The Measurement and Evaluation of Distribution Transformer Losses Under Non-Linear Loading

Size: px
Start display at page:

Download "The Measurement and Evaluation of Distribution Transformer Losses Under Non-Linear Loading"

Transcription

1 IEEE ower Engineering Society General Meeting, Denver CO, June 9, 4 / ESGM 4-7 e Measureent and Evaluation of Distribution ransforer Losses Under Non-Linear Loading Aleksandar Danjanovic,.D., Meber IEEE and Gregory Ferguson, BSc., Life Meber IEEE Abstract Haronic currents, generated by non-linear electronic loads, produce penalty losses in every eleent of an electrical distribution syste. [] ese aronic-related losses reduce syste efficiency, cause apparatus overeating, and increase power and air conditioning costs. [] Haronic currents effectively de-rate existing systes and, wen accoodated, add substantially to te capital cost of new distribution systes. e easureent and evaluation of transforer losses under linear and non-linear load conditions will be discussed. In addition, typical financial benefits tat result fro te application of ig efficiency aronic itigating distribution transforers, under non-linear loading, will be calculated. Index ers efficiency, aronics, non-linear load, penalty losses, transforer losses I. INRODUCION Existing Standards e igest standards for transforer efficiency in Nort Aerican are found in NEMA Standard ublication -, [3] CSA ublication C8.- and EA s Energy Star requireents. e easureent and calculation etods required by tese standards accurately deterine a transforer s losses and energy efficiency, wen it supplies linear resistive and/or inductive loads. e Non-Linear Load Reality Modern electrical distribution systes typically supply a ig percentage of nonlinear electronic loads, particularly in /8-volt systes. As a result, transforer losses increase and energy efficiency decrease. e level of deterioration is a function of aronic voltage agnitudes at a transforer s priary terinals, loadgenerated aronic current agnitudes at its secondary terinals and teir pase relationsips. ere are, unfortunately, no recognized standards for deterining transforer losses or efficiency under tese nonlinear conditions. Misleading Clais A nuber of ig efficiency distribution transforer anufacturers now clai efficiencies tat eet or exceed te requireents of NEMA - and CSA C8.- under severe but unspecified nonlinear loading. Several anufacturers ave even publised teir efficiency test etods. At best, tese clais are isleading since: (i ere is no recognized standard guide for deterining te energy efficiency of a distribution transforer or a standard test etod for easuring its energy consuption under nonlinear load conditions and (ii e anufacturers publised ower-in ower-out Measureent Metod, wic boasts ±.3% revenue class instruentation accuracy and ±.% watteter accuracy, will, in reality, produce an error of ±.5%,wen easuring te efficiency of a transforer under linear or nonlinear loading. As a result, teir claied efficiency of 98%, for a 75kVA transforer, ay, in fact, be only 96.5%. II. RANSFORMER LOSSES Haronic voltages and currents increase transforer losses. More specifically, aronic voltages increase losses in its agnetic core wile aronic currents increase losses in its windings and structure. e effect of aronic voltages is relatively sall since losses in te agnetic core are norally only % of te winding losses. A transforer s penalty losses are ainly due to aronic currents. Unfortunately, aronics currents are typically uc iger in /8-volt subsystes. ransforers operating at tese voltage levels require special consideration. IEEE SD and IEEE SD categorize transforer losses as No-Load Losses ( NL or Excitation Losses and Load Losses ( LL or Ipedance Losses. e su of tese losses is referred to as otal Losses ( LOSS : LOSS ( NL LL Excitation Losses [4] are priarily losses in te agnetic core and are due to agnetic ysteresis and eddy currents. Load Losses are divided into I R Losses and Stray Losses. I R Losses can be obtained, as follows: ax I R I R ( Eddy-currents, wic produce stray electroagnetic flux in te transforer s windings, agnetic core, core claps, enclosure and oter structural parts, cause Stray Losses. Wit ig aronic currents, te Eddy-Current Losses in te windings are te ost doinant losses in te transforer. otal Stray Losses ( S are proportional to te product of Fundaental Stray Losses ( S and te square of te product of te aronic currents and teir corresponding frequencies, as follows: S ax S I III. MEASURING OF RANSFORMER LOSSES (3 e easureent of a transforer s losses and calculation of its efficiency is very well understood and applied in te power and distribution transforer industry. However,

2 conventional No-Load Loss and Load Loss easureent etods only confir a transforer s perforance under linear load conditions. IEEE Std Standard est Code for Dry-ype Distribution and ower ransforers and NEMA -998 A Standard est Metod for Measuring te Energy Consuption of Distribution ransforers [5] specify te testing procedure for te easureent of losses and te calculation of efficiency under linear loading. e easureent of No-Load Losses is ade during an Open-Circuit est and te easureent of Load Losses is ade during a Sort-Circuit est. ese easureents can be used to calculate efficiency as follows: OU (4 OU LOSS Were: ransforer Efficiency Output ower (Watts OU ransforer ower Losses (Watts LOSS Conventional Metod of Measureents ransforer Losses and Efficiency - A transforer s otal Losses are obtained by calculating te difference between input and output power. A single-pase transforer can be considered as a twoport network (Figure, in wic te transforer losses are obtained as te difference between two products: p loss p p p (5 v in out p vi vi i i RANSFORMER Kt=N/N A ransforer as a wo-ort Network Figure e instruentation and connection diagra, for testing a single-pase transforer, is sown in Figure. v i V v INU OWER C A ESING RNASFORME RANSFORMER R C v i A v V OUU OWER Connection Diagra for a Single-ase ransforer Figure Depending on its kva rating, te efficiency of a distribution transforer is usually in te 9% to 98% range. o coply wit NEMA, CSA C8.- and te EA Energy Star. rogra, efficiencies ust be in te 97% to 98.9%. However, v NEMA, and all oter current standards, specifically excludes transforers tat supply nonlinear loads. We can derive te axiu full scale errors for te voltages and currents, and te axiu errors for losses and efficiency, for 75 kva 48/:8 tree-pase transforer, as follows: No-Load Losses = 86 Watts, Load Losses at % load =,74 Watts, Efficiency = wen te instruent transforers are.3% accuracy class, te volteter and aeters ave an accuracy of.%fs, and te watteters ave an accuracy of.%fs, as sown in Figure. e instruentation is suarized in able. Instruents Full Scale Full Scale Error V 48/.36 V - - C /5.5 C 4/5.5 V 3.3 V 3.3 A 5.5 A 5.5 able Losses and efficiency easureent errors, at unity power factor and % load can be calculated as follows: loss ( vt V(5 C A x ( V (5 Ct A x kW 74.6kW.3kW e losses easureent error is: Loss Loss.3 x 5.6% e efficiency easureent error is: eff.34% New Metod of Measureents ransforer Losses and Efficiency [6] Considering te transforer as a two-port network (Figure, instantaneous power absorbed by te transforer is defined by equation (5. By creating a new twoport network, wic is sown in Figure 3, we introduce a * current generator ( i i i / K, wic is parallel to port * p-p, and voltage generator ( v v / K v, wic is in series wit port p-p. Bot Input and Output ower coincide wit v i / K. e overall absorbed power troug ports p-p and p-p is zero. e instantaneous power absorbed will be equal to te su of te power delivered by tese generators. e power losses of te transforer can be expressed by: " p L ( i i / K v ( v / K v i p p (6

