OPTIMAL PLACEMENT AND UTILIZATION OF PHASOR MEASUREMENTS FOR STATE ESTIMATION

Size: px
Start display at page:

Download "OPTIMAL PLACEMENT AND UTILIZATION OF PHASOR MEASUREMENTS FOR STATE ESTIMATION"

Transcription

1 OPTIMAL PLACEMENT AND UTILIZATION OF PHASOR MEASUREMENTS FOR STATE ESTIMATION Xu Bei, Yeo Jun Yoon and Ali Abur Teas A&M University College Station, Teas, U.S.A. Abstract This paper presents a procedure by which new PMU locations can be systematically determined in order to render an observable system. The procedure is then etended to account or cases o loss o a single phasor measurement unit (PMU). Buses with zero and nonzero injections, and branches with power low measurements are also accounted or in this generalized procedure. Several cases involving dierent power system and measurement conigurations are presented where introducing ew etra strategically placed PMUs minimizes vulnerability o the measurement system against the loss o single PMUs. The paper also develops a linear estimator based on strictly PMU measurements and investigates the computational perormance as well as the bad data processing problem. Detection and identiication o PMU ailures are demonstrated via simulations. Keywords: State estimation, phasor measurement units, network observability, optimal meter placement, bad data processing, integer programming, graph theory. INTRODUCTION State estimators provide optimal estimates o bus voltage phasors based on the available measurements and knowledge about the network topology. Until recently, available measurement sets did not contain phase angle measurements due to the technical diiculties associated with the synchronization o measurements at remote locations. Global positioning satellite (GPS) technology alleviated these diiculties and lead to the development o phasor measurement units (PMU). As the PMUs become more and more aordable, their utilization will increase not only or substation applications but also at the control centers or the EMS applications. One o the applications, which will be signiicantly aected by the introduction o PMUs, is the state estimator. This paper is concerned with two aspects o this issue. One is related to the proper placement and the other to the eective utilization o these new devices or state estimation. The idea o using direct phasor measurements or system monitoring applications including the speciic case o state estimation is not new. Earlier work done by Phadke and his co-workers [-] introduces the use o PMUs or such applications. This work is later etended to the investigation o optimal location o PMUs where each PMU is assumed to provide voltage and current measurements at its associated bus and all incident branches []. It is thereore possible to ully monitor the system by using relatively less number o PMUs than the number o system buses. This problem is solved by using a graph theoretic observability analysis and an optimization method based on Simulated Annealing in []. Possible loss or ailure o PMUs is not considered in that study. In this paper, a numerical ormulation o the optimal PMU placement problem will be presented. Preliminary results, which do not account or the loss o PMUs are presented in [] earlier. This ormulation leads to a solution based on integer programming and also acilitates analysis o network observability. Furthermore, it is general enough to account or loss o single PMUs, eistence o zero and non-zero power injections and power low measurements. Using the measurement design ound by this method, the paper investigates the perormance o linear estimators that eclusively use PMUs and describes detection and identiication o ailed PMUs by using the residual based bad data processing methods. STATE ESTIMATION USING PHASOR MEASUREMENTS. State Estimation Measurements that are telemetered rom the substations are processed at the control centers by the state estimator. State estimator provides the optimal estimate o the system state based on the received measurements and the knowledge o the network model. Measurements may include the ollowing: - Power injections (real/reactive), - Power lows (real/reactive), - Bus voltage magnitude, - Line current magnitude, - Current injection magnitude. PMUs provide two other types o measurements, namely bus voltage phasors and branch current phasors. Depending on the type o PMUs used the number o channels used or measuring voltage and current phasors will vary. In this study, it is assumed that each PMU has enough channels to record the bus voltage phasor at its associated bus and current phasors along all branches that are incident to this bus.

2 State estimation can be ormulated as an optimization problem and solved using an appropriate numerical method. A common choice or the objective unction is the weighted sum o the measurement residual squares, which leads to the well known weighted least squares (WLS) state estimation solution. Formulation and solution methods or WLS state estimation when using the above-itemized conventional measurements are well documented in the literature and can be ound or instance in []. Incorporating phasor measurements to an eisting state estimator will require augmenting various arrays such as the measurement vector and the measurement Jacobian while not aecting the state vector. In that sense, the required modiications are not substantial and the overall problem ormulation does not change signiicantly. On the other hand, i enough PMUs eist to make the entire system observable based eclusively on PMU measurements, then the state estimation problem can be ormulated in a slightly simpler manner. In this case, the relation between the measured phasors and the system states will become linear yielding the ollowing linear measurement model: z = H + e () where: z : is the measurement vector containing the real and imaginary parts o the measured voltage and current phasors. H : is the measurement Jacobian, which is constant and a unction o the network model parameters only. : is the state vector containing the real and imaginary parts o bus voltage phasors. e: is the measurement error vector. This measurement model will lead to a linear state estimator, which will be given by the ollowing equation: T ˆ = G H R z () where: ˆ : is the estimated system state. T G = H R H : is the constant gain matri. T R = E{ e e ) : is the diagonal error covariance matri.. Bad Data Processing Note that several measurements will be associated with a single PMU in the measurement vector, z. In case o an error or ailure o a PMU, this will contaminate all measurements provided by that PMU. Bad data detection and identiication schemes typically process individual measurements and thereore they need to be used repeatedly on the aected measurements o the PMU in order to identiy the aulty PMU. This is accomplished by irst applying the largest normalized residual test to the measurements and then eliminating bad measurements one at a time in a cyclic manner. Due to the interactive nature o the measurements associated with a single PMU, they are vulnerable to error masking and possible misidentiication o bad data. Fortunately, this occurs when errors are conorming which is typically the case i there are topology errors. PLACEMENT OF PHASOR MEASUREMENTS The objective o PMU placement is to make the entire system observable using a minimum number o PMUs. This objective will be slightly modiied later in section. to account or loss o single PMUs. One o the assumptions about the considered PMUs is that each PMU has enough channels to measure bus voltage and all incident branch current phasors at a given bus. Discrete nature o the problem naturally results in deinition o a vector X o binary (/) decision variables, i as given below: i = i a PMU is installed at bus i otherwise Inner product o this binary vector and a vector containing corresponding installation costs o these PMUs, will be deined as the objective unction o the optimization problem. Constraints will be added in order to ensure ull network observability while minimizing the total installation cost o the PMUs. For an n-bus system, this optimization problem takes the ollowing orm: minimize subject to n w i i i ( X ) ˆ where: w i : is the installation cost o the PMU at bus i. ( X ) : is a vector unction representing the constraints. Its entries are non-zero i the corresponding bus voltage is solvable using the given measurement set and zero otherwise. ˆ : is a vector whose entries are all equal to. Proper deinition o the constraint vector unction, (X) is the key to the presented ormulation. Depending on the type o measurement system, this deinition will change, while the objective unction will remain the same. In order to simpliy the description o the constraint unction, it will be given using a small tutorial eample containing buses. Three cases will be discussed, where the eisting system has: - No measurements at all and no zero injections, - Zero and nonzero power injections, - Power injections and power lows. Network diagram or the -bus eample system is shown in Figure. Initially, or case, both o the conventional measurements, namely the power injection measurement at bus (dot shown net to bus ) and the power low measurement on line - (solid () ()

