On the Meaning of Message Sequence Charts

Size: px
Start display at page:

Download "On the Meaning of Message Sequence Charts"

Transcription

1 On the Meaning of Message Sequence Chats Manfed Boy Institut fü Infomatik Technische Univesität München Topics: We discuss Message Sequence Chats (MSCs) as a technique to descibe pattens of the inteaction between the components of a inteactive system as a technique to specify the behavio of the components of a system thei systematic use in the softwae development pocess Questions: What is the fomal meaning of a MSC fo the components of a system? How can MSCs be combined? What is the fomal meaning of a set of MSCs? How fa can MSCs seve as a pecise and compehensive mean of specification? What type of systems do MSCs efe to and what popeties do they specify pecisely? What is the methodological ole of MSCs and how do they fit into the development pocess? Pof. D. Manfed Boy: MeanMSC The Pupose of Message Sequence Chats LSTORE location c unlocked lock(p, c) location c unlocked MSCs as logical popeties of systems. locked(p, c) MSCs as pedicates on system components. location c locked fo pocess p Example: Component x: StoeIn y: StoeOut location c locked fo pocess p Reading and witing location c unlock(p, c) unlocked(p, c) location c locked fo pocess p LSTORE location c unlocked Pof. D. Manfed Boy: MeanMSC Successful Access to the Stoe Pof. D. Manfed Boy: MeanMSC

2 ENVIRONMENT x": StoeIn CACHE y": StoeOut CACHE x : StoeIn MANAGER x" s : StoeIn z : StoeIn y : StoeOut :StoeIn t : StoeOut s: StoeIn z: StoeOut LSTORE intenal Cache as a Data Flow Node LSTORE extenal Cache as a Netwok of Data Flow Nodes Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC location c unlocked location c locked fo pocess p in extenal stoe location c locked fo pocess p in intenal stoe location c ead fom extenal stoe Scenaios lock(p, c) Manage lock(p, c) locked(p, c) lock(p, c) locked(p, c) ead(p, c) ead(p, c, d) wite(p, c, d) LST ORE intenal LSTORE extenal Selected System Model Components x1: S1 f y1: S1' xn: Sn ym: Sm' location c updated in intenal stoe location c locked fo pocess p and updated locked(p, c) witten(p, c) Message Sequence Chat fo Successful Locking I be the set of input channels O be the set of output channels. With evey channel in the cannel set I O we associate a data type (I, O) is the syntactic inteface of a system component is given. Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC

3 Steams Valuations of channels Mω = Μ Μ steams of messages of set M C set of channels finite o infinite sequences of elements fom M type: C S types assigned to channels Mϖ set of infinite steams fom set M { } with an infinite numbe of time ticks. [s] caie set of data elements M = U{[s]: s S} M be the univese of all messages x: C Mϖ valuations of C Mϖ N M { }. whee fo each c C: x(c) [s]ϖ C set of valuations Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC Black box behavio of a component Composed Systems by data flow nets f : I ( O) x k = z k {y k+1: y f(x)} = {y k+1: y f(z)} I/O-functions timing popety. N set of identifies fo components (I M ω ) (O M ω ) time abstaction f.x = {y O M ω : z I: z = x y f.z} (ν, O) distibuted system with syntactic inteface (I, O) ν: N Com Com[I, O] set of I/O-functions with input channels I and output channels O. Black box view: f Com[I, O] whee f(x) = {y O: y I = x i N: y Out(ν(i)) ν(i)(y In(ν(i)) ) } Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC

4 Towads a Meaning of MSCs Questions Given a netwok of inteacting components with syntactic inteface (I, O) (ν: N Com, O) MSCs define (1) Is the component p descibed by the theads of the MSCs deteministic? (2) Is the component, afte a patten of behavio as specified, in a state whee again MSCs ae available to descibe the behavio? (3) Ae the MSCs dense pefixes, pojections, o fee selections of instances of inteactions? a pedicate Q p : I p ( O p ) (4) Is the set of MSCs meant as a loose sample o a compehensive set of equiements? fo each component p N epesented by a thead in the MSC. Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC Syntax and Stuctued Pesentation of MSCs t 1 t 2... t i... t n A MSC is a diagam with n vetical lines, called the theads, one fo each component of the system, that symbolize the flow of time fo each component time flows fom the top to the bottom. (1) i 1 (1) o 1 (1) i 2 (1) o 2 i 1 (2) (k) i 1 (2) o 1 M (j) o 1 (2) i 2 o 2 (2) M M M Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC

5 Causal consistency of MSCs t i A MSC is called consistent, if fo all its events thee is i o a patial odeing that contains the linea odeings of all the theads as subodeings (fo a compehensive discussion see [Alu et al. 96]). This means: no cycles in the causality flow of the events (no "causal loops"). Geneal Fom of a Thead in a MSC with Clusteed Input/Output An input o output patten is a finite channel valuation C * fo the channels in C which is defined as a mapping C (M { }) *. Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC Semantics of Sets of MSCs Specifying Deteministic Systems The Semantics of MSCs fo Nondeteministic Systems Behavio of a deteministic system component A nondeteministic system component is intepeted by a set valued function I O I ( O) The MSC is epesented by the equation f(i) = o and the specifying fomula o f(i) We call a function f compehensive with espect to a set of MSCs if it fulfills the specifying fomulas. Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC

6 Intoducing Contol and Data States f The Univese of Unfilteed Scenaios We get a set of conditional fomulas of the geneal foms i o χ: P(σ) o condition(x, y) y f σ χ (x) χ': Q(σ, σ ) condition(x, y) y = f χ σ (x) By choosing all instantiations fo the input histoy x and the output histoy y o f σ χ (i) P(σ) fo 1 k < n χ o ˆf σ (x) f χ σ (iˆx) P(σ) Q(σ, σ') This leads to a system of specifications of the function f σ χ. y f χ σ (x) o y = f χ σ (x) fo concete histoies y O and x I. Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC MSCs as Pojections Closed Wold Assumptions - A Canonical Behavio with a Set of MSCs Given pojection functions fo a steam x witten in the fom x N We specify then a set of MSCs by the fomulas i = x N y f(x): o = y N intepetion of the theads of a component: pojection: a MSC descibes a pefix of a pojection of the input and output, loose selection: a MSC descibes a loose selection of messages. This set of the pattens is called the filteed univese of inteaction pattens. An I/O-function I ( O) connects infinite input histoies with infinite output histoies. We define the meaning of a set of theads fo the function f by f * : I * ( O * ) whee fo a set of channels C we define C * as the set of valuations C (M * ) * (M * ) pefix odeing ffi Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC

7 DCS( O * ) = {Z C * : Z z C : z ffi x x Z z Z} * The patial odeing that we use on the set DCS is simply set inclusion. We define the function f * such that f * : I * DCS( O * ) Fo set of fomulas R = {Φ k : k K} whee each Φ k is of the fom y k f(x k ) o f(x kˆx') y kˆf(x') we specify the function f * as the -least time guaded function whee y k f * (x k ) Closues on the Canonical Behavio The function f * is completed into an I/O-function I ( O) by the following equation: f.x = {y O: k N: y k f * (x) k N: y k f * (x) y' f * (x): y k ffi y' y k = y'} f * (x kˆx') y kˆf * (x') Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC The constuction of the chaotic closue The Methodological Role of MSCs The function f is the inclusion lagest function with the following popeties: (1) f is time guaded, (2) if thee is a MSC that talks about the input x, then f(x) contains exactly those outputs explicitly descibed in one of the MSCs. (3) if fo an input x we can decompose x into x'ˆx'' such that exactly fo the input patten in x' output is specified by the MSCs we define the output fo x'' as being abitay. (1) In the ealy phases of equiements engineeing to get a fist idea which sevices the system should povide. (2) In the late phases of equiements engineeing as desciption techniques as pat of a fomal specification. (3) In the design phase illustation of the inteaction between the system pats (key technique fo the decomposition of a system, design pattens). (4) In the implementation phase we use MSCs to epesent test cases. In paticula, wheneve fo some input an input patten is not contained in a set of MSCs, the output can be abitay (chaos). Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC

8 Popety efinement Fist answe [Klein 98] ˆ I ( O) is called a popety efinement of a component with a behavio Let us undestand a set of scenaios as I ( O) the specification of the components if fo all input steams x I we have: ˆf(x) f(x) Conflict between efinement and equiements captue by sets of MSCs: # efinement steps that allow us to get id of nondeteministic altenatives, # the sets of MSCs that ae assumed to descibe all behavios that all should be possible. that shows fo input pattens coveed by scenaios exactly the behavio descibed by the scenaios and fo the input pattens not coveed abitay behavio. See "closed wold assumption". Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC Second Answe to the Conflict Refinement/Sets of MSCs Conclusion Distinguishing two kinds of MSCs Seveal ways to intepet sets of MSCs - Good MSCs: MSCs that descibe the intended behavio and inteaction, Bad MSCs: MSCs that descibe unwanted behavio, modeling failue cases that, howeve, have to be toleated, but should be avoided wheneve possible. Negative scenaios may be eliminated in efinement steps wheneve feasible. Suggested concepts: distinction between input messages and output messages essential. leads to a concept of causality. MSCs as component specifications MSCs in that way do not only descibe by an MSC vey loosely what may happen in a system but also quite stictly what must happen. Pof. D. Manfed Boy: MeanMSC Pof. D. Manfed Boy: MeanMSC

ANA BERRIZBEITIA, LUIS A. MEDINA, ALEXANDER C. MOLL, VICTOR H. MOLL, AND LAINE NOBLE

ANA BERRIZBEITIA, LUIS A. MEDINA, ALEXANDER C. MOLL, VICTOR H. MOLL, AND LAINE NOBLE THE p-adic VALUATION OF STIRLING NUMBERS ANA BERRIZBEITIA, LUIS A. MEDINA, ALEXANDER C. MOLL, VICTOR H. MOLL, AND LAINE NOBLE Abstact. Let p > 2 be a pime. The p-adic valuation of Stiling numbes of the

More information

Surveillance Points in High Dimensional Spaces

Surveillance Points in High Dimensional Spaces Société de Calcul Mathématique SA Tools fo decision help since 995 Suveillance Points in High Dimensional Spaces by Benad Beauzamy Januay 06 Abstact Let us conside any compute softwae, elying upon a lage

More information

4/18/2005. Statistical Learning Theory

4/18/2005. Statistical Learning Theory Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse

More information

Encapsulation theory: radial encapsulation. Edmund Kirwan *

Encapsulation theory: radial encapsulation. Edmund Kirwan * Encapsulation theoy: adial encapsulation. Edmund Kiwan * www.edmundkiwan.com Abstact This pape intoduces the concept of adial encapsulation, wheeby dependencies ae constained to act fom subsets towads