3 p v p i /K i * = i -i / K RANSFORMER Kt = N/N " Second ter is: ( v vk t idt i v * = v /K-v p i v Adt " iv AC v i v /K A ransforer as a wo-ort Network Figure 3 Average power for soe period of tie can be expressed by: " L ( i i / K vdt ( v / Kv idt (7 Equation (6 is valid for any constant K. Based on tis forulation, a new easuring etod is presented, wit te connection diagra sown in Figure 4. is etod also requires two watteters, or two sets of volteters and aeters. One set for a full range of voltages and sall currents and te oter set for sall voltages and full range of currents. ysical interpretation of tis etod can be explained using Figure 4. INU v V C v i i i i -i A A RANSFORMER ESING RNASFORMER v A V C p OUU v -v Connection Diagra for a Single-ase ransforer Figure 4 Based on te diagra as sown in Figure 4. ( i i / Kt vdt i v Adt iv AB e ter corresponds to te losses due to te circulation of agnetizing current in te priary added to agnetic core losses. at is equivalent to te transforer open circuit test. i dt dt v (8 (9 Equation (9 represents te su of te losses in te priary and secondary of te transforer, due to load current, wic is equivalent to a transforer sort-circuit test. Wit tis etod, it is possible to separately easure te core and copper losses of te transforer. Measureent under nonlinear load conditions is also possible. o evaluate te new easuring etod, using te proposed connection diagra in Figure 4, we analyze te sae exaple evaluated wit te conventional easuring approac, wit standard Metering Class Cs and Vs, and specially design differential Cs and Vs. e instruentation is suarized in able. Instruents Full Scale Full Scale Error V 48/.36 V /.36 C 5/5.5 C 5/5.5 V. V. A. A. Exciting current error is: able ( i i C A.6 ( i i ( i i / Input Voltage is easured wit te error: v V V.7 v v e core losses are easured wit te error: Fe v ( i i.33 Fe v ( i i e series voltage drop is easured wit te error: ( v v V V.68 ( v v ( v v Output current is easured wit error: i C A.79 i i / e copper losses are easured wit te error: Cu i ( v v.4 Cu i ( v v e core losses are easured wit te error: Fe v ( i i.33 Fe v ( i i e total losses are easured wit te error: Loss cu Fe.3.3% Loss Loss e efficiency easureent error is: eff.33% 3

4 IV. EVALUAION OF LOSSES AND MEASUREMEN Based on te presented two easureent etods, we will plot te losses and efficiency for bot etods. Figures 5a and 5b present Losses (kw vs. Load (pu wile Figures 6a and 6b present Efficiency (pu vs. Load (pu V & C Difference lus & Minus Error ower-in ower-out Minus Error ower-in ower-out lus Error V & C Difference lus & Minus Error lus Losses Measureent Error Figure 5a V & C Difference lus & Minus Error ower-in ower-out lus Error Minus Losses Measureent Error Figure 5b ower-in ower-out lus Error V & C Difference lus & Minus Error lus Efficiency Measureent Error Figure 6a Minus Efficiency Measureent Error Figure 6b IV. CONCLUSION A conventional approac to te easureent of losses in distribution transforers is based on te difference of two nuerically large ters tat are quite close in value. e easureent error in tis approac is significant and cannot be used to calculate efficiency of a igly efficient transforer. e error in deterining te losses and calculating te transforer s efficiency can be greatly reduced by using a new etod tat is based on te addition of two ters, wic are in te sae region of value. Fro tis presentation, it is obvious tat te easureent of transforer losses and calculation of transforer efficiency, wic is based on te ower-in ower-out Measureent Metod, is very inaccurate. Using current and voltage transforers wit Metering Class accuracy (.3% can lead to a easureent error in te.3% range. Wit te ore accurate current and voltage transforers (.%, te accuracy of easureent is iproved to.94%, wic is still not satisfactory for te easureent of transforer losses. Clais of ig transforer efficiencies under nonlinear loading, wen tested by tis conventional etod, tat is, by easuring te input and output power, will not be valid or tecnical eaningful, since it produces an error of.3% or.94% best case. By coparison, te etod based on Voltage and Current Difference as an error of less ten.35%. e ower-in ower-out Metod, for deterining a transforer s energy losses in a nonlinear load environent, is isleading and witout tecnical erit. e etod based on Voltage and Current Difference will accurately deterine a transforer s efficiency in any nonlinear load environent. V. REFERENCE []. Key & J-S. Lai, Costs and Benefits of Haronic Current Reduction for Switc-Mode ower Supplies in Coercial Office Buildings. IEEE Annual Meeting, October 995, Orlando, Florida. [] G.N.C. Ferguson, e Costs and Benefits of Haronic Current Reduction in Low Voltage Distribution Systes. International ower Quality Conference (IQC, October, Singapore. 4