3 square shown on line -) will be ignored. They will be gradually taken into account in cases and. Figure : Network diagram or the -bus system. Case : A system, which has no conventional measurements and/or zero injections Since it is assumed that a given PMU will provide phasors or the currents along branches that connect this bus to all its neighbors, once a bus is assigned a PMU, phasor voltages at all o its neighbors will be assumed to be known or solvable. An easy way to determine all such solvable buses is by using the binary connectivity matri A as deined below: i k = m A k, m = i k and m are connected () i otherwise This yields the ollowing matri or the -bus system o Figure : A = Taking the product o this matri and the binary decision vector X will provide the desired vector unction. Elements o this vector unction will be at least equal to one, i at least one neighbor o the corresponding bus is assigned a PMU. Hence, the constraint equations or the above eample or this case will be ormed as: ( X ) = A X = = + + () The operator + serves as the logical OR and the use o in the right hand side o the inequality ensures that at least one o the variables appearing in the sum will be non-zero. For eample, consider the constraints associated with bus and as given below: The irst constraint implies that at least one PMU must be placed at either one o buses or (or both) in order to make bus observable. Similarly, the second constraint indicates that at least one PMU should be installed at any one o the buses,,,, or in order to make bus observable.. Case : A system, which contains zero and nonzero injection measurements In this case, the injection measurement at bus will be taken into account when determining the PMU locations. Note that i the phasor voltages at any three out o our buses,, and are known, then the ourth one can be solved using the Kirchho s Current Law applied at bus where the net injected current is known. This observation allows a topology transormation where the bus, which has the injection measurement can be merged with any one o its neighbors. Injection measurements whether they are actual measurements or zero injections, are treated the same way. A word o caution needs to be added here in that, i the optimal solution chooses the newly ormed ictitious bus (merger o two actual buses) as a candidate bus, it may place one PMU on one o these two buses or two PMUs on both. In this paper, a topology analysis is applied to check the observability o the system once this happens. This also assures that the minimum number o PMUs will be placed. Figure shows the updated system diagram ater the merger o buses and into a new bus. The newly created branch - relects the original connection between buses and. Binary connection matri A or this case is given below: : A = () Hence, the constraints vector unction will be given

4 = = ( X ) (8) = + Figure : System diagram ater the merger o buses and.. Case : A system, which contains injections as well as low measurements. This case considers the most general situation where both injection and low measurements may be present, but not enough to make the entire system observable. So, the objective is to place PMUs in order to merge the observable islands ormed by the eisting conventional measurements and render a ully observable system. Flow measurement on branch - in the -bus eample system will be used to illustrate the approach. Eistence o this low measurement will lead to the modiication o the constraints or buses and accordingly. Modiication ollows the observation that having a low measurement along a given branch allows the calculation o one o the terminal bus voltage phasors when the other one is known. Hence, the constraint equations associated with the terminal buses o the measured branch can be merged into a single constraint. In the case o the eample system, the constraints or buses and are merged into a joint constraint as ollows: _ new = + Note that this new constraint ensures that i either one o the voltage phasors at buses or is observable, then the other one will also be observable. Applying this modiication to the constraints the ollowing set o inal constraints will be obtained: _ new = ( X ) = = + +. Placement strategy against loss o a single PMU So ar it is assumed that those PMUs which are placed by the proposed method, will unction perectly. While PMUs are highly reliable, they are prone to ailure just like any other measuring device. In order to guard against such unepected ailures o PMUs, the above placement strategy is etended to account or single PMU loss. In this paper, this objective is achieved by choosing two independent PMU sets, a primary set and a backup set, each o which can make the system observable on its own. I any PMU is lost, the other set o PMUs will guarantee the observability o the system. The primary set o PMUs is chosen by building the constraint unctions according to the procedures described in subsections above and solving the integerprogramming problem. The backup set is chosen by removing all the terms in the constraint unctions, i where bus i is in the primary set, in order to avoid picking up the same bus which appears in primary set. Then the integer-programming problem is solved to obtain the backup set. SIMULATION RESULTS Simulations are carried out on the IEEE -bus, IEEE -bus and IEEE 8-bus systems.. Case. In case, two groups o simulations are carried out on the three test systems, which initially have no low measurements. Loss o PMUs is not considered in this case. In the irst group o simulations, zero injections are simply ignored while in the second group, they are used as eisting measurements. Comparative simulation results are shown in Table. Having zero injections will reduce the number o required PMUs as can be seen rom these results. SYSTEMS NO. OF ZERO NUMBER OF PMUS IGNORING ZERO USING ZERO IEEE-BUS IEEE -BUS IEEE 8-BUS 9 Table : Results with and without considering zero injections

5 . Case. In this case, simulations o case are repeated by accounting or loss o single PMUs. Primary and backup locations are ound and combined results are shown in Table. SYSTEMS NO. OF ZERO NUMBER OF PMUS IGNORING ZERO USING ZERO IEEE -BUS 9 IEEE -BUS IEEE 8-BUS Table : Results considering loss o single PMUs. Case. In this case simulations are carried out using IEEE 8-bus system. Three sets o low measurements (P and Q) containing low measurements each, are added in the system one at a time. The locations o these low measurements in the system are given in Table. Simulation results are shown in Table. The required number o PMUs is reduced rom 9 to. Hence, as epected, having conventional measurements reduces the number o required PMUs to make the entire system observable. MEAS. FLOW MEASUREMENTS IN THE SET SET NO Table : Locations o low measurements used or case. SYSTEM IEEE 8-BUS FLOW MEASUREMENT SET Table : Simulation results or case. NUMBER OF PMUS NONE 9 AND, AND. Linear State Estimation using PMUs Perormance o the linear state estimator, which uses only PMU measurements, is evaluated by simulations. Due to space limitations PMU locations are shown only or the -bus system in Figure. Computation times, the number o PMUs and state variables are given or dierent size systems in Table. It is noted that, zero injections are not used in these simulations. Figure : PMU locations or the bus system (ignoring zero injections) Following these simulations, these test systems are used to simulate single PMU ailure cases. Bad PMU detection and identiication requires redundancy. This is accomplished by adding etra PMUs at buses and or the -bus system and PMU at bus 9 or the 8-bus system. System No o States No o PMUs CPU time (sec) Table : CPU times or the linear state estimator. Bad PMU is simulated by introducing errors to all measurements provided by the same PMU. Denoting voltage phasor components as V=E+jF and current phasor components as I=C+jD, the ollowing measurements are simulated as bad data: For the -bus system: V(), I(,), I(,) For the 8-bus system: V(9), I(9,), I(9,). Bad data processing is carried out using the cyclic application o the largest normalized residual test as discussed in section. above. Test results or both systems are shown in Tables and. BD ident. cycle Eliminated meas. Sorted Normalized Residuals st nd rd th E () /. E () / 98. E () / 9. C (,) /. C (,) /. C (,) /. C (,) /. C (,) / 8. C (,) /. C (,9) /.8 C (9,) /.8 C (,) /. V () I (,) I (,) No More Bad data

