific Research www.textroad.com Modificatio of Arrheius Model for Numerical Modellig of Turbulet
More informationA STUDY OF VIBRATION MEASURING AND FATIGUE ANALYSIS FOR CANTILEVER BEAMS
Joural of Techology, Vol. 3, No., pp. 47-56 (07) 47, * LabView ANSYS A STUDY OF VIBRATION MEASURING AND FATIGUE ANALYSIS FOR CANTILEVER BEAMS Yuo-Ter Tsai, * Hsie-Yag Li Departmet of Mechaical Egieerig
More informationTHE ENERGY BALANCE ERROR FOR CIRCUIT TRANSIENT ANALYSIS
THE ENERGY BALANCE ERROR FOR CIRCUIT TRANSIENT ANALYSIS FLORIN CONSTANTINESCU, ALEXANDRU GABRIEL GHEORGHE, MIRUNA NIŢESCU Key words: Trasiet aalysis, Eergy balace error, Time step coice. Two algoritms
More informationLecture 6 Chi Square Distribution (χ 2 ) and Least Squares Fitting
Lecture 6 Chi Square Distributio (χ ) ad Least Squares Fittig Chi Square Distributio (χ ) Suppose: We have a set of measuremets {x 1, x, x }. We kow the true value of each x i (x t1, x t, x t ). We would
More informationAnalysis of Algorithms. Introduction. Contents
Itroductio The focus of this module is mathematical aspects of algorithms. Our mai focus is aalysis of algorithms, which meas evaluatig efficiecy of algorithms by aalytical ad mathematical methods. We
More informationChapter 5 Vibrational Motion
Fall 4 Chapter 5 Vibratioal Motio... 65 Potetial Eergy Surfaces, Rotatios ad Vibratios... 65 Harmoic Oscillator... 67 Geeral Solutio for H.O.: Operator Techique... 68 Vibratioal Selectio Rules... 7 Polyatomic
More information8. СОВЕТУВАЊЕ. Охрид, септември ANALYSIS OF NO LOAD APPARENT POWER AND FREQUENCY SPECTRUM OF MAGNETIZING CURRENT FOR DIFFERENT CORE TYPES
8. СОВЕТУВАЊЕ Охрид, 22 24 септември Leoardo Štrac Frajo Keleme Kočar Power Trasformers Ltd. ANALYSS OF NO LOAD APPARENT POWER AND FREQENCY SPECTRM OF MAGNETZNG CRRENT FOR DFFERENT CORE TYPES ABSTRACT
More informationSTA6938-Logistic Regression Model
Dr. Yig Zhag STA6938-Logistic Regressio Model Topic -Simple (Uivariate) Logistic Regressio Model Outlies:. Itroductio. A Example-Does the liear regressio model always work? 3. Maximum Likelihood Curve
More informationOrthogonal Gaussian Filters for Signal Processing
Orthogoal Gaussia Filters for Sigal Processig Mark Mackezie ad Kiet Tieu Mechaical Egieerig Uiversity of Wollogog.S.W. Australia Abstract A Gaussia filter usig the Hermite orthoormal series of fuctios
More informationNew Exponential Strengthening Buffer Operators and Numerical Simulation
Sesors & Trasducers, Vol. 59, Issue, November 0, pp. 7-76 Sesors & Trasducers 0 by IFSA http://www.sesorsportal.com New Expoetial Stregtheig Buffer Operators ad Numerical Simulatio Cuifeg Li, Huajie Ye,
More informationEECS 442 Computer vision. Multiple view geometry Affine structure from Motion
EECS 442 Computer visio Multiple view geometry Affie structure from Motio - Affie structure from motio problem - Algebraic methods - Factorizatio methods Readig: [HZ] Chapters: 6,4,8 [FP] Chapter: 2 Some
More informationAnalysis of Foundation-Layered Soil Interaction Using Propagating Wave-modes Analysis
Aalysis of Foudatio-Layered Soil Iteractio Usig Propagatig Wave-modes Aalysis IGOR ŠPACAPAN & MIROSLAV PREMROV Faculty of Civil Egieerig Uiversity of Maribor Smetaova 7, Maribor SLOVENIA Abstract: - I