More information

Vanishing lines in generalized Adams spectral sequences are generic

Vanishing lines in generalized Adams spectral sequences are generic ISSN 364-0380 (on line) 465-3060 (pinted) 55 Geomety & Topology Volume 3 (999) 55 65 Published: 2 July 999 G G G G T T T G T T T G T G T GG TT G G G G GG T T T TT Vanishing lines in genealized Adams spectal

More information

The Implementation of the Conditions for the Existence of the Most Specific Generalizations w.r.t. General EL-TBoxes

The Implementation of the Conditions for the Existence of the Most Specific Generalizations w.r.t. General EL-TBoxes The Implementation of the Conditions fo the Existence of the Most Specific Genealizations w..t. Geneal EL-TBoxes Adian Nuadiansyah Technische Univesität Desden Supevised by: Anni-Yasmin Tuhan Febuay 12,

More information

Pushdown Automata (PDAs)

Pushdown Automata (PDAs) CHAPTER 2 Context-Fee Languages Contents Context-Fee Gammas definitions, examples, designing, ambiguity, Chomsky nomal fom Pushdown Automata definitions, examples, euivalence with context-fee gammas Non-Context-Fee

More information

Physics 2A Chapter 10 - Moment of Inertia Fall 2018

Physics 2A Chapter 10 - Moment of Inertia Fall 2018 Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.

More information

Lecture 28: Convergence of Random Variables and Related Theorems

Lecture 28: Convergence of Random Variables and Related Theorems EE50: Pobability Foundations fo Electical Enginees July-Novembe 205 Lectue 28: Convegence of Random Vaiables and Related Theoems Lectue:. Kishna Jagannathan Scibe: Gopal, Sudhasan, Ajay, Swamy, Kolla An

More information

Research Design - - Topic 17 Multiple Regression & Multiple Correlation: Two Predictors 2009 R.C. Gardner, Ph.D.

Research Design - - Topic 17 Multiple Regression & Multiple Correlation: Two Predictors 2009 R.C. Gardner, Ph.D. Reseach Design - - Topic 7 Multiple Regession & Multiple Coelation: Two Pedictos 009 R.C. Gadne, Ph.D. Geneal Rationale and Basic Aithmetic fo two pedictos Patial and semipatial coelation Regession coefficients

More information

EM Boundary Value Problems

EM Boundary Value Problems EM Bounday Value Poblems 10/ 9 11/ By Ilekta chistidi & Lee, Seung-Hyun A. Geneal Desciption : Maxwell Equations & Loentz Foce We want to find the equations of motion of chaged paticles. The way to do

More information

Syntactical content of nite approximations of partial algebras 1 Wiktor Bartol Inst. Matematyki, Uniw. Warszawski, Warszawa (Poland)

Syntactical content of nite approximations of partial algebras 1 Wiktor Bartol Inst. Matematyki, Uniw. Warszawski, Warszawa (Poland) Syntactical content of nite appoximations of patial algebas 1 Wikto Batol Inst. Matematyki, Uniw. Waszawski, 02-097 Waszawa (Poland) batol@mimuw.edu.pl Xavie Caicedo Dep. Matematicas, Univ. de los Andes,

More information

BIFURCATION ANALYSIS FOR A QUASI-LINEAR CENTRIFUGAL PENDULUM ABSORBER

BIFURCATION ANALYSIS FOR A QUASI-LINEAR CENTRIFUGAL PENDULUM ABSORBER 11 th Intenational Confeence on Vibation Poblems Z. Dimitovová et al. (eds.) Lisbon, Potugal, 9-12 Septembe 213 BIFURCATION ANALYSIS FOR A QUASI-LINEAR CENTRIFUGAL PENDULUM ABSORBER Eugen B. Keme* 1, Mikhail

More information

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD

More information

A Bijective Approach to the Permutational Power of a Priority Queue

A Bijective Approach to the Permutational Power of a Priority Queue A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation

More information

Deterministic vs Non-deterministic Graph Property Testing

Deterministic vs Non-deterministic Graph Property Testing Deteministic vs Non-deteministic Gaph Popety Testing Lio Gishboline Asaf Shapia Abstact A gaph popety P is said to be testable if one can check whethe a gaph is close o fa fom satisfying P using few andom

More information

Tutorial Exercises: Central Forces

Tutorial Exercises: Central Forces Tutoial Execises: Cental Foces. Tuning Points fo the Keple potential (a) Wite down the two fist integals fo cental motion in the Keple potential V () = µm/ using J fo the angula momentum and E fo the total

More information

Hydroelastic Analysis of a 1900 TEU Container Ship Using Finite Element and Boundary Element Methods

Hydroelastic Analysis of a 1900 TEU Container Ship Using Finite Element and Boundary Element Methods TEAM 2007, Sept. 10-13, 2007,Yokohama, Japan Hydoelastic Analysis of a 1900 TEU Containe Ship Using Finite Element and Bounday Element Methods Ahmet Egin 1)*, Levent Kaydıhan 2) and Bahadı Uğulu 3) 1)

More information

The Substring Search Problem

The Substring Search Problem The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is

More information

THE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX. Jaejin Lee

THE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX. Jaejin Lee Koean J. Math. 23 (2015), No. 3, pp. 427 438 http://dx.doi.og/10.11568/kjm.2015.23.3.427 THE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX Jaejin Lee Abstact. The Schensted algoithm fist descibed by Robinson

More information

PAPER 39 STOCHASTIC NETWORKS

PAPER 39 STOCHASTIC NETWORKS MATHEMATICAL TRIPOS Pat III Tuesday, 2 June, 2015 1:30 pm to 4:30 pm PAPER 39 STOCHASTIC NETWORKS Attempt no moe than FOUR questions. Thee ae FIVE questions in total. The questions cay equal weight. STATIONERY

More information

The second law of thermodynamics - II.