5 [3] NEMA Standard ublication -, Guide for Deterining Energy Efficiency for Distribution ransforers. [4] IEEE Standard C , est Code for Dry- ype Distribution ower ransforers. [5] NEMA Standard ublication -998, Standard est Metod for Measuring te Energy Consuption of Distribution ransforers [6] D. Lin, E.F. Fucs, M. Doyle Coputer-Aided esting of Electrical Apparatus Supplying Non-Linear Loads, IEEE ransactions on ower Systes, Vol., No., February 997. VI. BIOGRAHIES Aleksandar Danjanovic was born in Yugoslavia in 96. He received a B.S. Degree in Electrical Engineering fro te University of St. Kiril and Metodij, Skopje, Yugoslavia, and a Master Degree and D in Electrical Engineering fro swine University of ecnology, retoria, Sout Africa. His experience includes eployent wit ABB &D, Sout Africa, Instruent ransforers, Inc., USA, and asetronics, Inc., USA. Mr. Danjanovic joined ower Quality International, Inc., USA, in, as its Vice-resident, Engineering. His researc interests include electroagnetics, power syste odeling, analysis and design. Gregory Ferguson was born in oronto, Canada in 937. He received a B.Sc. Degree in Engineering ecnology fro Ryerson olytecnic University, oronto. His experience includes eployent wit te Ontario Hydro-Electric ower Coission and Scarboroug ublic Utilities, Canada. He is te founder of Ferguson Engineering Services, Inc., Canada, Electrical esting Instruents, Ltd., Canada, ower Quality International, Inc., USA and FES International, Inc., Canada & USA. Mr. Ferguson is a Life Meber in IEEE. His interests include electrical power syste analysis, design, optiization and forensics. 5

Derivative at a point

Derivative at a point Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Derivative at a point Wat you need to know already: Te concept of liit and basic etods for coputing liits. Wat you can

More information

lecture 35: Linear Multistep Mehods: Truncation Error

lecture 35: Linear Multistep Mehods: Truncation Error 88 lecture 5: Linear Multistep Meods: Truncation Error 5.5 Linear ultistep etods One-step etods construct an approxiate solution x k+ x(t k+ ) using only one previous approxiation, x k. Tis approac enoys

More information

PH 222-2C Fall Electromagnetic Oscillations and Alternating Current. Lectures 18-19

PH 222-2C Fall Electromagnetic Oscillations and Alternating Current. Lectures 18-19 H - Fall 0 Electroagnetic Oscillations and Alternating urrent ectures 8-9 hapter 3 (Halliday/esnick/Walker, Fundaentals of hysics 8 th edition) hapter 3 Electroagnetic Oscillations and Alternating urrent

More information

Chapter 10 Objectives

Chapter 10 Objectives Chapter 10 Engr8 Circuit Analysis Dr Curtis Nelson Chapter 10 Objectives Understand the following AC power concepts: Instantaneous power; Average power; Root Mean Squared (RMS) value; Reactive power; Coplex

More information

5.1 The derivative or the gradient of a curve. Definition and finding the gradient from first principles

5.1 The derivative or the gradient of a curve. Definition and finding the gradient from first principles Capter 5: Dierentiation In tis capter, we will study: 51 e derivative or te gradient o a curve Deinition and inding te gradient ro irst principles 5 Forulas or derivatives 5 e equation o te tangent line

More information

MEASURING INSTRUMENTS

MEASURING INSTRUMENTS CLASS NOTES ON ELECTRICAL MEASUREMENTS & INSTRUMENTATION 05 MEASURING INSTRUMENTS. Definition of instruents An instruent is a device in which we can deterine the agnitude or value of the quantity to be

More information

BEF BEF Chapter 2. Outline BASIC PRINCIPLES 09/10/2013. Introduction. Phasor Representation. Complex Power Triangle.

BEF BEF Chapter 2. Outline BASIC PRINCIPLES 09/10/2013. Introduction. Phasor Representation. Complex Power Triangle. BEF 5503 BEF 5503 Chapter BASC PRNCPLES Outline 1 3 4 5 6 7 8 9 ntroduction Phasor Representation Coplex Power Triangle Power Factor Coplex Power in AC Single Phase Circuits Coplex Power in Balanced Three-Phase

More information

Chapter 28: Alternating Current

Chapter 28: Alternating Current hapter 8: Alternating urrent Phasors and Alternating urrents Alternating current (A current) urrent which varies sinusoidally in tie is called alternating current (A) as opposed to direct current (D).

More information

Design of 25 KA Current Injection Transformer Core with Finite Element Method

Design of 25 KA Current Injection Transformer Core with Finite Element Method 1 Design of 5 KA Current Injection Transforer Core ith Finite Eleent Method HOSSEIN HEYDARI, MOHSEN ARIANNEJAD, FARAMARZ FAGHIHI Iran University of Science and Technology, Tehran, Iran Abstract.Since Current

More information

Successful Brushless A.C. Power Extraction From The Faraday Acyclic Generator

Successful Brushless A.C. Power Extraction From The Faraday Acyclic Generator Successful Brushless A.C. Power Extraction Fro The Faraday Acyclic Generator July 11, 21 Volt =.2551552 volt 1) If we now consider that the voltage is capable of producing current if the ri of the disk

More information

Section 12. Afocal Systems

Section 12. Afocal Systems OPTI-0/0 Geoetrical and Instruental Optics Copyrigt 08 Jon E. Greivenkap - Section Aocal Systes Gaussian Optics Teores In te initial discussion o Gaussian optics, one o te teores deined te two dierent

More information

1 Proving the Fundamental Theorem of Statistical Learning

1 Proving the Fundamental Theorem of Statistical Learning THEORETICAL MACHINE LEARNING COS 5 LECTURE #7 APRIL 5, 6 LECTURER: ELAD HAZAN NAME: FERMI MA ANDDANIEL SUO oving te Fundaental Teore of Statistical Learning In tis section, we prove te following: Teore.

More information

Chapter 10 ACSS Power

Chapter 10 ACSS Power Objectives: Power concepts: instantaneous power, average power, reactive power, coplex power, power factor Relationships aong power concepts the power triangle Balancing power in AC circuits Condition

More information

Mutual capacitor and its applications

Mutual capacitor and its applications Mutual capacitor and its applications Chun Li, Jason Li, Jieing Li CALSON Technologies, Toronto, Canada E-ail: calandli@yahoo.ca Published in The Journal of Engineering; Received on 27th October 2013;

More information

Tutorial 2 (Solution) 1. An electron is confined to a one-dimensional, infinitely deep potential energy well of width L = 100 pm.

Tutorial 2 (Solution) 1. An electron is confined to a one-dimensional, infinitely deep potential energy well of width L = 100 pm. Seester 007/008 SMS0 Modern Pysics Tutorial Tutorial (). An electron is confined to a one-diensional, infinitely deep potential energy well of widt L 00 p. a) Wat is te least energy te electron can ave?

