Chapter 4. Moving Observer Method. 4.1 Overview. 4.2 Theory

Size: px
Start display at page:

Download "Chapter 4. Moving Observer Method. 4.1 Overview. 4.2 Theory"

Transcription

1 Chapter 4 Moving Observer Method 4.1 Overview For a compete description of traffic stream modeing, one woud reuire fow, speed, and density. Obtaining these parameters simutaneousy is a difficut task if we use separate techniues. Since we have a fundamenta euation of traffic fow, which gives the fow as the product of density and space mean speed, if we knew any two parameters, the third can be computed. Moving car or moving observer method of traffic stream measurement has been deveoped to provide simutaneous measurement of traffic stream variabes. It has the advantage of obtaining the compete state with just three observers, and a vehice. Determination of any of the two parameters of the traffic fow wi provide the third one by the euation = u.k. Thus, moving observer method is the most commony used method to get the reationship between the fundamenta stream characteristics. In this method, the observer moves in the traffic stream unike a other previous methods. 4.2 Theory Consider a stream of vehices moving in the north bound direction. Two different cases of motion can be considered. The first case considers the traffic stream to be moving and the observer to be stationary. If n o is the number of vehices overtaking the observer during a period, t, then fow is n 0 t, or n 0 = t (4.1) The second case assumes that the stream is stationary and the observer moves with speed v o. If n p is the number of vehices overtaken by observer over a ength, then by definition, density k is np n p = k (4.2) Dr. Tom V. Mathew, IIT Bombay 4.1 February 19, 2014

2 Figure 4:1: Iustration of moving observer method or n p = k.v o.t (4.3) where v 0 is the speed of the observer and t is the time taken for the observer to cover the road stretch. Now consider the case when the observer is moving within the stream. In that case m o vehices wi overtake the observer and m p vehices wi be overtaken by the observer in the test vehice. Let the difference m is given by m 0 - m p, then from euation 4.1 and euation 4.3, m = m 0 m p = t k v o t (4.4) This euation is the basic euation of moving observer method, which reates, k to the counts m, t and v o that can be obtained from the test. However, we have two unknowns, and k, but ony one euation. For generating another euation, the test vehice is run twice once with the traffic stream and another one against traffic stream, i.e. m w = t w k v w t w (4.5) = t w k m a = t a + k v a t a (4.6) = t a + k where, a, w denotes against and with traffic fow. It may be noted that the sign of euation 4.6 is negative, because test vehice moving in the opposite direction can be considered as a case when the test vehice is moving in the stream with negative veocity. Further, in this case, a the vehices wi be overtaking, since it is moving with negative speed. In other words, when the test vehice moves in the opposite direction, the observer simpy counts the number of vehices in the opposite direction. Adding euation 4.5 and 4.6, we wi get the first parameter of the Dr. Tom V. Mathew, IIT Bombay 4.2 February 19, 2014

3 stream, namey the fow() as: Now cacuating space mean speed from euation 4.5, = m w + m a t w + t a (4.7) m w t w = kv w = v v w [ ] = v t ( w = 1 v 1 ) t ( w = 1 t ) avg t w If v s is the mean stream speed, then average trave time is given by t avg = v s. Therefore, m w t avg = t w (1 t avg t w ) = t w t avg = t w m w = v, Rewriting the above euation, we get the second parameter of the traffic fow, namey the mean speed v s and can be written as, v s = t w mw Thus two parameters of the stream can be determined. Knowing the two parameters the third parameter of traffic fow density (k) can be found out as (4.8) k = v s (4.9) For increase accuracy and reiabiity, the test is performed a number of times and the average resuts are to be taken. Dr. Tom V. Mathew, IIT Bombay 4.3 February 19, 2014