6 Table : Bad data identiication cycles or -bus system with a bad PMU at bus. Bad components o voltage and current phasors are correctly identiied and eliminated thanks to locally redundant measurement conigurations or both cases. As discussed in section., it is possible to guarantee bad PMU detection and identiication by making sure that none o the PMUs are critical. This can be achieved by the measurement design proposed in section.. Cost associated with such a design versus the beneits o bad PMU detection capability can be evaluated. CONCLUSIONS This paper is concerned with two issues related to the phasor measurement units. The irst issue is proper placement o these devices or a given budget. This issue is addressed via a - integer programming method, where injections and power low measurements are also considered. As a urther consideration, loss o single PMUs is also taken into account to minimize the vulnerability o state estimation to PMU ailures. Once placed, the utilization o PMUs or state estimation is investigated. Potential beneits o incorporating these devices into the eisting measurement set, both rom the point o view o bad data elimination as well as computational perormance, are identiied and illustrated by simulated eamples. REFERENCES BD identiication cycle Eliminated meas. Sorted Normalized Residuals in Descending Order st nd rd th E (9) / 88.8 C(9,) /. E () /. C(9,) /.8 C (9,) /. C(,9) /. C (9.) /.8 C (,9) / 9. C (,9) /. E (8) /. E () /. E (8) /.98 V (9) I (9,) I (9,) No More Bad Data Table : Bad data identiication cycles or 8-bus system with a bad PMU at bus 9. [] A. G. Phadke, Synchronized phasor measurements in power systems, IEEE Computer Applications in Power, Vol., Issue, pp. -, April 99. [] A. G. Phadke, J. S. Thorp, and K. J. Karimi, State Estimation with Phasor Measurements, IEEE Transactions on Power Systems, Vol., No., pp. -, February 98. [] T. L. Baldwin, L. Mili, M. B. Boisen, and R. Adapa, Power System Observability With Minimal Phasor Measurement Placement, IEEE Transactions on Power Systems, Vol. 8, No., pp. -, May 99. [] Bei Xu and A. Abur, Observability Analysis and Measurement Placement or Systems with PMUs, Proceedings o the IEEE PES Power Systems Conerence and Eposition, October -,, New York, NY. [] A. Abur and A.G. Eposito, Power System State Estimation, Marcel Dekker,.

Role of Synchronized Measurements In Operation of Smart Grids

Role of Synchronized Measurements In Operation of Smart Grids Role of Synchronized Measurements In Operation of Smart Grids Ali Abur Electrical and Computer Engineering Department Northeastern University Boston, Massachusetts Boston University CISE Seminar November

More information

Mixed Integer Linear Programming and Nonlinear Programming for Optimal PMU Placement

Mixed Integer Linear Programming and Nonlinear Programming for Optimal PMU Placement Mied Integer Linear Programg and Nonlinear Programg for Optimal PMU Placement Anas Almunif Department of Electrical Engineering University of South Florida, Tampa, FL 33620, USA Majmaah University, Al

More information

Fine Tuning Of State Estimator Using Phasor Values From Pmu s

Fine Tuning Of State Estimator Using Phasor Values From Pmu s National conference on Engineering Innovations and Solutions (NCEIS 2018) International Journal of Scientific Research in Computer Science, Engineering and Information Technology 2018 IJSRCSEIT Volume

More information

Optimal PMU Placement for Power System State Estimation with Random Communication Packet Losses

Optimal PMU Placement for Power System State Estimation with Random Communication Packet Losses 2011 9th IEEE International Conference on Control and Automation (ICCA) Santiago, Chile, December 19-21, 2011 TueB1.1 Optimal PMU Placement for Power System State Estimation with Random Communication Packet

More information

Improvement of Sparse Computation Application in Power System Short Circuit Study

Improvement of Sparse Computation Application in Power System Short Circuit Study Volume 44, Number 1, 2003 3 Improvement o Sparse Computation Application in Power System Short Circuit Study A. MEGA *, M. BELKACEMI * and J.M. KAUFFMANN ** * Research Laboratory LEB, L2ES Department o

More information

Critical Measurement Set with PMU for Hybrid State Estimation

Critical Measurement Set with PMU for Hybrid State Estimation 6th NATIONAL POWER SYSTEMS CONFERENCE, 5th-th DECEMBER, 200 25 Critical Measurement Set with for Hybrid State Estimation K.Jamuna and K.S.Swarup Department of Electrical Engineering Indian Institute of

More information

Optimal Placement of PMUs in Power Systems Using Mixed Integer Non Linear Programming and Bacterial Foraging Algorithm

Optimal Placement of PMUs in Power Systems Using Mixed Integer Non Linear Programming and Bacterial Foraging Algorithm 150 ECTI TRANSACTIONS ON ELECTRICAL ENG., ELECTRONICS, AND COMMUNICATIONS VOL.9, NO.1 February 2011 Optimal Placement of PMUs in Power Systems Using Mixed Integer Non Linear Programming and Bacterial Foraging

More information

Numerical Methods - Lecture 2. Numerical Methods. Lecture 2. Analysis of errors in numerical methods

Numerical Methods - Lecture 2. Numerical Methods. Lecture 2. Analysis of errors in numerical methods Numerical Methods - Lecture 1 Numerical Methods Lecture. Analysis o errors in numerical methods Numerical Methods - Lecture Why represent numbers in loating point ormat? Eample 1. How a number 56.78 can

More information

We would now like to turn our attention to a specific family of functions, the one to one functions.

We would now like to turn our attention to a specific family of functions, the one to one functions. 9.6 Inverse Functions We would now like to turn our attention to a speciic amily o unctions, the one to one unctions. Deinition: One to One unction ( a) (b A unction is called - i, or any a and b in the

More information

NONLINEAR CONTROL OF POWER NETWORK MODELS USING FEEDBACK LINEARIZATION

NONLINEAR CONTROL OF POWER NETWORK MODELS USING FEEDBACK LINEARIZATION NONLINEAR CONTROL OF POWER NETWORK MODELS USING FEEDBACK LINEARIZATION Steven Ball Science Applications International Corporation Columbia, MD email: sball@nmtedu Steve Schaer Department o Mathematics

More information

Objectives. By the time the student is finished with this section of the workbook, he/she should be able

Objectives. By the time the student is finished with this section of the workbook, he/she should be able FUNCTIONS Quadratic Functions......8 Absolute Value Functions.....48 Translations o Functions..57 Radical Functions...61 Eponential Functions...7 Logarithmic Functions......8 Cubic Functions......91 Piece-Wise

More information

ADVANCEMENTS IN TRANSMISSION LINE FAULT LOCATION

ADVANCEMENTS IN TRANSMISSION LINE FAULT LOCATION University o Kentucy UKnowledge University o Kentucy Doctoral Dissertations Graduate School 2010 ADVANCEMENTS IN TRANSMISSION LINE FAULT LOCATION Ning Kang University o Kentucy, glucenama@hotmail.com Clic

More information

MEASUREMENTS that are telemetered to the control

MEASUREMENTS that are telemetered to the control 2006 IEEE TRANSACTIONS ON POWER SYSTEMS, VOL. 19, NO. 4, NOVEMBER 2004 Auto Tuning of Measurement Weights in WLS State Estimation Shan Zhong, Student Member, IEEE, and Ali Abur, Fellow, IEEE Abstract This

More information

( x) f = where P and Q are polynomials.