More information

Neural Networks Trained with the EEM Algorithm: Tuning the Smoothing Parameter

Neural Networks Trained with the EEM Algorithm: Tuning the Smoothing Parameter eural etworks Trained wit te EEM Algorit: Tuning te Sooting Paraeter JORGE M. SATOS,2, JOAQUIM MARQUES DE SÁ AD LUÍS A. ALEXADRE 3 Intituto de Engenaria Bioédica, Porto, Portugal 2 Instituto Superior de

More information

AN IMPROVED WEIGHTED TOTAL HARMONIC DISTORTION INDEX FOR INDUCTION MOTOR DRIVES

AN IMPROVED WEIGHTED TOTAL HARMONIC DISTORTION INDEX FOR INDUCTION MOTOR DRIVES AN IMPROVED WEIGHTED TOTA HARMONIC DISTORTION INDEX FOR INDUCTION MOTOR DRIVES Tomas A. IPO University of Wisconsin, 45 Engineering Drive, Madison WI, USA P: -(608)-6-087, Fax: -(608)-6-5559, lipo@engr.wisc.edu

More information

c hc h c h. Chapter Since E n L 2 in Eq. 39-4, we see that if L is doubled, then E 1 becomes (2.6 ev)(2) 2 = 0.65 ev.

c hc h c h. Chapter Since E n L 2 in Eq. 39-4, we see that if L is doubled, then E 1 becomes (2.6 ev)(2) 2 = 0.65 ev. Capter 39 Since n L in q 39-4, we see tat if L is doubled, ten becoes (6 ev)() = 065 ev We first note tat since = 666 0 34 J s and c = 998 0 8 /s, 34 8 c6 66 0 J sc 998 0 / s c 40eV n 9 9 60 0 J / ev 0

More information

ELG3311: Assignment 3

ELG3311: Assignment 3 LG33: ssignent 3 roble 6-: The Y-connected synchronous otor whose naeplate is shown in Figure 6- has a perunit synchronous reactance of 0.9 and a per-unit resistance of 0.0. (a What is the rated input

More information

Introduction to Derivatives

Introduction to Derivatives Introduction to Derivatives 5-Minute Review: Instantaneous Rates and Tangent Slope Recall te analogy tat we developed earlier First we saw tat te secant slope of te line troug te two points (a, f (a))

More information

Numerical Solution for Non-Stationary Heat Equation in Cooling of Computer Radiator System

Numerical Solution for Non-Stationary Heat Equation in Cooling of Computer Radiator System (JZS) Journal of Zankoy Sulaiani, 9, 1(1) Part A (97-1) A119 Nuerical Solution for Non-Stationary Heat Equation in Cooling of Coputer Radiator Syste Aree A. Maad*, Faraidun K. Haa Sal**, and Najadin W.

More information

Non-Linear Thermal Model for Transformers Study

Non-Linear Thermal Model for Transformers Study Aida Bulucea, George Manolea, iliana Perescu-Popescu Non-inear Teral Model for Transforers Study MARIUS CONSTANTIN POPESCU NIKOS E. MASTORAKIS CORNEIA AIDA BUUCEA GHEORGHE MANOEA IIANA PERESCU-POPESCU

More information

Problem Set 7: Potential Energy and Conservation of Energy AP Physics C Supplementary Problems

Problem Set 7: Potential Energy and Conservation of Energy AP Physics C Supplementary Problems Proble Set 7: Potential Energy and Conservation of Energy AP Pysics C Suppleentary Probles 1. Approxiately 5.5 x 10 6 kg of water drops 50 over Niagara Falls every second. (a) Calculate te aount of potential

More information

Power Quality Analysis Including Dips and Swells

Power Quality Analysis Including Dips and Swells International Journal of Electrical Engineering. ISSN 0974-158 Volue 4, Nuber 6 (011), pp. 697-709 International Research Publication House http://www.irphouse.co Power Quality Analysis Including Dips

More information

Now multiply the left-hand-side by ω and the right-hand side by dδ/dt (recall ω= dδ/dt) to get:

Now multiply the left-hand-side by ω and the right-hand side by dδ/dt (recall ω= dδ/dt) to get: Equal Area Criterion.0 Developent of equal area criterion As in previous notes, all powers are in per-unit. I want to show you the equal area criterion a little differently than the book does it. Let s

More information

1 Analysis of heat transfer in a single-phase transformer

1 Analysis of heat transfer in a single-phase transformer Assignent -7 Analysis of heat transr in a single-phase transforer The goal of the first assignent is to study the ipleentation of equivalent circuit ethod (ECM) and finite eleent ethod (FEM) for an electroagnetic

More information

Determination of Active and Reactive Power in Multi-Phase Systems through Analytical Signals Associated Current and Voltage Signals

Determination of Active and Reactive Power in Multi-Phase Systems through Analytical Signals Associated Current and Voltage Signals 56 ACA ELECROEHNICA Deterination of Active and Reactive Power in ulti-phase Systes through Analytical Signals Associated Current and Voltage Signals Gheorghe ODORAN, Oana UNEAN and Anca BUZURA Suary -

More information

LAB #3: ELECTROSTATIC FIELD COMPUTATION

LAB #3: ELECTROSTATIC FIELD COMPUTATION ECE 306 Revised: 1-6-00 LAB #3: ELECTROSTATIC FIELD COMPUTATION Purpose During tis lab you will investigate te ways in wic te electrostatic field can be teoretically predicted. Bot analytic and nuerical

More information

Combining functions: algebraic methods

Combining functions: algebraic methods Combining functions: algebraic metods Functions can be added, subtracted, multiplied, divided, and raised to a power, just like numbers or algebra expressions. If f(x) = x 2 and g(x) = x + 2, clearly f(x)

More information

U V. r In Uniform Field the Potential Difference is V Ed

U V. r In Uniform Field the Potential Difference is V Ed SPHI/W nit 7.8 Electric Potential Page of 5 Notes Physics Tool box Electric Potential Energy the electric potential energy stored in a syste k of two charges and is E r k Coulobs Constant is N C 9 9. E

More information

EE5900 Spring Lecture 4 IC interconnect modeling methods Zhuo Feng

EE5900 Spring Lecture 4 IC interconnect modeling methods Zhuo Feng EE59 Spring Parallel LSI AD Algoriths Lecture I interconnect odeling ethods Zhuo Feng. Z. Feng MTU EE59 So far we ve considered only tie doain analyses We ll soon see that it is soeties preferable to odel

More information

Faraday's Law Warm Up

Faraday's Law Warm Up Faraday's Law-1 Faraday's Law War Up 1. Field lines of a peranent agnet For each peranent agnet in the diagra below draw several agnetic field lines (or a agnetic vector field if you prefer) corresponding