More informationVisco-acoustic Reverse-time Migration Using the Pseudo-analytical Method
Visco-acoustic Reverse-time Migratio Usig the Pseudo-aalytical Method J. Ramos-Martiez* (Petroleum Geo-Services), A.A. Valeciao (Petroleum Geo-Services) & M. Orlovich (Petroleum Geo-Services) SUMMARY We
More informationA Simplified Derivation of Scalar Kalman Filter using Bayesian Probability Theory
6th Iteratioal Workshop o Aalysis of Dyamic Measuremets Jue -3 0 Göteorg Swede A Simplified Derivatio of Scalar Kalma Filter usig Bayesia Proaility Theory Gregory Kyriazis Imetro - Electrical Metrology
More informationDECOMPOSITION METHOD FOR SOLVING A SYSTEM OF THIRD-ORDER BOUNDARY VALUE PROBLEMS. Park Road, Islamabad, Pakistan
Mathematical ad Computatioal Applicatios, Vol. 9, No. 3, pp. 30-40, 04 DECOMPOSITION METHOD FOR SOLVING A SYSTEM OF THIRD-ORDER BOUNDARY VALUE PROBLEMS Muhammad Aslam Noor, Khalida Iayat Noor ad Asif Waheed
More informationChapter 12 EM algorithms The Expectation-Maximization (EM) algorithm is a maximum likelihood method for models that have hidden variables eg. Gaussian
Chapter 2 EM algorithms The Expectatio-Maximizatio (EM) algorithm is a maximum likelihood method for models that have hidde variables eg. Gaussia Mixture Models (GMMs), Liear Dyamic Systems (LDSs) ad Hidde
More informationBIOSTATISTICS. Lecture 5 Interval Estimations for Mean and Proportion. dr. Petr Nazarov
Microarray Ceter BIOSTATISTICS Lecture 5 Iterval Estimatios for Mea ad Proportio dr. Petr Nazarov 15-03-013 petr.azarov@crp-sate.lu Lecture 5. Iterval estimatio for mea ad proportio OUTLINE Iterval estimatios
More informationTESTING OF THE FORCES IN CABLE OF SUSPENSION STRUCTURE AND BRIDGES
TSTING OF TH FORCS IN CABL OF SUSPNSION STRUCTUR AND BRIDGS Zhou, M. 1, Liu, Z. ad Liu, J. 1 College of the Muicipal Techology, Guagzhou Uiversity, Guagzhou. Guagzhou Muicipal ad Ladscape gieerig Quality
More informationNumerical Solution of the Two Point Boundary Value Problems By Using Wavelet Bases of Hermite Cubic Spline Wavelets
Australia Joural of Basic ad Applied Scieces, 5(): 98-5, ISSN 99-878 Numerical Solutio of the Two Poit Boudary Value Problems By Usig Wavelet Bases of Hermite Cubic Splie Wavelets Mehdi Yousefi, Hesam-Aldie
More informationUsing SAS to Evaluate Integrals and Reverse Functions in Power and Sample Size Calculations
Usig SAS to Evaluate Itegrals ad everse Fuctios i Power ad Sample Size Calculatios Xigshu Zhu, Merck &Co., Ic. Blue Bell, PA 94 Shupig Zhag, Merck &Co., Ic. Blue Bell, PA 94 ABSTACT We have recetly created
More informationBayesian Control Charts for the Two-parameter Exponential Distribution
Bayesia Cotrol Charts for the Two-parameter Expoetial Distributio R. va Zyl, A.J. va der Merwe 2 Quitiles Iteratioal, ruaavz@gmail.com 2 Uiversity of the Free State Abstract By usig data that are the mileages
More informationHarmonic balance approaches to the nonlinear oscillators in which the restoring force is inversely proportional to the dependent variable
Joural of Soud ad Vibratio, Vol. 314, Nº 3-5, 775-78 (008) Harmoic balace approaches to the oliear oscillators i which the restorig force is iversely proportioal to the depedet variable A. Belédez, D.