( x) f = where P and Q are polynomials. 9.8 Graphing Rational Functions Lets begin with a deinition. Deinition: Rational Function A rational unction is a unction o the orm ( ) ( ) ( ) P where P and Q are polynomials. Q An eample o a simple rational

More information

Differentiation. The main problem of differential calculus deals with finding the slope of the tangent line at a point on a curve.

Differentiation. The main problem of differential calculus deals with finding the slope of the tangent line at a point on a curve. Dierentiation The main problem o dierential calculus deals with inding the slope o the tangent line at a point on a curve. deinition() : The slope o a curve at a point p is the slope, i it eists, o the

More information

(One Dimension) Problem: for a function f(x), find x 0 such that f(x 0 ) = 0. f(x)

(One Dimension) Problem: for a function f(x), find x 0 such that f(x 0 ) = 0. f(x) Solving Nonlinear Equations & Optimization One Dimension Problem: or a unction, ind 0 such that 0 = 0. 0 One Root: The Bisection Method This one s guaranteed to converge at least to a singularity, i not

More information

9.1 The Square Root Function

9.1 The Square Root Function Section 9.1 The Square Root Function 869 9.1 The Square Root Function In this section we turn our attention to the square root unction, the unction deined b the equation () =. (1) We begin the section

More information

9.3 Graphing Functions by Plotting Points, The Domain and Range of Functions

9.3 Graphing Functions by Plotting Points, The Domain and Range of Functions 9. Graphing Functions by Plotting Points, The Domain and Range o Functions Now that we have a basic idea o what unctions are and how to deal with them, we would like to start talking about the graph o

More information

RATIONAL FUNCTIONS. Finding Asymptotes..347 The Domain Finding Intercepts Graphing Rational Functions

RATIONAL FUNCTIONS. Finding Asymptotes..347 The Domain Finding Intercepts Graphing Rational Functions RATIONAL FUNCTIONS Finding Asymptotes..347 The Domain....350 Finding Intercepts.....35 Graphing Rational Functions... 35 345 Objectives The ollowing is a list o objectives or this section o the workbook.

More information

Lecture 8 Optimization

Lecture 8 Optimization 4/9/015 Lecture 8 Optimization EE 4386/5301 Computational Methods in EE Spring 015 Optimization 1 Outline Introduction 1D Optimization Parabolic interpolation Golden section search Newton s method Multidimensional

More information

«Develop a better understanding on Partial fractions»

«Develop a better understanding on Partial fractions» «Develop a better understanding on Partial ractions» ackground inormation: The topic on Partial ractions or decomposing actions is irst introduced in O level dditional Mathematics with its applications

More information

Supplementary material for Continuous-action planning for discounted infinite-horizon nonlinear optimal control with Lipschitz values

Supplementary material for Continuous-action planning for discounted infinite-horizon nonlinear optimal control with Lipschitz values Supplementary material or Continuous-action planning or discounted ininite-horizon nonlinear optimal control with Lipschitz values List o main notations x, X, u, U state, state space, action, action space,

More information

OBSERVER/KALMAN AND SUBSPACE IDENTIFICATION OF THE UBC BENCHMARK STRUCTURAL MODEL

OBSERVER/KALMAN AND SUBSPACE IDENTIFICATION OF THE UBC BENCHMARK STRUCTURAL MODEL OBSERVER/KALMAN AND SUBSPACE IDENTIFICATION OF THE UBC BENCHMARK STRUCTURAL MODEL Dionisio Bernal, Burcu Gunes Associate Proessor, Graduate Student Department o Civil and Environmental Engineering, 7 Snell

More information

Robust Residual Selection for Fault Detection

Robust Residual Selection for Fault Detection Robust Residual Selection or Fault Detection Hamed Khorasgani*, Daniel E Jung**, Gautam Biswas*, Erik Frisk**, and Mattias Krysander** Abstract A number o residual generation methods have been developed

More information

Probabilistic Optimisation applied to Spacecraft Rendezvous on Keplerian Orbits

Probabilistic Optimisation applied to Spacecraft Rendezvous on Keplerian Orbits Probabilistic Optimisation applied to pacecrat Rendezvous on Keplerian Orbits Grégory aive a, Massimiliano Vasile b a Université de Liège, Faculté des ciences Appliquées, Belgium b Dipartimento di Ingegneria

More information

Analog Computing Technique

Analog Computing Technique Analog Computing Technique by obert Paz Chapter Programming Principles and Techniques. Analog Computers and Simulation An analog computer can be used to solve various types o problems. It solves them in

More information

Smart Grid State Estimation by Weighted Least Square Estimation

Smart Grid State Estimation by Weighted Least Square Estimation International Journal of Engineering and Advanced Technology (IJEAT) ISSN: 2249 8958, Volume-5, Issue-6, August 2016 Smart Grid State Estimation by Weighted Least Square Estimation Nithin V G, Libish T

More information

On the Use of PMUs in Power System State Estimation

On the Use of PMUs in Power System State Estimation On the Use of PMUs in Power System State Estimation Antonio Gómez-Expósito Ali Abur Patricia Rousseaux University of Seville Northeastern University University of Liège Seville, Spain Boston, USA Liège,

More information

Feasibility of a Multi-Pass Thomson Scattering System with Confocal Spherical Mirrors

Feasibility of a Multi-Pass Thomson Scattering System with Confocal Spherical Mirrors Plasma and Fusion Research: Letters Volume 5, 044 200) Feasibility o a Multi-Pass Thomson Scattering System with Conocal Spherical Mirrors Junichi HIRATSUKA, Akira EJIRI, Yuichi TAKASE and Takashi YAMAGUCHI

More information

Scattered Data Approximation of Noisy Data via Iterated Moving Least Squares

Scattered Data Approximation of Noisy Data via Iterated Moving Least Squares Scattered Data Approximation o Noisy Data via Iterated Moving Least Squares Gregory E. Fasshauer and Jack G. Zhang Abstract. In this paper we ocus on two methods or multivariate approximation problems

More information

Physics 5153 Classical Mechanics. Solution by Quadrature-1

Physics 5153 Classical Mechanics. Solution by Quadrature-1 October 14, 003 11:47:49 1 Introduction Physics 5153 Classical Mechanics Solution by Quadrature In the previous lectures, we have reduced the number o eective degrees o reedom that are needed to solve