4 4.3 Proof 4.4 Assumptions Numerica Exampe The ength of a road stretch used for conducting the moving observer test is 0.5 km and the speed with which the test vehice moved is 20 km/hr. Given that the number of vehices encountered in the stream whie the test vehice was moving against the traffic stream is 107, number of vehices that had overtaken the test vehice is 10, and the number of vehices overtaken by the test vehice is 74, find the fow, density and average speed of the stream. Soution Time taken by the test vehice to reach the other end of the stream whie it is moving aong with the traffic is t w = 0.5 = hr 20 Time taken by the observer to reach the other end of the stream whie it is moving against the traffic is t a = t w = hr Fow is given by euation, = 107+(10 74) = 860 veh/hr Stream speed v s can be found out from euationv s = = 5 km/hr Density can be found out from euation as k = 860 = 172veh/km 5 Numerica Exampe The data from four moving observer test methods are shown in the tabe. Coumn 1 gives the sampe number, coumn 2 gives the number of vehices moving against the stream, coumn 3 gives the number of vehices that had overtaken the test vehice, and ast coumn gives the number of vehices overtaken by the test vehice. Find the three fundamenta stream parameters for each set of data. Aso pot the fundamenta diagrams of traffic fow. Sampe no Soution From the cacuated vaues of fow, density and speed, the three fundamenta diagrams can be potted as shown in figure 4:2. Dr. Tom V. Mathew, IIT Bombay 4.4 February 19, 2014

5 Sampe no. m a m o m p m w = (m o m p ) t a t w = ma+mw t a+t w u = t w mw k = v speed u density k speed u fow fow density k Figure 4:2: Fundamenta diagrams of traffic fow Dr. Tom V. Mathew, IIT Bombay 4.5 February 19, 2014

6 4.5 Summary Traffic engineering studies differ from other studies in the fact that they reuire extensive data from the fied which cannot be exacty created in any aboratory. Speed data are coected from measurements at a point or over a short section or over an area. Traffic fow data are coected at a point. Moving observer method is one in which both speed and traffic fow data are obtained by a singe experiment. 4.6 References 1. L. R Kadiyai. Traffic Engineering and Transportation Panning. Khanna Pubishers, New Dehi, Dr. Tom V. Mathew, IIT Bombay 4.6 February 19, 2014

Traffic data collection

Traffic data collection Chapter 32 Traffic data coection 32.1 Overview Unike many other discipines of the engineering, the situations that are interesting to a traffic engineer cannot be reproduced in a aboratory. Even if road

More information

Tracking Control of Multiple Mobile Robots

Tracking Control of Multiple Mobile Robots Proceedings of the 2001 IEEE Internationa Conference on Robotics & Automation Seou, Korea May 21-26, 2001 Tracking Contro of Mutipe Mobie Robots A Case Study of Inter-Robot Coision-Free Probem Jurachart

More information

(Refer Slide Time: 2:34) L C V

(Refer Slide Time: 2:34) L C V Microwave Integrated Circuits Professor Jayanta Mukherjee Department of Eectrica Engineering Indian Intitute of Technoogy Bombay Modue 1 Lecture No 2 Refection Coefficient, SWR, Smith Chart. Heo wecome

More information

Physics 235 Chapter 8. Chapter 8 Central-Force Motion

Physics 235 Chapter 8. Chapter 8 Central-Force Motion Physics 35 Chapter 8 Chapter 8 Centra-Force Motion In this Chapter we wi use the theory we have discussed in Chapter 6 and 7 and appy it to very important probems in physics, in which we study the motion

More information

An Implementation Parallel Monte Carlo Method for Traffic Flow Simulation

An Implementation Parallel Monte Carlo Method for Traffic Flow Simulation An Impementation Parae Monte Caro Method for Traffic Fow Simuation Hsun-Jun Cho and Fan-Yu Lai Department of Transportation Enineerin and Manaement Nationa Chiao Tun University Ta Hsueh Road, Hsinchu Taiwan

More information

Mass Transport 2: Fluids Outline

Mass Transport 2: Fluids Outline ass Transport : Fuids Outine Diffusivity in soids, iquids, gases Fick s 1st aw in fuid systems Diffusion through a stagnant gas fim Fick s nd aw Diffusion in porous media Knudsen diffusion ass Transfer