More informationStability Analysis and Bifurcation Control of Hysteresis Current Controlled Ćuk Converter Using Filippov s Method
Stability Aalysis ad Bifurcatio otrol of Hysteresis urret otrolled Ću overter Usig Filippov s Method I. Daho*, D. Giaouris * (Member IE, B. Zahawi*(Member IE, V. Picer*(Member IE ad S. Baerjee** *School
More informationSignal Processing in Mechatronics
Sigal Processig i Mechatroics Zhu K.P. AIS, UM. Lecture, Brief itroductio to Sigals ad Systems, Review of Liear Algebra ad Sigal Processig Related Mathematics . Brief Itroductio to Sigals What is sigal
More informationSome New Iterative Methods for Solving Nonlinear Equations
World Applied Scieces Joural 0 (6): 870-874, 01 ISSN 1818-495 IDOSI Publicatios, 01 DOI: 10.589/idosi.wasj.01.0.06.830 Some New Iterative Methods for Solvig Noliear Equatios Muhammad Aslam Noor, Khalida
More informationLOSS-MINIMIZATION CONTROL OF SCALAR- CONTROLLED INDUCTION MOTOR DRIVES
LOSS-MINIMIZATION CONTROL OF SCALAR- CONTROLLED INDUCTION MOTOR DRIVES Hussei Sarha, Rateb Al-Issa, ad Qazem Jaber Departmet of Mechatroics Egieerig, Faculty of Egieerig Techology Al-Balqa Applied Uiversity,
More informationAddition: Property Name Property Description Examples. a+b = b+a. a+(b+c) = (a+b)+c
Notes for March 31 Fields: A field is a set of umbers with two (biary) operatios (usually called additio [+] ad multiplicatio [ ]) such that the followig properties hold: Additio: Name Descriptio Commutativity
More informationPOWER SERIES SOLUTION OF FIRST ORDER MATRIX DIFFERENTIAL EQUATIONS
Joural of Applied Mathematics ad Computatioal Mechaics 4 3(3) 3-8 POWER SERIES SOLUION OF FIRS ORDER MARIX DIFFERENIAL EQUAIONS Staisław Kukla Izabela Zamorska Istitute of Mathematics Czestochowa Uiversity
More informationASYMPTOTIC CLOSED-LOOP DESIGN OF ERROR RESILIENT PREDICTIVE COMPRESSION SYSTEMS. Sina Zamani, Tejaswi Nanjundaswamy, Kenneth Rose
ASYMPTOTIC OSED-LOOP DESIGN OF ERROR RESILIENT PREDICTIVE COMPRESSION SYSTEMS Sia Zamai, Tejaswi Najudaswamy, Keeth Rose Departmet of Electrical ad Computer Egieerig, Uiversity of Califoria Sata Barbara,
More informationDamped Vibration of a Non-prismatic Beam with a Rotational Spring
Vibratios i Physical Systems Vol.6 (0) Damped Vibratio of a No-prismatic Beam with a Rotatioal Sprig Wojciech SOCHACK stitute of Mechaics ad Fudametals of Machiery Desig Uiversity of Techology, Czestochowa,
More informationNotes on iteration and Newton s method. Iteration
Notes o iteratio ad Newto s method Iteratio Iteratio meas doig somethig over ad over. I our cotet, a iteratio is a sequece of umbers, vectors, fuctios, etc. geerated by a iteratio rule of the type 1 f
More informationModeling of Finite Gradient Elasticity Using Optimal Transportation Method
9 th Iteratioal Cogress of Croatia Society of Mechaics 18-22 September 2018 Split, Croatia Modelig of Fiite Gradiet Elasticity Usig Optimal Trasportatio Method Boris JALUŠIĆ *, Christia WEIßENFELS +, Jurica
More information