More information

On the Impact of Stochastic Loads and Wind Generation on Under Load Tap Changers

On the Impact of Stochastic Loads and Wind Generation on Under Load Tap Changers On te Ipact of Stocastic Loads and Wind Generation on Under Load Tap Cangers M. A. A. Murad, Student Meber, IEEE, F. M. Mele, Student Meber, IEEE, F. Milano, Fellow, IEEE Scool of Electrical & Electronic

More information

Homotopy analysis of 1D unsteady, nonlinear groundwater flow through porous media

Homotopy analysis of 1D unsteady, nonlinear groundwater flow through porous media Hootopy analysis of D unsteady, nonlinear groundwater flow troug porous edia Autor Song, Hao, Tao, Longbin Publised 7 Journal Title Journal of Coastal Researc Copyrigt Stateent 7 CERF. Te attaced file

More information

Numerical Differentiation

Numerical Differentiation Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function

More information

HOW TO DEAL WITH FFT SAMPLING INFLUENCES ON ADEV CALCULATIONS

HOW TO DEAL WITH FFT SAMPLING INFLUENCES ON ADEV CALCULATIONS HOW TO DEAL WITH FFT SAMPLING INFLUENCES ON ADEV CALCULATIONS Po-Ceng Cang National Standard Time & Frequency Lab., TL, Taiwan 1, Lane 551, Min-Tsu Road, Sec. 5, Yang-Mei, Taoyuan, Taiwan 36 Tel: 886 3

More information

A Simplified Analytical Approach for Efficiency Evaluation of the Weaving Machines with Automatic Filling Repair

A Simplified Analytical Approach for Efficiency Evaluation of the Weaving Machines with Automatic Filling Repair Proceedings of the 6th SEAS International Conference on Siulation, Modelling and Optiization, Lisbon, Portugal, Septeber -4, 006 0 A Siplified Analytical Approach for Efficiency Evaluation of the eaving

More information

Determining Limits of Thermal NDT of Thick Graphite/Epoxy Composites

Determining Limits of Thermal NDT of Thick Graphite/Epoxy Composites ECNDT 006 - We.3.8.1 Deterining Liits of Teral NDT of Tick Grapite/Epoy Coposites Vladiir VAVILOV Institute of Introscopy Tosk Russia Abstract. Te known approac to inspecting tin coposites by using infrared

More information

Current Developments in the Field of Shock Calibration

Current Developments in the Field of Shock Calibration XVIII IMEKO WORLD CONGRESS Metrology for a Sustainale Developent Septeer, 17, 6, Rio de Janeiro, Brazil Current Developents in te Field of Sock Caliration T. Bruns 1, A. Link, C. Elster 3 1 Pysikalisc-Tecnisce

More information

1. Introduction. We consider the model problem: seeking an unknown function u satisfying

1. Introduction. We consider the model problem: seeking an unknown function u satisfying A DISCONTINUOUS LEAST-SQUARES FINITE ELEMENT METHOD FOR SECOND ORDER ELLIPTIC EQUATIONS XIU YE AND SHANGYOU ZHANG Abstract In tis paper, a discontinuous least-squares (DLS) finite element metod is introduced

More information

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015 Lecture : Transition State Teory. tkins & DePaula: 7.6-7.7 University o Wasinton Departent o Ceistry Ceistry 453 Winter Quarter 05. ctivated Kinetics Kinetic rate uations are overned by several principles.

More information

Physics Teach Yourself Series Topic 15: Wavelike nature of matter (Unit 4)

Physics Teach Yourself Series Topic 15: Wavelike nature of matter (Unit 4) Pysics Teac Yourself Series Topic 15: Wavelie nature of atter (Unit 4) A: Level 14, 474 Flinders Street Melbourne VIC 3000 T: 1300 134 518 W: tss.co.au E: info@tss.co.au TSSM 2017 Page 1 of 8 Contents

More information

NUCLEAR THERMAL-HYDRAULIC FUNDAMENTALS

NUCLEAR THERMAL-HYDRAULIC FUNDAMENTALS NUCLEAR THERMAL-HYDRAULIC FUNDAMENTALS Dr. J. Micael Doster Departent of Nuclear Engineering Nort Carolina State University Raleig, NC Copyrigted POER CYCLES Te analysis of Terodynaic Cycles is based alost

More information

UNCERTAINTIES IN THE APPLICATION OF ATMOSPHERIC AND ALTITUDE CORRECTIONS AS RECOMMENDED IN IEC STANDARDS

UNCERTAINTIES IN THE APPLICATION OF ATMOSPHERIC AND ALTITUDE CORRECTIONS AS RECOMMENDED IN IEC STANDARDS Paper Published on the16th International Syposiu on High Voltage Engineering, Cape Town, South Africa, 2009 UNCERTAINTIES IN THE APPLICATION OF ATMOSPHERIC AND ALTITUDE CORRECTIONS AS RECOMMENDED IN IEC

More information

About the definition of parameters and regimes of active two-port networks with variable loads on the basis of projective geometry

About the definition of parameters and regimes of active two-port networks with variable loads on the basis of projective geometry About the definition of paraeters and regies of active two-port networks with variable loads on the basis of projective geoetry PENN ALEXANDR nstitute of Electronic Engineering and Nanotechnologies "D

More information

th Annual IEEE Power Electronics Specialists Conference Aachen, Germany, Parallel Connection of Piezoelectric Transformers

th Annual IEEE Power Electronics Specialists Conference Aachen, Germany, Parallel Connection of Piezoelectric Transformers 004 35th Annual IEEE ower Electronics Specialists Conference Aachen, Gerany, 004 arallel Connection of iezoelectric Transforers Svetlana Bronstein, Gregory Ivensky and Sa Ben-Yaakov* ower Electronics Laboratory

More information

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015 Mat 3A Discussion Notes Week 4 October 20 and October 22, 205 To prepare for te first midterm, we ll spend tis week working eamples resembling te various problems you ve seen so far tis term. In tese notes

More information

Consider a function f we ll specify which assumptions we need to make about it in a minute. Let us reformulate the integral. 1 f(x) dx.

Consider a function f we ll specify which assumptions we need to make about it in a minute. Let us reformulate the integral. 1 f(x) dx. Capter 2 Integrals as sums and derivatives as differences We now switc to te simplest metods for integrating or differentiating a function from its function samples. A careful study of Taylor expansions

More information

Last lecture (#4): J vortex. J tr

Last lecture (#4): J vortex. J tr Last lecture (#4): We completed te discussion of te B-T pase diagram of type- and type- superconductors. n contrast to type-, te type- state as finite resistance unless vortices are pinned by defects.