The second law of thermodynamics - II. Januay 21, 2013 The second law of themodynamics - II. Asaf Pe e 1 1. The Schottky defect At absolute zeo tempeatue, the atoms of a solid ae odeed completely egulaly on a cystal lattice. As the tempeatue

More information

DonnishJournals

DonnishJournals DonnishJounals 041-1189 Donnish Jounal of Educational Reseach and Reviews. Vol 1(1) pp. 01-017 Novembe, 014. http:///dje Copyight 014 Donnish Jounals Oiginal Reseach Pape Vecto Analysis Using MAXIMA Savaş

More information

UNIT 13: ANGULAR MOMENTUM AND TORQUE AS VECTORS Approximate Classroom Time: Two 100 minute sessions

UNIT 13: ANGULAR MOMENTUM AND TORQUE AS VECTORS Approximate Classroom Time: Two 100 minute sessions Name SFU e-mail @sfu.ca Date(YY/MM/DD) / / Section Goup UNIT 13: ANGULAR MOMENTUM AND TORQUE AS VECTORS Appoximate Classoom Time: Two 100 minute sessions Help! Pue logical thinking cannot yield us any

More information

Lecture 2 - Thermodynamics Overview

Lecture 2 - Thermodynamics Overview 2.625 - Electochemical Systems Fall 2013 Lectue 2 - Themodynamics Oveview D.Yang Shao-Hon Reading: Chapte 1 & 2 of Newman, Chapte 1 & 2 of Bad & Faulkne, Chaptes 9 & 10 of Physical Chemisty I. Lectue Topics:

More information

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations Intenational Jounal of Recent Tends in Engineeing, Vol, No., May 9 Steady State and Tansient Pefomance Analysis of Thee Phase Induction Machine using MATAB Simulations Pof. Himanshu K. Patel Assistant

More information

you of a spring. The potential energy for a spring is given by the parabola U( x)

you of a spring. The potential energy for a spring is given by the parabola U( x) Small oscillations The theoy of small oscillations is an extemely impotant topic in mechanics. Conside a system that has a potential enegy diagam as below: U B C A x Thee ae thee points of stable equilibium,

More information

A Short Combinatorial Proof of Derangement Identity arxiv: v1 [math.co] 13 Nov Introduction

A Short Combinatorial Proof of Derangement Identity arxiv: v1 [math.co] 13 Nov Introduction A Shot Combinatoial Poof of Deangement Identity axiv:1711.04537v1 [math.co] 13 Nov 2017 Ivica Matinjak Faculty of Science, Univesity of Zageb Bijenička cesta 32, HR-10000 Zageb, Coatia and Dajana Stanić

More information

Chapter 7-8 Rotational Motion

Chapter 7-8 Rotational Motion Chapte 7-8 Rotational Motion What is a Rigid Body? Rotational Kinematics Angula Velocity ω and Acceleation α Unifom Rotational Motion: Kinematics Unifom Cicula Motion: Kinematics and Dynamics The Toque,

More information

Long-range stress re-distribution resulting from damage in heterogeneous media

Long-range stress re-distribution resulting from damage in heterogeneous media Long-ange stess e-distibution esulting fom damage in heteogeneous media Y.L.Bai (1), F.J.Ke (1,2), M.F.Xia (1,3) X.H.Zhang (1) and Z.K. Jia (1) (1) State Key Laboatoy fo Non-linea Mechanics (LNM), Institute

More information

Sesqui-pushout rewriting

Sesqui-pushout rewriting Sesqui-pushout ewiting Andea Coadini Dipatimento di Infomatica, Pisa, Italy IFIP WG 1.3 - La Roche en Adennes, June 6, 2006. Joint wok with Tobias Heindel Fank Hemann Babaa König Univesität Stuttgat, Gemany

More information

To Feel a Force Chapter 7 Static equilibrium - torque and friction

To Feel a Force Chapter 7 Static equilibrium - torque and friction To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on

More information

Stress, Cauchy s equation and the Navier-Stokes equations

Stress, Cauchy s equation and the Navier-Stokes equations Chapte 3 Stess, Cauchy s equation and the Navie-Stokes equations 3. The concept of taction/stess Conside the volume of fluid shown in the left half of Fig. 3.. The volume of fluid is subjected to distibuted

More information

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations MATH 415, WEEK 3: Paamete-Dependence and Bifucations 1 A Note on Paamete Dependence We should pause to make a bief note about the ole played in the study of dynamical systems by the system s paametes.

More information

Lecture 18: Graph Isomorphisms

Lecture 18: Graph Isomorphisms INFR11102: Computational Complexity 22/11/2018 Lectue: Heng Guo Lectue 18: Gaph Isomophisms 1 An Athu-Melin potocol fo GNI Last time we gave a simple inteactive potocol fo GNI with pivate coins. We will

More information

Vector d is a linear vector function of vector d when the following relationships hold:

Vector d is a linear vector function of vector d when the following relationships hold: Appendix 4 Dyadic Analysis DEFINITION ecto d is a linea vecto function of vecto d when the following elationships hold: d x = a xxd x + a xy d y + a xz d z d y = a yxd x + a yy d y + a yz d z d z = a zxd

More information

( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx.

( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx. 9. LAGRANGIAN OF THE ELECTROMAGNETIC FIELD In the pevious section the Lagangian and Hamiltonian of an ensemble of point paticles was developed. This appoach is based on a qt. This discete fomulation can

More information

Lifting Private Information Retrieval from Two to any Number of Messages

Lifting Private Information Retrieval from Two to any Number of Messages Lifting Pivate Infomation Retieval fom Two to any umbe of Messages Rafael G.L. D Oliveia, Salim El Rouayheb ECE, Rutges Univesity, Piscataway, J Emails: d746@scaletmail.utges.edu, salim.elouayheb@utges.edu

More information

1D2G - Numerical solution of the neutron diffusion equation

1D2G - Numerical solution of the neutron diffusion equation DG - Numeical solution of the neuton diffusion equation Y. Danon Daft: /6/09 Oveview A simple numeical solution of the neuton diffusion equation in one dimension and two enegy goups was implemented. Both

More information

Psychometric Methods: Theory into Practice Larry R. Price

Psychometric Methods: Theory into Practice Larry R. Price ERRATA Psychometic Methods: Theoy into Pactice Lay R. Pice Eos wee made in Equations 3.5a and 3.5b, Figue 3., equations and text on pages 76 80, and Table 9.1. Vesions of the elevant pages that include

More information

A Formal Account of the Open Provenance Model

A Formal Account of the Open Provenance Model Fomal ccount of the Open ovenance Model Natalia Kwasnikowska Hasselt Univesity and Tansnational Univesity of Limbug Belgium Luc Moeau Univesity of Southampton United Kingdom Jan Van den Bussche Hasselt

More information

Topic 4a Introduction to Root Finding & Bracketing Methods

Topic 4a Introduction to Root Finding & Bracketing Methods /8/18 Couse Instucto D. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: cumpf@utep.edu Topic 4a Intoduction to Root Finding & Backeting Methods EE 4386/531 Computational Methods in EE Outline

More information

New problems in universal algebraic geometry illustrated by boolean equations

New problems in universal algebraic geometry illustrated by boolean equations New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic

More information

On decompositions of complete multipartite graphs into the union of two even cycles

On decompositions of complete multipartite graphs into the union of two even cycles On decompositions of complete multipatite gaphs into the union of two even cycles A. Su, J. Buchanan, R. C. Bunge, S. I. El-Zanati, E. Pelttai, G. Rasmuson, E. Spaks, S. Tagais Depatment of Mathematics

More information

Simple model of skeletal matter composed of magnetized electrically conducting thin rods

Simple model of skeletal matter composed of magnetized electrically conducting thin rods Simple model of skeletal matte composed of magnetized electically conducting thin ods A.B. Kukushkin, K.V. Cheepanov NFI RRC Kuchatov Institute, Moscow, 1318, Russia A simple electodynamic model fo descibing

More information

Qualifying Examination Electricity and Magnetism Solutions January 12, 2006

Qualifying Examination Electricity and Magnetism Solutions January 12, 2006 1 Qualifying Examination Electicity and Magnetism Solutions Januay 12, 2006 PROBLEM EA. a. Fist, we conside a unit length of cylinde to find the elationship between the total chage pe unit length λ and

More information

Fall 2016 Semester METR 3113 Atmospheric Dynamics I: Introduction to Atmospheric Kinematics and Dynamics

Fall 2016 Semester METR 3113 Atmospheric Dynamics I: Introduction to Atmospheric Kinematics and Dynamics Fall 06 Semeste METR 33 Atmospheic Dynamics I: Intoduction to Atmospheic Kinematics Dynamics Lectue 7 Octobe 3 06 Topics: Scale analysis of the equations of hoizontal motion Geostophic appoximation eostophic

More information

PS113 Chapter 5 Dynamics of Uniform Circular Motion

PS113 Chapter 5 Dynamics of Uniform Circular Motion PS113 Chapte 5 Dynamics of Unifom Cicula Motion 1 Unifom cicula motion Unifom cicula motion is the motion of an object taveling at a constant (unifom) speed on a cicula path. The peiod T is the time equied

More information

10/04/18. P [P(x)] 1 negl(n).

10/04/18. P [P(x)] 1 negl(n). Mastemath, Sping 208 Into to Lattice lgs & Cypto Lectue 0 0/04/8 Lectues: D. Dadush, L. Ducas Scibe: K. de Boe Intoduction In this lectue, we will teat two main pats. Duing the fist pat we continue the

More information

LINEAR MOMENTUM Physical quantities that we have been using to characterize the motion of a particle

LINEAR MOMENTUM Physical quantities that we have been using to characterize the motion of a particle LINEAR MOMENTUM Physical quantities that we have been using to chaacteize the otion of a paticle v Mass Velocity v Kinetic enegy v F Mechanical enegy + U Linea oentu of a paticle (1) is a vecto! Siple

More information

Merging Uncertain Multi-Version XML Documents

Merging Uncertain Multi-Version XML Documents Meging Uncetain Multi-Vesion XML Documents M. Lamine BA, Talel Abdessalem & Piee Senellat ACM DocEng 2013-1st Intenational Wokshop on Document Changes (Floence, Italy) Septembe 10 th, 2013 M. L. Ba, T.