More information

Least-Squares Spectral Analysis Theory Summary

Least-Squares Spectral Analysis Theory Summary Least-Squares Spectral Analysis Theory Summary Reerence: Mtamakaya, J. D. (2012). Assessment o Atmospheric Pressure Loading on the International GNSS REPRO1 Solutions Periodic Signatures. Ph.D. dissertation,

More information

Optimal PMU Placement

Optimal PMU Placement Optimal PMU Placement S. A. Soman Department of Electrical Engineering Indian Institute of Technology Bombay Dec 2, 2011 PMU Numerical relays as PMU System Observability Control Center Architecture WAMS

More information

3. Several Random Variables

3. Several Random Variables . Several Random Variables. Two Random Variables. Conditional Probabilit--Revisited. Statistical Independence.4 Correlation between Random Variables. Densit unction o the Sum o Two Random Variables. Probabilit

More information

2. ETA EVALUATIONS USING WEBER FUNCTIONS. Introduction

2. ETA EVALUATIONS USING WEBER FUNCTIONS. Introduction . ETA EVALUATIONS USING WEBER FUNCTIONS Introduction So ar we have seen some o the methods or providing eta evaluations that appear in the literature and we have seen some o the interesting properties

More information

Roberto s Notes on Differential Calculus Chapter 8: Graphical analysis Section 1. Extreme points

Roberto s Notes on Differential Calculus Chapter 8: Graphical analysis Section 1. Extreme points Roberto s Notes on Dierential Calculus Chapter 8: Graphical analysis Section 1 Extreme points What you need to know already: How to solve basic algebraic and trigonometric equations. All basic techniques

More information

STUDY OF THE UTILIZATION AND BENEFITS OF PHASOR MEASUREMENT UNITS FOR LARGE SCALE POWER SYSTEM STATE ESTIMATION. A Thesis YEO JUN YOON

STUDY OF THE UTILIZATION AND BENEFITS OF PHASOR MEASUREMENT UNITS FOR LARGE SCALE POWER SYSTEM STATE ESTIMATION. A Thesis YEO JUN YOON STUDY OF THE UTILIZATION AND BENEFITS OF PHASOR MEASUREMENT UNITS FOR LARGE SCALE POWER SYSTEM STATE ESTIMATION A Thesis by YEO JUN YOON Submitted to the Office of Graduate Studies of Texas A&M University

More information

Math 2412 Activity 1(Due by EOC Sep. 17)

Math 2412 Activity 1(Due by EOC Sep. 17) Math 4 Activity (Due by EOC Sep. 7) Determine whether each relation is a unction.(indicate why or why not.) Find the domain and range o each relation.. 4,5, 6,7, 8,8. 5,6, 5,7, 6,6, 6,7 Determine whether

More information

CONVECTIVE HEAT TRANSFER CHARACTERISTICS OF NANOFLUIDS. Convective heat transfer analysis of nanofluid flowing inside a

CONVECTIVE HEAT TRANSFER CHARACTERISTICS OF NANOFLUIDS. Convective heat transfer analysis of nanofluid flowing inside a Chapter 4 CONVECTIVE HEAT TRANSFER CHARACTERISTICS OF NANOFLUIDS Convective heat transer analysis o nanoluid lowing inside a straight tube o circular cross-section under laminar and turbulent conditions

More information

The Deutsch-Jozsa Problem: De-quantization and entanglement

The Deutsch-Jozsa Problem: De-quantization and entanglement The Deutsch-Jozsa Problem: De-quantization and entanglement Alastair A. Abbott Department o Computer Science University o Auckland, New Zealand May 31, 009 Abstract The Deustch-Jozsa problem is one o the

More information

CÁTEDRA ENDESA DE LA UNIVERSIDAD DE SEVILLA

CÁTEDRA ENDESA DE LA UNIVERSIDAD DE SEVILLA Detection of System Disturbances Using Sparsely Placed Phasor Measurements Ali Abur Department of Electrical and Computer Engineering Northeastern University, Boston abur@ece.neu.edu CÁTEDRA ENDESA DE

More information

Example: When describing where a function is increasing, decreasing or constant we use the x- axis values.

Example: When describing where a function is increasing, decreasing or constant we use the x- axis values. Business Calculus Lecture Notes (also Calculus With Applications or Business Math II) Chapter 3 Applications o Derivatives 31 Increasing and Decreasing Functions Inormal Deinition: A unction is increasing

More information

Chapter 6 Reliability-based design and code developments

Chapter 6 Reliability-based design and code developments Chapter 6 Reliability-based design and code developments 6. General Reliability technology has become a powerul tool or the design engineer and is widely employed in practice. Structural reliability analysis

More information

Curve Sketching. The process of curve sketching can be performed in the following steps:

Curve Sketching. The process of curve sketching can be performed in the following steps: Curve Sketching So ar you have learned how to ind st and nd derivatives o unctions and use these derivatives to determine where a unction is:. Increasing/decreasing. Relative extrema 3. Concavity 4. Points

More information

AP Calculus Notes: Unit 1 Limits & Continuity. Syllabus Objective: 1.1 The student will calculate limits using the basic limit theorems.

AP Calculus Notes: Unit 1 Limits & Continuity. Syllabus Objective: 1.1 The student will calculate limits using the basic limit theorems. Syllabus Objective:. The student will calculate its using the basic it theorems. LIMITS how the outputs o a unction behave as the inputs approach some value Finding a Limit Notation: The it as approaches

More information

CAPACITOR PLACEMENT IN UNBALANCED POWER SYSTEMS

CAPACITOR PLACEMENT IN UNBALANCED POWER SYSTEMS CAPACITOR PLACEMET I UBALACED POWER SSTEMS P. Varilone and G. Carpinelli A. Abur Dipartimento di Ingegneria Industriale Department of Electrical Engineering Universita degli Studi di Cassino Texas A&M

More information

Supplementary Information Reconstructing propagation networks with temporal similarity

Supplementary Information Reconstructing propagation networks with temporal similarity Supplementary Inormation Reconstructing propagation networks with temporal similarity Hao Liao and An Zeng I. SI NOTES A. Special range. The special range is actually due to two reasons: the similarity

More information

AS conceived during the 1970 s [1], [2], [3], [4] State

AS conceived during the 1970 s [1], [2], [3], [4] State A Framework for Estimation of Power Systems Based on Synchronized Phasor Measurement Data Luigi Vanfretti, Student Member, IEEE, Joe H. Chow, Fellow, IEEE, Sanjoy Sarawgi, Member, IEEE, Dean Ellis and

More information

Categories and Natural Transformations

Categories and Natural Transformations Categories and Natural Transormations Ethan Jerzak 17 August 2007 1 Introduction The motivation or studying Category Theory is to ormalise the underlying similarities between a broad range o mathematical