More information

SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY

SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY (Section 3.2: Derivative Functions and Differentiability) 3.2.1 SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY LEARNING OBJECTIVES Know, understand, and apply te Limit Definition of te Derivative

More information

THE STURM-LIOUVILLE-TRANSFORMATION FOR THE SOLUTION OF VECTOR PARTIAL DIFFERENTIAL EQUATIONS. L. Trautmann, R. Rabenstein

THE STURM-LIOUVILLE-TRANSFORMATION FOR THE SOLUTION OF VECTOR PARTIAL DIFFERENTIAL EQUATIONS. L. Trautmann, R. Rabenstein Worksop on Transforms and Filter Banks (WTFB),Brandenburg, Germany, Marc 999 THE STURM-LIOUVILLE-TRANSFORMATION FOR THE SOLUTION OF VECTOR PARTIAL DIFFERENTIAL EQUATIONS L. Trautmann, R. Rabenstein Lerstul

More information

The derivative function

The derivative function Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Te derivative function Wat you need to know already: f is at a point on its grap and ow to compute it. Wat te derivative

More information

Numerical Studies of a Nonlinear Heat Equation with Square Root Reaction Term

Numerical Studies of a Nonlinear Heat Equation with Square Root Reaction Term Nuerical Studies of a Nonlinear Heat Equation with Square Root Reaction Ter Ron Bucire, 1 Karl McMurtry, 1 Ronald E. Micens 2 1 Matheatics Departent, Occidental College, Los Angeles, California 90041 2

More information

This exam is formed of three exercises in three pages numbered from 1 to 3 The use of non-programmable calculators is recommended.

This exam is formed of three exercises in three pages numbered from 1 to 3 The use of non-programmable calculators is recommended. 009 وزارة التربية والتعلين العالي الوديرية العاهة للتربية دائرة االهتحانات اهتحانات الشهادة الثانىية العاهة الفرع : علىم الحياة مسابقة في مادة الفيزياء المدة ساعتان االسن: الرقن: الدورة العادية للعام This

More information

Numerical Analysis MTH603. dy dt = = (0) , y n+1. We obtain yn. Therefore. and. Copyright Virtual University of Pakistan 1

Numerical Analysis MTH603. dy dt = = (0) , y n+1. We obtain yn. Therefore. and. Copyright Virtual University of Pakistan 1 Numerical Analysis MTH60 PREDICTOR CORRECTOR METHOD Te metods presented so far are called single-step metods, were we ave seen tat te computation of y at t n+ tat is y n+ requires te knowledge of y n only.

More information

Higher Derivatives. Differentiable Functions

Higher Derivatives. Differentiable Functions Calculus 1 Lia Vas Higer Derivatives. Differentiable Functions Te second derivative. Te derivative itself can be considered as a function. Te instantaneous rate of cange of tis function is te second derivative.

More information

OBJECTIVES INTRODUCTION

OBJECTIVES INTRODUCTION M7 Chapter 3 Section 1 OBJECTIVES Suarize data using easures of central tendency, such as the ean, edian, ode, and idrange. Describe data using the easures of variation, such as the range, variance, and

More information

Chapter 1: Basics of Vibrations for Simple Mechanical Systems

Chapter 1: Basics of Vibrations for Simple Mechanical Systems Chapter 1: Basics of Vibrations for Siple Mechanical Systes Introduction: The fundaentals of Sound and Vibrations are part of the broader field of echanics, with strong connections to classical echanics,

More information

Intelligent Systems: Reasoning and Recognition. Perceptrons and Support Vector Machines

Intelligent Systems: Reasoning and Recognition. Perceptrons and Support Vector Machines Intelligent Systes: Reasoning and Recognition Jaes L. Crowley osig 1 Winter Seester 2018 Lesson 6 27 February 2018 Outline Perceptrons and Support Vector achines Notation...2 Linear odels...3 Lines, Planes

More information

Study Committee B5 Colloquium 2005 September Calgary, CANADA

Study Committee B5 Colloquium 2005 September Calgary, CANADA 36 Study oittee B olloquiu Septeber 4-6 algary, ND ero Sequence urrent opensation for Distance Protection applied to Series opensated Parallel Lines TKHRO KSE* PHL G BEUMONT Toshiba nternational (Europe

More information

EE 330 Lecture 30. Basic amplifier architectures

EE 330 Lecture 30. Basic amplifier architectures 33 Lecture 3 asic aplifier architectures asic plifier Structures MOS and ipolar Transistors oth have 3 priary terinals MOS transistor has a fourth terinal that is generally considered a parasitic D terinal

More information

Proc. of the IEEE/OES Seventh Working Conference on Current Measurement Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES

Proc. of the IEEE/OES Seventh Working Conference on Current Measurement Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES Proc. of the IEEE/OES Seventh Working Conference on Current Measureent Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES Belinda Lipa Codar Ocean Sensors 15 La Sandra Way, Portola Valley, CA 98 blipa@pogo.co

More information

A note on the multiplication of sparse matrices

A note on the multiplication of sparse matrices Cent. Eur. J. Cop. Sci. 41) 2014 1-11 DOI: 10.2478/s13537-014-0201-x Central European Journal of Coputer Science A note on the ultiplication of sparse atrices Research Article Keivan Borna 12, Sohrab Aboozarkhani

More information

2 Q 10. Likewise, in case of multiple particles, the corresponding density in 2 must be averaged over all

2 Q 10. Likewise, in case of multiple particles, the corresponding density in 2 must be averaged over all Lecture 6 Introduction to kinetic theory of plasa waves Introduction to kinetic theory So far we have been odeling plasa dynaics using fluid equations. The assuption has been that the pressure can be either

More information

MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL 1 - BASIC DIFFERENTIATION

MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL 1 - BASIC DIFFERENTIATION MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL 1 - BASIC DIFFERENTIATION Tis tutorial is essential pre-requisite material for anyone stuing mecanical engineering. Tis tutorial uses te principle of

More information

Logarithmic functions

Logarithmic functions Roberto s Notes on Differential Calculus Capter 5: Derivatives of transcendental functions Section Derivatives of Logaritmic functions Wat ou need to know alread: Definition of derivative and all basic

More information

Main Points: 1. Limit of Difference Quotients. Prep 2.7: Derivatives and Rates of Change. Names of collaborators:

Main Points: 1. Limit of Difference Quotients. Prep 2.7: Derivatives and Rates of Change. Names of collaborators: Name: Section: Names of collaborators: Main Points:. Definition of derivative as limit of difference quotients. Interpretation of derivative as slope of grap. Interpretation of derivative as instantaneous

More information

Sensorless Control of Induction Motor Drive Using SVPWM - MRAS Speed Observer

Sensorless Control of Induction Motor Drive Using SVPWM - MRAS Speed Observer Journal of Eerging Trends in Engineering and Applied Sciences (JETEAS) 2 (3): 509-513 Journal Scholarlink of Eerging Research Trends Institute in Engineering Journals, 2011 and Applied (ISSN: 2141-7016)

More information

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March EN4: Dynaics and ibrations Midter Exaination Tuesday Marc 4 14 Scool of Engineering Brown University NAME: General Instructions No collaboration of any kind is peritted on tis exaination. You ay bring

More information

DYNAMIC TEMPERATURE FIELD IN THE FERROMAGNETIC PLATE INDUCED BY MOVING HIGH FREQUENCY INDUCTOR

DYNAMIC TEMPERATURE FIELD IN THE FERROMAGNETIC PLATE INDUCED BY MOVING HIGH FREQUENCY INDUCTOR Milosevic-Mitic, V., et al.: Dynaic Teperature Field in te Ferroagnetic plate induced by oving THERMAL SCIENCE: Year, Vol. 7, Suppl., pp. S47-S56 S47 DYNAMIC TEMPERATURE FIELD IN THE FERROMAGNETIC PLATE

More information

EE 330 Lecture 31. Basic amplifier architectures. Common Emitter/Source Common Collector/Drain Common Base/Gate

EE 330 Lecture 31. Basic amplifier architectures. Common Emitter/Source Common Collector/Drain Common Base/Gate 33 Lecture 3 asic aplifier architectures oon itter/source oon ollector/drain oon ase/gate eview fro arlier Lecture Two-port representation of aplifiers plifiers can be odeled as a two-port y 2 2 y y 22

More information

The Verlet Algorithm for Molecular Dynamics Simulations

The Verlet Algorithm for Molecular Dynamics Simulations Cemistry 380.37 Fall 2015 Dr. Jean M. Standard November 9, 2015 Te Verlet Algoritm for Molecular Dynamics Simulations Equations of motion For a many-body system consisting of N particles, Newton's classical

More information

A NEW ELECTROSTATIC FIELD GEOMETRY. Jerry E. Bayles

A NEW ELECTROSTATIC FIELD GEOMETRY. Jerry E. Bayles INTRODUCTION A NEW ELECTROSTATIC FIELD GEOMETRY by Jerry E Bayles The purpose of this paper is to present the electrostatic field in geoetrical ters siilar to that of the electrogravitational equation

More information

Spinning Disk and Chladni Plates

Spinning Disk and Chladni Plates Spinning Disk and Chladni Plates Subitted By MD MARUFUR RAHMAN Msc Sustainable Energy Systes Beng(Hons) Mechanical Engineering Bsc Coputer Science and Engineering Table of Contents Spinning Disk... 3 1.0

More information

An earlier article in this column considered the problem

An earlier article in this column considered the problem --- CALC CORNER Estiating nternal Air Cooling Teperature Reduction in a Closed Box Utilizing Theroelectrically Enhanced Heat Rejection Previously published in February, 2013 Bob Sions BM Retired The following

More information

CHAPTER 19: Single-Loop IMC Control

CHAPTER 19: Single-Loop IMC Control When I coplete this chapter, I want to be able to do the following. Recognize that other feedback algoriths are possible Understand the IMC structure and how it provides the essential control features

More information

Investigating Euler s Method and Differential Equations to Approximate π. Lindsay Crowl August 2, 2001

Investigating Euler s Method and Differential Equations to Approximate π. Lindsay Crowl August 2, 2001 Investigating Euler s Metod and Differential Equations to Approximate π Lindsa Crowl August 2, 2001 Tis researc paper focuses on finding a more efficient and accurate wa to approximate π. Suppose tat x

More information

The research of the rst author was supported in part by an Information Technology

The research of the rst author was supported in part by an Information Technology Tecnical Report 95-376 Absorbing Boundary Conditions for te Scrodinger Equation Toas Fevens Hong Jiang February 16, 1995 Te researc of te rst autor was supported in part by an Inforation Tecnology Researc

More information

Lecture 2 Introduction

Lecture 2 Introduction EE 333 POWER SYSTEMS ENGNEERNG Lecture 2 ntroduction Dr. Lei Wu Departent of Electrical and Coputer Engineering Clarkson University Resilient Underground Microgrid in Potsda, NY Funded by NYSERDAR + National

More information

Tangent Lines-1. Tangent Lines

Tangent Lines-1. Tangent Lines Tangent Lines- Tangent Lines In geometry, te tangent line to a circle wit centre O at a point A on te circle is defined to be te perpendicular line at A to te line OA. Te tangent lines ave te special property

More information

Research on Power Output Characteristics of Magnetic Core in Energy Harvesting Devices

Research on Power Output Characteristics of Magnetic Core in Energy Harvesting Devices Sensors & Transducers Vol. 74 Issue 7 July 04 pp. 53-59 Sensors & Transducers 04 by IFSA Publishing S. L. http://www.sensorsportal.co Research on Power Output Characteristics of Magnetic Core in Energy

More information

HARMONIC ALLOCATION TO MV CUSTOMERS IN RURAL DISTRIBUTION SYSTEMS

HARMONIC ALLOCATION TO MV CUSTOMERS IN RURAL DISTRIBUTION SYSTEMS HARMONIC ALLOCATION TO MV CUSTOMERS IN RURAL DISTRIBUTION SYSTEMS V Gosbell University of Wollongong Department of Electrical, Computer & Telecommunications Engineering, Wollongong, NSW 2522, Australia

More information

General Properties of Radiation Detectors Supplements

General Properties of Radiation Detectors Supplements Phys. 649: Nuclear Techniques Physics Departent Yarouk University Chapter 4: General Properties of Radiation Detectors Suppleents Dr. Nidal M. Ershaidat Overview Phys. 649: Nuclear Techniques Physics Departent

More information

The Design and Simulation of Electro-Hydraulic Velocity Control System

The Design and Simulation of Electro-Hydraulic Velocity Control System Te Design and Siulation of Electro-Hydraulic Velocity Control Syste Fengtao in * Key aboratory of Ministry of Education for Conveyance and Equipent, East Cina Jiaotong University, Nancang 330013, Cina