More information

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries c 26 Noninear Phenomena in Compex Systems First-Order Corrections to Gutzwier s Trace Formua for Systems with Discrete Symmetries Hoger Cartarius, Jörg Main, and Günter Wunner Institut für Theoretische

More information

RELUCTANCE The resistance of a material to the flow of charge (current) is determined for electric circuits by the equation

RELUCTANCE The resistance of a material to the flow of charge (current) is determined for electric circuits by the equation INTRODUCTION Magnetism pays an integra part in amost every eectrica device used today in industry, research, or the home. Generators, motors, transformers, circuit breakers, teevisions, computers, tape

More information

FOURIER SERIES ON ANY INTERVAL

FOURIER SERIES ON ANY INTERVAL FOURIER SERIES ON ANY INTERVAL Overview We have spent considerabe time earning how to compute Fourier series for functions that have a period of 2p on the interva (-p,p). We have aso seen how Fourier series

More information

Preamble. Flow and Fluid Velocity. In this section of my lectures we will be. To do this we will use as an analogy

Preamble. Flow and Fluid Velocity. In this section of my lectures we will be. To do this we will use as an analogy Preambe Resistance Physics, 8 th Edition Custom Edition Cutne & Johnson Chapter 20.3 Pages 602-605 In this section of my ectures we wi be deveoping the concept of resistance. To do this we wi use as an

More information

A mezoscopic vehicles pursuit model for managing traffic during a massive evacuation

A mezoscopic vehicles pursuit model for managing traffic during a massive evacuation A mezoscopic vehices pursuit mode for managing traffic during a massive evacuation Houssein Aaeddine a,b, Mindjid Maizia a, Kama Serrhini a, Emmanue Néron b a Laboratoire Citères de université de Tours

More information

Copyright information to be inserted by the Publishers. Unsplitting BGK-type Schemes for the Shallow. Water Equations KUN XU

Copyright information to be inserted by the Publishers. Unsplitting BGK-type Schemes for the Shallow. Water Equations KUN XU Copyright information to be inserted by the Pubishers Unspitting BGK-type Schemes for the Shaow Water Equations KUN XU Mathematics Department, Hong Kong University of Science and Technoogy, Cear Water

More information

Path planning with PH G2 splines in R2

Path planning with PH G2 splines in R2 Path panning with PH G2 spines in R2 Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru To cite this version: Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru. Path panning with PH G2 spines

More information

Forces of Friction. through a viscous medium, there will be a resistance to the motion. and its environment

Forces of Friction. through a viscous medium, there will be a resistance to the motion. and its environment Forces of Friction When an object is in motion on a surface or through a viscous medium, there wi be a resistance to the motion This is due to the interactions between the object and its environment This

More information

LECTURE 10. The world of pendula

LECTURE 10. The world of pendula LECTURE 0 The word of pendua For the next few ectures we are going to ook at the word of the pane penduum (Figure 0.). In a previous probem set we showed that we coud use the Euer- Lagrange method to derive

More information

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l Probem 7. Simpe Penduum SEMINAR. PENDULUMS A simpe penduum means a mass m suspended by a string weightess rigid rod of ength so that it can swing in a pane. The y-axis is directed down, x-axis is directed

More information

AAPT UNITED STATES PHYSICS TEAM AIP 2012 DO NOT DISTRIBUTE THIS PAGE

AAPT UNITED STATES PHYSICS TEAM AIP 2012 DO NOT DISTRIBUTE THIS PAGE 2012 Semifina Exam 1 AAPT UNITED STATES PHYSICS TEAM AIP 2012 Semifina Exam DO NOT DISTRIBUTE THIS PAGE Important Instructions for the Exam Supervisor This examination consists of two parts. Part A has

More information

VTU-NPTEL-NMEICT Project

VTU-NPTEL-NMEICT Project MODUE-X -CONTINUOUS SYSTEM : APPROXIMATE METHOD VIBRATION ENGINEERING 14 VTU-NPTE-NMEICT Project Progress Report The Project on Deveopment of Remaining Three Quadrants to NPTE Phase-I under grant in aid