More information

Mesa College Math SAMPLES

Mesa College Math SAMPLES Mesa College Math 6 - SAMPLES Directions: NO CALCULATOR. Write neatly, show your work and steps. Label your work so it s easy to ollow. Answers without appropriate work will receive NO credit. For inal

More information

Linear Equations in Linear Algebra

Linear Equations in Linear Algebra 1 Linear Equations in Linear Algebra 1.1 SYSTEMS OF LINEAR EQUATIONS LINEAR EQUATION,, 1 n A linear equation in the variables equation that can be written in the form a a a b 1 1 2 2 n n a a is an where

More information

AH 2700A. Attenuator Pair Ratio for C vs Frequency. Option-E 50 Hz-20 khz Ultra-precision Capacitance/Loss Bridge

AH 2700A. Attenuator Pair Ratio for C vs Frequency. Option-E 50 Hz-20 khz Ultra-precision Capacitance/Loss Bridge 0 E ttenuator Pair Ratio or vs requency NEEN-ERLN 700 Option-E 0-0 k Ultra-precision apacitance/loss ridge ttenuator Ratio Pair Uncertainty o in ppm or ll Usable Pairs o Taps 0 0 0. 0. 0. 07/08/0 E E E

More information

Power System State Estimation and Optimal Measurement Placement for Distributed Multi-Utility Operation

Power System State Estimation and Optimal Measurement Placement for Distributed Multi-Utility Operation PSERC Power System State Estimation and Optimal Measurement Placement for Distributed Multi-Utility Operation Final Project Report Power Systems Engineering Research Center A National Science Foundation

More information

Bayesian Technique for Reducing Uncertainty in Fatigue Failure Model

Bayesian Technique for Reducing Uncertainty in Fatigue Failure Model 9IDM- Bayesian Technique or Reducing Uncertainty in Fatigue Failure Model Sriram Pattabhiraman and Nam H. Kim University o Florida, Gainesville, FL, 36 Copyright 8 SAE International ABSTRACT In this paper,

More information

Fin efficiency of the newly developed Compartmented Coil of a Single Coil Twin Fan System

Fin efficiency of the newly developed Compartmented Coil of a Single Coil Twin Fan System Fin eiciency o the newly developed Compartmented Coil o a Single Coil Twin Fan System ABSTRACT In predicting the perormance o any cooling coil, HVAC designers ace multiold challenges in designing the system

More information

3.5 Graphs of Rational Functions

3.5 Graphs of Rational Functions Math 30 www.timetodare.com Eample Graph the reciprocal unction ( ) 3.5 Graphs o Rational Functions Answer the ollowing questions: a) What is the domain o the unction? b) What is the range o the unction?

More information

TESTING TIMED FINITE STATE MACHINES WITH GUARANTEED FAULT COVERAGE

TESTING TIMED FINITE STATE MACHINES WITH GUARANTEED FAULT COVERAGE TESTING TIMED FINITE STATE MACHINES WITH GUARANTEED FAULT COVERAGE Khaled El-Fakih 1, Nina Yevtushenko 2 *, Hacene Fouchal 3 1 American University o Sharjah, PO Box 26666, UAE kelakih@aus.edu 2 Tomsk State

More information

Basic mathematics of economic models. 3. Maximization

Basic mathematics of economic models. 3. Maximization John Riley 1 January 16 Basic mathematics o economic models 3 Maimization 31 Single variable maimization 1 3 Multi variable maimization 6 33 Concave unctions 9 34 Maimization with non-negativity constraints

More information

Fatigue verification of high loaded bolts of a rocket combustion chamber.

Fatigue verification of high loaded bolts of a rocket combustion chamber. Fatigue veriication o high loaded bolts o a rocket combustion chamber. Marcus Lehmann 1 & Dieter Hummel 1 1 Airbus Deence and Space, Munich Zusammenassung Rocket engines withstand intense thermal and structural

More information

arxiv:quant-ph/ v2 12 Jan 2006

arxiv:quant-ph/ v2 12 Jan 2006 Quantum Inormation and Computation, Vol., No. (25) c Rinton Press A low-map model or analyzing pseudothresholds in ault-tolerant quantum computing arxiv:quant-ph/58176v2 12 Jan 26 Krysta M. Svore Columbia

More information

COMPARISON OF THERMAL CHARACTERISTICS BETWEEN THE PLATE-FIN AND PIN-FIN HEAT SINKS IN NATURAL CONVECTION

COMPARISON OF THERMAL CHARACTERISTICS BETWEEN THE PLATE-FIN AND PIN-FIN HEAT SINKS IN NATURAL CONVECTION HEFAT014 10 th International Conerence on Heat Transer, Fluid Mechanics and Thermodynamics 14 6 July 014 Orlando, Florida COMPARISON OF THERMA CHARACTERISTICS BETWEEN THE PATE-FIN AND PIN-FIN HEAT SINKS

More information

Online Appendix: The Continuous-type Model of Competitive Nonlinear Taxation and Constitutional Choice by Massimo Morelli, Huanxing Yang, and Lixin Ye

Online Appendix: The Continuous-type Model of Competitive Nonlinear Taxation and Constitutional Choice by Massimo Morelli, Huanxing Yang, and Lixin Ye Online Appendix: The Continuous-type Model o Competitive Nonlinear Taxation and Constitutional Choice by Massimo Morelli, Huanxing Yang, and Lixin Ye For robustness check, in this section we extend our

More information

Optimal Control of process

Optimal Control of process VYSOKÁ ŠKOLA BÁŇSKÁ TECHNICKÁ UNIVERZITA OSTRAVA FAKULTA METALURGIE A MATERIÁLOVÉHO INŽENÝRSTVÍ Optimal Control o process Study Support Milan Heger Ostrava 8 Title: Optimal Control o process Code: Author:

More information

An Alternative Poincaré Section for Steady-State Responses and Bifurcations of a Duffing-Van der Pol Oscillator

An Alternative Poincaré Section for Steady-State Responses and Bifurcations of a Duffing-Van der Pol Oscillator An Alternative Poincaré Section or Steady-State Responses and Biurcations o a Duing-Van der Pol Oscillator Jang-Der Jeng, Yuan Kang *, Yeon-Pun Chang Department o Mechanical Engineering, National United

More information

On the Girth of (3,L) Quasi-Cyclic LDPC Codes based on Complete Protographs

On the Girth of (3,L) Quasi-Cyclic LDPC Codes based on Complete Protographs On the Girth o (3,L) Quasi-Cyclic LDPC Codes based on Complete Protographs Sudarsan V S Ranganathan, Dariush Divsalar and Richard D Wesel Department o Electrical Engineering, University o Caliornia, Los

More information

Review of Prerequisite Skills for Unit # 2 (Derivatives) U2L2: Sec.2.1 The Derivative Function

Review of Prerequisite Skills for Unit # 2 (Derivatives) U2L2: Sec.2.1 The Derivative Function UL1: Review o Prerequisite Skills or Unit # (Derivatives) Working with the properties o exponents Simpliying radical expressions Finding the slopes o parallel and perpendicular lines Simpliying rational