More information

AVOIDING PITFALLS IN MEASUREMENT UNCERTAINTY ANALYSIS

AVOIDING PITFALLS IN MEASUREMENT UNCERTAINTY ANALYSIS VOIDING ITFLLS IN ESREENT NERTINTY NLYSIS Benny R. Sith Inchwor Solutions Santa Rosa, Suary: itfalls, both subtle and obvious, await the new or casual practitioner of easureent uncertainty analysis. This

More information

DETECTION OF NONLINEARITY IN VIBRATIONAL SYSTEMS USING THE SECOND TIME DERIVATIVE OF ABSOLUTE ACCELERATION

DETECTION OF NONLINEARITY IN VIBRATIONAL SYSTEMS USING THE SECOND TIME DERIVATIVE OF ABSOLUTE ACCELERATION DETECTION OF NONLINEARITY IN VIBRATIONAL SYSTEMS USING THE SECOND TIME DERIVATIVE OF ABSOLUTE ACCELERATION Masaki WAKUI 1 and Jun IYAMA and Tsuyoshi KOYAMA 3 ABSTRACT This paper shows a criteria to detect

More information

Preface. Here are a couple of warnings to my students who may be here to get a copy of what happened on a day that you missed.

Preface. Here are a couple of warnings to my students who may be here to get a copy of what happened on a day that you missed. Preface Here are my online notes for my course tat I teac ere at Lamar University. Despite te fact tat tese are my class notes, tey sould be accessible to anyone wanting to learn or needing a refreser

More information

Effect of Mosquito Repellent on the Transmission Model of Chikungunya Fever

Effect of Mosquito Repellent on the Transmission Model of Chikungunya Fever Aerican Journal of Applied Sciences 9 (4): 563-569, ISSN 546-939 Science Publications Effect of Mosquito Repellent on te Transission Model of Cikungunya Fever Surapol Naowarat, Prasit Tongjae and I. Ming

More information

PH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition)

PH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) PH 1-A Fall 014 Waves - I Lectures 4-5 Chapter 16 (Halliday/Resnick/Walker, Fundaentals of Physics 9 th edition) 1 Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will

More information

Section 3.1: Derivatives of Polynomials and Exponential Functions

Section 3.1: Derivatives of Polynomials and Exponential Functions Section 3.1: Derivatives of Polynomials and Exponential Functions In previous sections we developed te concept of te derivative and derivative function. Te only issue wit our definition owever is tat it

More information

Exam 3 Solutions. 1. Which of the following statements is true about the LR circuit shown?

Exam 3 Solutions. 1. Which of the following statements is true about the LR circuit shown? PHY49 Spring 5 Prof. Darin Acosta Prof. Paul Avery April 4, 5 PHY49, Spring 5 Exa Solutions. Which of the following stateents is true about the LR circuit shown? It is (): () Just after the switch is closed

More information

Reading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6.

Reading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6. PHY10 Electricity Topic 6 (Lectures 9 & 10) Electric Current and Resistance n this topic, we will cover: 1) Current in a conductor ) Resistivity 3) Resistance 4) Oh s Law 5) The Drude Model of conduction

More information

Elastic Force: A Force Balance: Elastic & Gravitational Force: Force Example: Determining Spring Constant. Some Other Forces

Elastic Force: A Force Balance: Elastic & Gravitational Force: Force Example: Determining Spring Constant. Some Other Forces Energy Balance, Units & Proble Solving: Mechanical Energy Balance ABET Course Outcoes: 1. solve and docuent the solution of probles involving eleents or configurations not previously encountered (e) (e.g.

More information

2. A crack which is oblique (Swedish sned ) with respect to the xy coordinate system is to be analysed. TMHL

2. A crack which is oblique (Swedish sned ) with respect to the xy coordinate system is to be analysed. TMHL (Del I, teori; 1 p.) 1. In fracture echanics, the concept of energy release rate is iportant. Fro the fundaental energy balance of a case with possible crack growth, one usually derives the equation where

More information

A method to determine relative stroke detection efficiencies from multiplicity distributions

A method to determine relative stroke detection efficiencies from multiplicity distributions A ethod to deterine relative stroke detection eiciencies ro ultiplicity distributions Schulz W. and Cuins K. 2. Austrian Lightning Detection and Inoration Syste (ALDIS), Kahlenberger Str.2A, 90 Vienna,

More information

EXPERIMENTAL INVESTIGATION OF TANGENTIAL CONTACT STIFFNESS AND EQUIVALENT DAMPING

EXPERIMENTAL INVESTIGATION OF TANGENTIAL CONTACT STIFFNESS AND EQUIVALENT DAMPING Proceedings in Manufacturing Systes, Volue 7, Issue, ISSN 7-9 EXPERIMENTL INVESTIGTION OF TNGENTIL CONTCT STIFFNESS ND EQUIVLENT DMPING Iuliana PISCN,*, Tierry JNSSENS, Farid L-BENDER, Cristina PUPĂZĂ

More information

ma x = -bv x + F rod.

ma x = -bv x + F rod. Notes on Dynaical Systes Dynaics is the study of change. The priary ingredients of a dynaical syste are its state and its rule of change (also soeties called the dynaic). Dynaical systes can be continuous

More information

1 2 dispersion(leakage) reactance

1 2 dispersion(leakage) reactance Mircea cel Batran Naval Acadey cientific Bulletin, Volue XIV 0 Issue Publised by Mircea cel Batran Naval Acadey Press, Constanta, oania THE INDUCTION MACHINE. MODEING AND IMUATION. Florenţiu DEIU Paul

More information

lecture 26: Richardson extrapolation

lecture 26: Richardson extrapolation 43 lecture 26: Ricardson extrapolation 35 Ricardson extrapolation, Romberg integration Trougout numerical analysis, one encounters procedures tat apply some simple approximation (eg, linear interpolation)

More information

Properties of the Spin-flip Amplitude of Hadron Elastic Scattering and Possible Polarization Effects at RHIC

Properties of the Spin-flip Amplitude of Hadron Elastic Scattering and Possible Polarization Effects at RHIC Properties of te Spin-flip Amplitude of Hadron Elastic Scattering and Possible Polarization Effects at RHIC arxiv:ep-p/0210418v1 30 Oct 2002 O. V. Selyugin 1 Joint Institute for Nuclear Researc, Dubna,

More information