More information

Physics Dynamics: Springs

Physics Dynamics: Springs F A C U L T Y O F E D U C A T I O N Department of Curricuum and Pedagogy Physics Dynamics: Springs Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund

More information

Lecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String

Lecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String ecture Notes for Math 251: ODE and PDE. ecture 3: 1.7 Wave Equation and Vibrations of an Eastic String Shawn D. Ryan Spring 212 ast Time: We studied other Heat Equation probems with various other boundary

More information

Related Topics Maxwell s equations, electrical eddy field, magnetic field of coils, coil, magnetic flux, induced voltage

Related Topics Maxwell s equations, electrical eddy field, magnetic field of coils, coil, magnetic flux, induced voltage Magnetic induction TEP Reated Topics Maxwe s equations, eectrica eddy fied, magnetic fied of cois, coi, magnetic fux, induced votage Principe A magnetic fied of variabe frequency and varying strength is

More information

Uniprocessor Feasibility of Sporadic Tasks with Constrained Deadlines is Strongly conp-complete

Uniprocessor Feasibility of Sporadic Tasks with Constrained Deadlines is Strongly conp-complete Uniprocessor Feasibiity of Sporadic Tasks with Constrained Deadines is Strongy conp-compete Pontus Ekberg and Wang Yi Uppsaa University, Sweden Emai: {pontus.ekberg yi}@it.uu.se Abstract Deciding the feasibiity

More information

EVERYDAY EXAMPLES OF ENGINEERING CONCEPTS

EVERYDAY EXAMPLES OF ENGINEERING CONCEPTS EVERYDAY EXAMPLES OF ENGINEERING CONCEPTS F7: Simiitude & dimensiona anaysis Copyright 04 This work is icensed under the Creative Commons Attribution-NonCommercia-NoDerivs.0 Unported License. To view a

More information

6.434J/16.391J Statistics for Engineers and Scientists May 4 MIT, Spring 2006 Handout #17. Solution 7

6.434J/16.391J Statistics for Engineers and Scientists May 4 MIT, Spring 2006 Handout #17. Solution 7 6.434J/16.391J Statistics for Engineers and Scientists May 4 MIT, Spring 2006 Handout #17 Soution 7 Probem 1: Generating Random Variabes Each part of this probem requires impementation in MATLAB. For the

More information

Incorporation of surface tension to interface energy balance in crystal growth

Incorporation of surface tension to interface energy balance in crystal growth Cryst. Res. Techno. 42, No. 9, 914 919 (2007) / OI 10.1002/crat.200710927 Incorporation of surface tension to interface energy baance in crysta growth M. Yidiz and. ost* Crysta Growth aboratory, epartment

More information

Acoustic Nondestructive Testing and Measurement of Tension for Steel Reinforcing Members

Acoustic Nondestructive Testing and Measurement of Tension for Steel Reinforcing Members Acoustic Nondestructive Testing and Measurement of Tension for Stee Reinforcing Members Part 1 Theory by Michae K. McInerney PURPOSE: This Coasta and Hydrauics Engineering Technica Note (CHETN) describes

More information

Two-sample inference for normal mean vectors based on monotone missing data

Two-sample inference for normal mean vectors based on monotone missing data Journa of Mutivariate Anaysis 97 (006 6 76 wwweseviercom/ocate/jmva Two-sampe inference for norma mean vectors based on monotone missing data Jianqi Yu a, K Krishnamoorthy a,, Maruthy K Pannaa b a Department

More information

Paper presented at the Workshop on Space Charge Physics in High Intensity Hadron Rings, sponsored by Brookhaven National Laboratory, May 4-7,1998