More information

Explosive Contagion in Networks (Supplementary Information)

Explosive Contagion in Networks (Supplementary Information) Eplosive Contagion in Netwoks (Supplementay Infomation) Jesús Gómez-Gadeñes,, Laua Loteo, Segei N. Taaskin, and Fancisco J. Péez-Reche Institute fo Biocomputation and Physics of Comple Systems (BIFI),

More information

Maintaining Consistency in Layered Architectures of Mobile Ad-Hoc Networks

Maintaining Consistency in Layered Architectures of Mobile Ad-Hoc Networks Maintaining Consistency in Layeed Achitectues of Mobile Ad-Hoc Netwoks Julia Padbeg, Kathin Hoffmann, Hatmut Ehig, Tony Modica, Enico Biemann, and Claudia Emel Institute fo Softwae Technology and Theoetical

More information

Review Notes on Maxwell's Equations

Review Notes on Maxwell's Equations ELEC344 Micowave Engineeing, Sping 2002 Handout #1 Kevin Chen Review Notes on Maxwell's Equations Review of Vecto Poducts and the Opeato The del, gad o nabla opeato is a vecto, and can be pat of a scala

More information

F-IF Logistic Growth Model, Abstract Version

F-IF Logistic Growth Model, Abstract Version F-IF Logistic Gowth Model, Abstact Vesion Alignments to Content Standads: F-IFB4 Task An impotant example of a model often used in biology o ecology to model population gowth is called the logistic gowth

More information

I. CONSTRUCTION OF THE GREEN S FUNCTION

I. CONSTRUCTION OF THE GREEN S FUNCTION I. CONSTRUCTION OF THE GREEN S FUNCTION The Helmohltz equation in 4 dimensions is 4 + k G 4 x, x = δ 4 x x. In this equation, G is the Geen s function and 4 efes to the dimensionality. In the vey end,

More information

Math 124B February 02, 2012

Math 124B February 02, 2012 Math 24B Febuay 02, 202 Vikto Gigoyan 8 Laplace s equation: popeties We have aleady encounteed Laplace s equation in the context of stationay heat conduction and wave phenomena. Recall that in two spatial

More information

Functions Defined on Fuzzy Real Numbers According to Zadeh s Extension

Functions Defined on Fuzzy Real Numbers According to Zadeh s Extension Intenational Mathematical Foum, 3, 2008, no. 16, 763-776 Functions Defined on Fuzzy Real Numbes Accoding to Zadeh s Extension Oma A. AbuAaqob, Nabil T. Shawagfeh and Oma A. AbuGhneim 1 Mathematics Depatment,

More information

A Comparison and Contrast of Some Methods for Sample Quartiles

A Comparison and Contrast of Some Methods for Sample Quartiles A Compaison and Contast of Some Methods fo Sample Quatiles Anwa H. Joade and aja M. Latif King Fahd Univesity of Petoleum & Mineals ABSTACT A emainde epesentation of the sample size n = 4m ( =, 1, 2, 3)

More information

Waves and Polarization in General

Waves and Polarization in General Waves and Polaization in Geneal Wave means a distubance in a medium that tavels. Fo light, the medium is the electomagnetic field, which can exist in vacuum. The tavel pat defines a diection. The distubance

More information

Markscheme May 2017 Calculus Higher level Paper 3

Markscheme May 2017 Calculus Higher level Paper 3 M7/5/MATHL/HP3/ENG/TZ0/SE/M Makscheme May 07 Calculus Highe level Pape 3 pages M7/5/MATHL/HP3/ENG/TZ0/SE/M This makscheme is the popety of the Intenational Baccalaueate and must not be epoduced o distibuted

More information

Safety variations in steel designed using Eurocode 3

Safety variations in steel designed using Eurocode 3 JCSS Wokshop on eliability Based Code Calibation Safety vaiations in steel designed using Euocode 3 Mike Byfield Canfield Univesity Swindon, SN6 8LA, UK David Nethecot Impeial College London SW7 2BU, UK

More information

Duality between Statical and Kinematical Engineering Systems

Duality between Statical and Kinematical Engineering Systems Pape 00, Civil-Comp Ltd., Stiling, Scotland Poceedings of the Sixth Intenational Confeence on Computational Stuctues Technology, B.H.V. Topping and Z. Bittna (Editos), Civil-Comp Pess, Stiling, Scotland.

More information

ADVANCED SUBSIDIARY (AS) General Certificate of Education Mathematics Assessment Unit F1. assessing. Module FP1: Further Pure Mathematics 1

ADVANCED SUBSIDIARY (AS) General Certificate of Education Mathematics Assessment Unit F1. assessing. Module FP1: Further Pure Mathematics 1 ADVACED SUBSIDIARY (AS) Geneal Cetificate of Education 15 Mathematics Assessment Unit F1 assessing Module F1: Futhe ue Mathematics 1 [AMF11] WEDESDAY 4 UE, MRIG MAR SCHEME 958.1 F GCE ADVACED/ADVACED SUBSIDIARY

More information

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0}, ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability

More information

Exploration of the three-person duel

Exploration of the three-person duel Exploation of the thee-peson duel Andy Paish 15 August 2006 1 The duel Pictue a duel: two shootes facing one anothe, taking tuns fiing at one anothe, each with a fixed pobability of hitting his opponent.