More information

Received: 30 July 2017; Accepted: 29 September 2017; Published: 8 October 2017

Received: 30 July 2017; Accepted: 29 September 2017; Published: 8 October 2017 mathematics Article Least-Squares Solution o Linear Dierential Equations Daniele Mortari ID Aerospace Engineering, Texas A&M University, College Station, TX 77843, USA; mortari@tamu.edu; Tel.: +1-979-845-734

More information

New Functions from Old Functions

New Functions from Old Functions .3 New Functions rom Old Functions In this section we start with the basic unctions we discussed in Section. and obtain new unctions b shiting, stretching, and relecting their graphs. We also show how

More information

The concept of limit

The concept of limit Roberto s Notes on Dierential Calculus Chapter 1: Limits and continuity Section 1 The concept o limit What you need to know already: All basic concepts about unctions. What you can learn here: What limits

More information

Reliability Block Diagram Extensions for Non-Parametric Probabilistic Analysis

Reliability Block Diagram Extensions for Non-Parametric Probabilistic Analysis Reliability Block Diagram Extensions or Non-Parametric Probabilistic Analysis Philip C Davis, Mitchell A Thornton, Theodore W Manikas Darwin Deason Institute or Cyber Security Southern Methodist University

More information

Relating axial motion of optical elements to focal shift

Relating axial motion of optical elements to focal shift Relating aial motion o optical elements to ocal shit Katie Schwertz and J. H. Burge College o Optical Sciences, University o Arizona, Tucson AZ 857, USA katie.schwertz@gmail.com ABSTRACT In this paper,

More information

MEASUREMENT UNCERTAINTIES

MEASUREMENT UNCERTAINTIES MEASUREMENT UNCERTAINTIES What distinguishes science rom philosophy is that it is grounded in experimental observations. These observations are most striking when they take the orm o a quantitative measurement.

More information

Acoustic forcing of flexural waves and acoustic fields for a thin plate in a fluid

Acoustic forcing of flexural waves and acoustic fields for a thin plate in a fluid Acoustic orcing o leural waves and acoustic ields or a thin plate in a luid Darryl MCMAHON Maritime Division, Deence Science and Technology Organisation, HMAS Stirling, WA Australia ABSTACT Consistency

More information

Section 3.4: Concavity and the second Derivative Test. Find any points of inflection of the graph of a function.

Section 3.4: Concavity and the second Derivative Test. Find any points of inflection of the graph of a function. Unit 3: Applications o Dierentiation Section 3.4: Concavity and the second Derivative Test Determine intervals on which a unction is concave upward or concave downward. Find any points o inlection o the

More information

Introduction to Compact Dynamical Modeling. II.1 Steady State Simulation. Luca Daniel Massachusetts Institute of Technology. dx dt.

Introduction to Compact Dynamical Modeling. II.1 Steady State Simulation. Luca Daniel Massachusetts Institute of Technology. dx dt. Course Outline NS & NIH Introduction to Compact Dynamical Modeling II. Steady State Simulation uca Daniel Massachusetts Institute o Technology Quic Snea Preview I. ssembling Models rom Physical Problems

More information

CinChE Problem-Solving Strategy Chapter 4 Development of a Mathematical Algorithm. partitioning. procedure

CinChE Problem-Solving Strategy Chapter 4 Development of a Mathematical Algorithm. partitioning. procedure Development o a Mathematical Algorithm Transormation Process Mathematical Model partitioning procedure Mathematical Algorithm The mathematical algorithm is a plan (or blueprint) that identiies the independent

More information

Automatica. Distributed fault detection for interconnected second-order systems

Automatica. Distributed fault detection for interconnected second-order systems Automatica 47 (20) 2757 2764 Contents lists available at SciVerse ScienceDirect Automatica journal homepage: www.elsevier.com/locate/automatica Brie paper Distributed ault detection or interconnected second-order

More information

it simpliies the notation, we write unary unction symbols without parenthesis, e.g., h((h(x);a)) would be written as h(hx; a). By s[t] we indicate tha

it simpliies the notation, we write unary unction symbols without parenthesis, e.g., h((h(x);a)) would be written as h(hx; a). By s[t] we indicate tha Fast Algorithms or Uniorm Semi-Uniication Alberto Oliart Λ Laboratorio Nacional de Inormática Avanzada, A.C. Rébsamen 8, Xalapa, Veracruz, Mexico aoliart@lania.mx Wayne Snyder Boston University Computer

More information

Simulation of Plane Motion of Semiautonomous Underwater Vehicle

Simulation of Plane Motion of Semiautonomous Underwater Vehicle Proceedings o the European Computing Conerence Simulation o Plane Motion o Semiautonomous Underwater Vehicle JERZY GARUS, JÓZEF MAŁECKI Faculty o Mechanical and Electrical Engineering Naval University

More information

Figure 1: Bayesian network for problem 1. P (A = t) = 0.3 (1) P (C = t) = 0.6 (2) Table 1: CPTs for problem 1. (c) P (E B) C P (D = t) f 0.9 t 0.

Figure 1: Bayesian network for problem 1. P (A = t) = 0.3 (1) P (C = t) = 0.6 (2) Table 1: CPTs for problem 1. (c) P (E B) C P (D = t) f 0.9 t 0. Probabilistic Artiicial Intelligence Problem Set 3 Oct 27, 2017 1. Variable elimination In this exercise you will use variable elimination to perorm inerence on a bayesian network. Consider the network

More information

Performance Assessment of Generalized Differential Evolution 3 (GDE3) with a Given Set of Problems

Performance Assessment of Generalized Differential Evolution 3 (GDE3) with a Given Set of Problems Perormance Assessment o Generalized Dierential Evolution (GDE) with a Given Set o Problems Saku Kukkonen, Student Member, IEEE and Jouni Lampinen Abstract This paper presents results or the CEC 007 Special

More information

Probability, Statistics, and Reliability for Engineers and Scientists MULTIPLE RANDOM VARIABLES

Probability, Statistics, and Reliability for Engineers and Scientists MULTIPLE RANDOM VARIABLES CHATER robability, Statistics, and Reliability or Engineers and Scientists MULTILE RANDOM VARIABLES Second Edition A. J. Clark School o Engineering Department o Civil and Environmental Engineering 6a robability

More information

Maximum Flow. Reading: CLRS Chapter 26. CSE 6331 Algorithms Steve Lai

Maximum Flow. Reading: CLRS Chapter 26. CSE 6331 Algorithms Steve Lai Maximum Flow Reading: CLRS Chapter 26. CSE 6331 Algorithms Steve Lai Flow Network A low network G ( V, E) is a directed graph with a source node sv, a sink node tv, a capacity unction c. Each edge ( u,

More information

Syllabus Objective: 2.9 The student will sketch the graph of a polynomial, radical, or rational function.