Paper presented at the Workshop on Space Charge Physics in High Intensity Hadron Rings, sponsored by Brookhaven National Laboratory, May 4-7,1998 Paper presented at the Workshop on Space Charge Physics in High ntensity Hadron Rings, sponsored by Brookhaven Nationa Laboratory, May 4-7,998 Noninear Sef Consistent High Resoution Beam Hao Agorithm in

More information

Traffic Density Estimation with the Cell Transmission Model 1

Traffic Density Estimation with the Cell Transmission Model 1 Traffic Density Estimation ith the Ce Transmission Mode Laura Muñoz, Xiaotian Sun, Roberto Horoitz 2, Luis Avarez 3 Department of Mechanica Engineering University of Caifornia at Berkeey Berkeey, CA 9472-174

More information

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE KATIE L. MAY AND MELISSA A. MITCHELL Abstract. We show how to identify the minima path network connecting three fixed points on

More information

Metal Oxide Semiconductor Field Effect Transistors (MOSFETs) Prof. Ali M. Niknejad Prof. Rikky Muller

Metal Oxide Semiconductor Field Effect Transistors (MOSFETs) Prof. Ali M. Niknejad Prof. Rikky Muller EECS 105 Spring 2017, Modue 3 Meta Oxide Semiconductor Fied Effect Transistors (MOSFETs) Prof. Ai M. Niknejad Prof. Rikky Muer Department of EECS University of Caifornia, Berkeey Announcements Prof. Rikky

More information

SydU STAT3014 (2015) Second semester Dr. J. Chan 18

SydU STAT3014 (2015) Second semester Dr. J. Chan 18 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Stratified Random Samping.1 Introduction Description The popuation of size N is divided into mutuay excusive and exhaustive subpopuations caed

More information

Combining reaction kinetics to the multi-phase Gibbs energy calculation

Combining reaction kinetics to the multi-phase Gibbs energy calculation 7 th European Symposium on Computer Aided Process Engineering ESCAPE7 V. Pesu and P.S. Agachi (Editors) 2007 Esevier B.V. A rights reserved. Combining reaction inetics to the muti-phase Gibbs energy cacuation

More information

СРАВНИТЕЛЕН АНАЛИЗ НА МОДЕЛИ НА ГРЕДИ НА ЕЛАСТИЧНА ОСНОВА COMPARATIVE ANALYSIS OF ELASTIC FOUNDATION MODELS FOR BEAMS

СРАВНИТЕЛЕН АНАЛИЗ НА МОДЕЛИ НА ГРЕДИ НА ЕЛАСТИЧНА ОСНОВА COMPARATIVE ANALYSIS OF ELASTIC FOUNDATION MODELS FOR BEAMS СРАВНИТЕЛЕН АНАЛИЗ НА МОДЕЛИ НА ГРЕДИ НА ЕЛАСТИЧНА ОСНОВА Милко Стоянов Милошев 1, Константин Савков Казаков 2 Висше Строително Училище Л. Каравелов - София COMPARATIVE ANALYSIS OF ELASTIC FOUNDATION MODELS

More information

CE601-Structura Anaysis I UNIT-IV SOPE-DEFECTION METHOD 1. What are the assumptions made in sope-defection method? (i) Between each pair of the supports the beam section is constant. (ii) The joint in

More information

GOYAL BROTHERS PRAKASHAN

GOYAL BROTHERS PRAKASHAN Assignments in Mathematics Cass IX (Term 2) 14. STATISTICS IMPORTANT TERMS, DEFINITIONS AND RESULTS The facts or figures, which are numerica or otherwise, coected with a definite purpose are caed data.

More information

Problem Set 6: Solutions

Problem Set 6: Solutions University of Aabama Department of Physics and Astronomy PH 102 / LeCair Summer II 2010 Probem Set 6: Soutions 1. A conducting rectanguar oop of mass M, resistance R, and dimensions w by fas from rest

More information

A Statistical Framework for Real-time Event Detection in Power Systems

A Statistical Framework for Real-time Event Detection in Power Systems 1 A Statistica Framework for Rea-time Event Detection in Power Systems Noan Uhrich, Tim Christman, Phiip Swisher, and Xichen Jiang Abstract A quickest change detection (QCD) agorithm is appied to the probem

More information

EECS 117 Homework Assignment 3 Spring ω ω. ω ω. ω ω. Using the values of the inductance and capacitance, the length of 2 cm corresponds 1.5π.