More information

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up

More information

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018 Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field

More information

Using Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu

Using Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu Available at https://edupediapublicationsog/jounals Volume 3 Issue 4 Febuay 216 Using Laplace Tansfom to Evaluate Impope Integals Chii-Huei Yu Depatment of Infomation Technology, Nan Jeon Univesity of

More information

3.1 Random variables

3.1 Random variables 3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated

More information

A Crash Course in (2 2) Matrices

A Crash Course in (2 2) Matrices A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula

More information

B. Spherical Wave Propagation

B. Spherical Wave Propagation 11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We

More information

c n ψ n (r)e ient/ h (2) where E n = 1 mc 2 α 2 Z 2 ψ(r) = c n ψ n (r) = c n = ψn(r)ψ(r)d 3 x e 2r/a0 1 πa e 3r/a0 r 2 dr c 1 2 = 2 9 /3 6 = 0.

c n ψ n (r)e ient/ h (2) where E n = 1 mc 2 α 2 Z 2 ψ(r) = c n ψ n (r) = c n = ψn(r)ψ(r)d 3 x e 2r/a0 1 πa e 3r/a0 r 2 dr c 1 2 = 2 9 /3 6 = 0. Poblem {a} Fo t : Ψ(, t ψ(e iet/ h ( whee E mc α (α /7 ψ( e /a πa Hee we have used the gound state wavefunction fo Z. Fo t, Ψ(, t can be witten as a supeposition of Z hydogenic wavefunctions ψ n (: Ψ(,

More information

Chapter 5 Linear Equations: Basic Theory and Practice

Chapter 5 Linear Equations: Basic Theory and Practice Chapte 5 inea Equations: Basic Theoy and actice In this chapte and the next, we ae inteested in the linea algebaic equation AX = b, (5-1) whee A is an m n matix, X is an n 1 vecto to be solved fo, and

More information

15 Solving the Laplace equation by Fourier method

15 Solving the Laplace equation by Fourier method 5 Solving the Laplace equation by Fouie method I aleady intoduced two o thee dimensional heat equation, when I deived it, ecall that it taes the fom u t = α 2 u + F, (5.) whee u: [0, ) D R, D R is the

More information

APPENDIX. For the 2 lectures of Claude Cohen-Tannoudji on Atom-Atom Interactions in Ultracold Quantum Gases

APPENDIX. For the 2 lectures of Claude Cohen-Tannoudji on Atom-Atom Interactions in Ultracold Quantum Gases APPENDIX Fo the lectues of Claude Cohen-Tannoudji on Atom-Atom Inteactions in Ultacold Quantum Gases Pupose of this Appendix Demonstate the othonomalization elation(ϕ ϕ = δ k k δ δ )k - The wave function

More information

HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS?

HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS? 6th INTERNATIONAL MULTIDISCIPLINARY CONFERENCE HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS? Cecília Sitkuné Göömbei College of Nyíegyháza Hungay Abstact: The

More information

Brief summary of functional analysis APPM 5440 Fall 2014 Applied Analysis

Brief summary of functional analysis APPM 5440 Fall 2014 Applied Analysis Bief summay of functional analysis APPM 5440 Fall 014 Applied Analysis Stephen Becke, stephen.becke@coloado.edu Standad theoems. When necessay, I used Royden s and Keyzsig s books as a efeence. Vesion

More information

arxiv: v1 [quant-ph] 15 Nov 2018

arxiv: v1 [quant-ph] 15 Nov 2018 Bayesian estimation of switching ates fo blinking emittes axiv:8.6627v [quant-ph] 5 Nov 28 Jemy Geody,, 2 Lachlan J Roges,, 2, Cameon M Roges, 3 Thomas Volz,, 2 and Alexei Gilchist, 2 Depatment of Physics

More information

FUSE Fusion Utility Sequence Estimator

FUSE Fusion Utility Sequence Estimator FUSE Fusion Utility Sequence Estimato Belu V. Dasaathy Dynetics, Inc. P. O. Box 5500 Huntsville, AL 3584-5500 belu.d@dynetics.com Sean D. Townsend Dynetics, Inc. P. O. Box 5500 Huntsville, AL 3584-5500

More information

Synthesis for Unbounded Bit-vector Arithmetic

Synthesis for Unbounded Bit-vector Arithmetic Synthesis fo Unbounded Bit-vecto Aithmetic Andej Spielmann and Vikto Kuncak School of Compute and Communication Sciences (I&C) École Polytechnique Fédéale de Lausanne (EPFL), Switzeland Abstact. We popose

More information

MULTILAYER PERCEPTRONS

MULTILAYER PERCEPTRONS Last updated: Nov 26, 2012 MULTILAYER PERCEPTRONS Outline 2 Combining Linea Classifies Leaning Paametes Outline 3 Combining Linea Classifies Leaning Paametes Implementing Logical Relations 4 AND and OR

More information

A Markov Decision Approach for the Computation of Testability of RTL Constructs

A Markov Decision Approach for the Computation of Testability of RTL Constructs A Makov Decision Appoach fo the Computation of Testability of RTL Constucts José Miguel Fenandes Abstact In the analysis of digital cicuits, to study testability estimation measues, dissipated powe and

More information

MATH 417 Homework 3 Instructor: D. Cabrera Due June 30. sin θ v x = v r cos θ v θ r. (b) Then use the Cauchy-Riemann equations in polar coordinates

MATH 417 Homework 3 Instructor: D. Cabrera Due June 30. sin θ v x = v r cos θ v θ r. (b) Then use the Cauchy-Riemann equations in polar coordinates MATH 417 Homewok 3 Instucto: D. Cabea Due June 30 1. Let a function f(z) = u + iv be diffeentiable at z 0. (a) Use the Chain Rule and the fomulas x = cosθ and y = to show that u x = u cosθ u θ, v x = v