Syllabus Objective: 2.9 The student will sketch the graph of a polynomial, radical, or rational function. Precalculus Notes: Unit Polynomial Functions Syllabus Objective:.9 The student will sketch the graph o a polynomial, radical, or rational unction. Polynomial Function: a unction that can be written in

More information

Scattering of Solitons of Modified KdV Equation with Self-consistent Sources

Scattering of Solitons of Modified KdV Equation with Self-consistent Sources Commun. Theor. Phys. Beijing, China 49 8 pp. 89 84 c Chinese Physical Society Vol. 49, No. 4, April 5, 8 Scattering o Solitons o Modiied KdV Equation with Sel-consistent Sources ZHANG Da-Jun and WU Hua

More information

References Ideal Nyquist Channel and Raised Cosine Spectrum Chapter 4.5, 4.11, S. Haykin, Communication Systems, Wiley.

References Ideal Nyquist Channel and Raised Cosine Spectrum Chapter 4.5, 4.11, S. Haykin, Communication Systems, Wiley. Baseand Data Transmission III Reerences Ideal yquist Channel and Raised Cosine Spectrum Chapter 4.5, 4., S. Haykin, Communication Systems, iley. Equalization Chapter 9., F. G. Stremler, Communication Systems,

More information

A Method for Assimilating Lagrangian Data into a Shallow-Water-Equation Ocean Model

A Method for Assimilating Lagrangian Data into a Shallow-Water-Equation Ocean Model APRIL 2006 S A L M A N E T A L. 1081 A Method or Assimilating Lagrangian Data into a Shallow-Water-Equation Ocean Model H. SALMAN, L.KUZNETSOV, AND C. K. R. T. JONES Department o Mathematics, University

More information

The 2nd Texas A&M at Galveston Mathematics Olympiad. September 24, Problems & Solutions

The 2nd Texas A&M at Galveston Mathematics Olympiad. September 24, Problems & Solutions nd Math Olympiad Solutions Problem #: The nd Teas A&M at Galveston Mathematics Olympiad September 4, 00 Problems & Solutions Written by Dr. Lin Qiu A runner passes 5 poles in 30 seconds. How long will

More information

Relating axial motion of optical elements to focal shift

Relating axial motion of optical elements to focal shift Relating aial motion o optical elements to ocal shit Katie Schwertz and J. H. Burge College o Optical Sciences, University o Arizona, Tucson AZ 857, USA katie.schwertz@gmail.com ABSTRACT In this paper,

More information

Analysis of Foundation Damping from Theoretical Models and Forced Vibration Testing

Analysis of Foundation Damping from Theoretical Models and Forced Vibration Testing 6 th International Conerence on Earthquae Geotechnical Engineering 1-4 November 2015 Christchurch, New Zealand Analysis o Foundation Damping rom Theoretical Models and Forced Vibration Testing M. J. Givens

More information

Do new competitors, new customers, new suppliers,... sustain, destroy or create competitive advantage?

Do new competitors, new customers, new suppliers,... sustain, destroy or create competitive advantage? Do new competitors, new customers, new suppliers,... sustain, destroy or create competitive advantage? Glenn MacDonald Olin School o Business Washington University MichaelD.Ryall Melbourne Business School

More information

Today. Introduction to optimization Definition and motivation 1-dimensional methods. Multi-dimensional methods. General strategies, value-only methods

Today. Introduction to optimization Definition and motivation 1-dimensional methods. Multi-dimensional methods. General strategies, value-only methods Optimization Last time Root inding: deinition, motivation Algorithms: Bisection, alse position, secant, Newton-Raphson Convergence & tradeos Eample applications o Newton s method Root inding in > 1 dimension

More information

RELIABILITY OF BURIED PIPELINES WITH CORROSION DEFECTS UNDER VARYING BOUNDARY CONDITIONS

RELIABILITY OF BURIED PIPELINES WITH CORROSION DEFECTS UNDER VARYING BOUNDARY CONDITIONS REIABIITY OF BURIE PIPEIES WITH CORROSIO EFECTS UER VARYIG BOUARY COITIOS Ouk-Sub ee 1 and ong-hyeok Kim 1. School o Mechanical Engineering, InHa University #53, Yonghyun-ong, am-ku, Incheon, 40-751, Korea

More information

The Ascent Trajectory Optimization of Two-Stage-To-Orbit Aerospace Plane Based on Pseudospectral Method

The Ascent Trajectory Optimization of Two-Stage-To-Orbit Aerospace Plane Based on Pseudospectral Method Available online at www.sciencedirect.com ScienceDirect Procedia Engineering 00 (014) 000 000 www.elsevier.com/locate/procedia APISAT014, 014 Asia-Paciic International Symposium on Aerospace Technology,

More information

Approximate probabilistic optimization using exact-capacity-approximate-response-distribution (ECARD)

Approximate probabilistic optimization using exact-capacity-approximate-response-distribution (ECARD) Struct Multidisc Optim (009 38:613 66 DOI 10.1007/s00158-008-0310-z RESEARCH PAPER Approximate probabilistic optimization using exact-capacity-approximate-response-distribution (ECARD Sunil Kumar Richard

More information

FOF (Functionally Observable Fault): A unified mode for testing and debugging - ATPG and application to debugging -

FOF (Functionally Observable Fault): A unified mode for testing and debugging - ATPG and application to debugging - FOF Functionally Observable Fault: uniied mode or testing and debugging - TPG and application to debugging - Masahiro Fujita VLSI Design and Education enter VDE University o Tokyo Stuck-at ault and unctional

More information

z-axis SUBMITTED BY: Ms. Harjeet Kaur Associate Professor Department of Mathematics PGGCG 11, Chandigarh y-axis x-axis

z-axis SUBMITTED BY: Ms. Harjeet Kaur Associate Professor Department of Mathematics PGGCG 11, Chandigarh y-axis x-axis z-ais - - SUBMITTED BY: - -ais - - - - - - -ais Ms. Harjeet Kaur Associate Proessor Department o Mathematics PGGCG Chandigarh CONTENTS: Function o two variables: Deinition Domain Geometrical illustration

More information

Reliability Assessment with Correlated Variables using Support Vector Machines

Reliability Assessment with Correlated Variables using Support Vector Machines Reliability Assessment with Correlated Variables using Support Vector Machines Peng Jiang, Anirban Basudhar, and Samy Missoum Aerospace and Mechanical Engineering Department, University o Arizona, Tucson,

More information

Part I: Thin Converging Lens

Part I: Thin Converging Lens Laboratory 1 PHY431 Fall 011 Part I: Thin Converging Lens This eperiment is a classic eercise in geometric optics. The goal is to measure the radius o curvature and ocal length o a single converging lens

More information

Dynamic Modeling and Control of Shunt Active Power Filter

Dynamic Modeling and Control of Shunt Active Power Filter Dynamic Modeling and Control o Shunt Active Power Filter Utkal Ranjan Muduli Electrical Engineering Indian Institute o Technology Gandhinagar Gujarat, India-82424 Email: utkalranjan muduli@iitgn.ac.in

More information