More information

A Converse to Low-Rank Matrix Completion

A Converse to Low-Rank Matrix Completion A Convese to Low-Rank Matix Completion Daniel L. Pimentel-Alacón, Robet D. Nowak Univesity of Wisconsin-Madison Abstact In many pactical applications, one is given a subset Ω of the enties in a d N data

More information

Hammerstein Model Identification Based On Instrumental Variable and Least Square Methods

Hammerstein Model Identification Based On Instrumental Variable and Least Square Methods Intenational Jounal of Emeging Tends & Technology in Compute Science (IJETTCS) Volume 2, Issue, Januay Febuay 23 ISSN 2278-6856 Hammestein Model Identification Based On Instumental Vaiable and Least Squae

More information

ATMO 551a Fall 08. Diffusion

ATMO 551a Fall 08. Diffusion Diffusion Diffusion is a net tanspot of olecules o enegy o oentu o fo a egion of highe concentation to one of lowe concentation by ando olecula) otion. We will look at diffusion in gases. Mean fee path

More information

Interaction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r)

Interaction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r) Supplementay mateial fo Inteaction of Feedfowad and Feedback Steams in Visual Cotex in a Fiing-Rate Model of Columna Computations Tobias Bosch and Heiko Neumann Institute fo Neual Infomation Pocessing

More information

Journal of Inequalities in Pure and Applied Mathematics

Journal of Inequalities in Pure and Applied Mathematics Jounal of Inequalities in Pue and Applied Mathematics COEFFICIENT INEQUALITY FOR A FUNCTION WHOSE DERIVATIVE HAS A POSITIVE REAL PART S. ABRAMOVICH, M. KLARIČIĆ BAKULA AND S. BANIĆ Depatment of Mathematics

More information

On the Comparison of Stability Analysis with Phase Portrait for a Discrete Prey-Predator System

On the Comparison of Stability Analysis with Phase Portrait for a Discrete Prey-Predator System Intenational Jounal of Applied Engineeing Reseach ISSN 0973-4562 Volume 12, Nume 24 (2017) pp. 15273-15277 Reseach India Pulications. http://www.ipulication.com On the Compaison of Staility Analysis with

More information

Nuclear Medicine Physics 02 Oct. 2007

Nuclear Medicine Physics 02 Oct. 2007 Nuclea Medicine Physics Oct. 7 Counting Statistics and Eo Popagation Nuclea Medicine Physics Lectues Imaging Reseach Laboatoy, Radiology Dept. Lay MacDonald 1//7 Statistics (Summaized in One Slide) Type

More information

Three-dimensional Quantum Cellular Neural Network and Its Application to Image Processing *

Three-dimensional Quantum Cellular Neural Network and Its Application to Image Processing * Thee-dimensional Quantum Cellula Neual Netwok and Its Application to Image Pocessing * Sen Wang, Li Cai, Huanqing Cui, Chaowen Feng, Xiaokuo Yang Science College, Ai Foce Engineeing Univesity Xi an 701,

More information

Probablistically Checkable Proofs

Probablistically Checkable Proofs Lectue 12 Pobablistically Checkable Poofs May 13, 2004 Lectue: Paul Beame Notes: Chis Re 12.1 Pobablisitically Checkable Poofs Oveview We know that IP = PSPACE. This means thee is an inteactive potocol

More information

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra Poceedings of the 006 IASME/SEAS Int. Conf. on ate Resouces, Hydaulics & Hydology, Chalkida, Geece, May -3, 006 (pp7-) Analytical Solutions fo Confined Aquifes with non constant Pumping using Compute Algeba

More information

TheWaveandHelmholtzEquations

TheWaveandHelmholtzEquations TheWaveandHelmholtzEquations Ramani Duaiswami The Univesity of Mayland, College Pak Febuay 3, 2006 Abstact CMSC828D notes (adapted fom mateial witten with Nail Gumeov). Wok in pogess 1 Acoustic Waves 1.1

More information

Compactly Supported Radial Basis Functions

Compactly Supported Radial Basis Functions Chapte 4 Compactly Suppoted Radial Basis Functions As we saw ealie, compactly suppoted functions Φ that ae tuly stictly conditionally positive definite of ode m > do not exist The compact suppot automatically

More information

Voltage ( = Electric Potential )

Voltage ( = Electric Potential ) V-1 of 10 Voltage ( = lectic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage

More information

EN40: Dynamics and Vibrations. Midterm Examination Thursday March

EN40: Dynamics and Vibrations. Midterm Examination Thursday March EN40: Dynamics and Vibations Midtem Examination Thusday Mach 9 2017 School of Engineeing Bown Univesity NAME: Geneal Instuctions No collaboation of any kind is pemitted on this examination. You may bing

More information

A Primer For Conant & Ashby's Good-Regulator Theorem

A Primer For Conant & Ashby's Good-Regulator Theorem A Pime Fo Conant & Ashby's Good-Regulato Theoem by Daniel L. Scholten Page 2 of 44 Table of Contents Intoduction...3 What the theoem claims...4 Poving the claim...9 The Regulato's Responsiveness to the

More information

arxiv: v1 [math.co] 1 Apr 2011

arxiv: v1 [math.co] 1 Apr 2011 Weight enumeation of codes fom finite spaces Relinde Juius Octobe 23, 2018 axiv:1104.0172v1 [math.co] 1 Ap 2011 Abstact We study the genealized and extended weight enumeato of the - ay Simplex code and

More information