EECS 117 Homework Assignment 3 Spring ω ω. ω ω. ω ω. Using the values of the inductance and capacitance, the length of 2 cm corresponds 1.5π. EES 7 Homework Assignment Sprg 4. Suppose the resonant frequency is equa to ( -.5. The oad impedance is If, is equa to ( ( The ast equaity hods because ( -.5. Furthermore, ( Usg the vaues of the ductance

More information

How the backpropagation algorithm works Srikumar Ramalingam School of Computing University of Utah

How the backpropagation algorithm works Srikumar Ramalingam School of Computing University of Utah How the backpropagation agorithm works Srikumar Ramaingam Schoo of Computing University of Utah Reference Most of the sides are taken from the second chapter of the onine book by Michae Nieson: neuranetworksanddeepearning.com

More information

A Brief Introduction to Markov Chains and Hidden Markov Models

A Brief Introduction to Markov Chains and Hidden Markov Models A Brief Introduction to Markov Chains and Hidden Markov Modes Aen B MacKenzie Notes for December 1, 3, &8, 2015 Discrete-Time Markov Chains You may reca that when we first introduced random processes,

More information

Efficiently Generating Random Bits from Finite State Markov Chains

Efficiently Generating Random Bits from Finite State Markov Chains 1 Efficienty Generating Random Bits from Finite State Markov Chains Hongchao Zhou and Jehoshua Bruck, Feow, IEEE Abstract The probem of random number generation from an uncorreated random source (of unknown

More information

High Efficiency Development of a Reciprocating Compressor by Clarification of Loss Generation in Bearings

High Efficiency Development of a Reciprocating Compressor by Clarification of Loss Generation in Bearings Purdue University Purdue e-pubs Internationa Compressor Engineering Conference Schoo of Mechanica Engineering 2010 High Efficiency Deveopment of a Reciprocating Compressor by Carification of Loss Generation

More information

Seasonal Time Series Data Forecasting by Using Neural Networks Multiscale Autoregressive Model

Seasonal Time Series Data Forecasting by Using Neural Networks Multiscale Autoregressive Model American ourna of Appied Sciences 7 (): 372-378, 2 ISSN 546-9239 2 Science Pubications Seasona Time Series Data Forecasting by Using Neura Networks Mutiscae Autoregressive Mode Suhartono, B.S.S. Uama and

More information

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes Maima and Minima 1. Introduction In this Section we anayse curves in the oca neighbourhood of a stationary point and, from this anaysis, deduce necessary conditions satisfied by oca maima and oca minima.

More information

THINKING IN PYRAMIDS

THINKING IN PYRAMIDS ECS 178 Course Notes THINKING IN PYRAMIDS Kenneth I. Joy Institute for Data Anaysis and Visuaization Department of Computer Science University of Caifornia, Davis Overview It is frequenty usefu to think

More information

Numerical Simulation for Optimizing Temperature Gradients during Single Crystal Casting Process

Numerical Simulation for Optimizing Temperature Gradients during Single Crystal Casting Process ISIJ Internationa Vo 54 (2014) No 2 pp 254 258 Numerica Simuation for Optimizing Temperature Gradients during Singe Crysta Casting Process Aeksandr Aeksandrovich INOZEMTSEV 1) Aeksandra Sergeevna DUBROVSKAYA

More information

Selmer groups and Euler systems

Selmer groups and Euler systems Semer groups and Euer systems S. M.-C. 21 February 2018 1 Introduction Semer groups are a construction in Gaois cohomoogy that are cosey reated to many objects of arithmetic importance, such as cass groups

More information

Maintenance activities planning and grouping for complex structure systems

Maintenance activities planning and grouping for complex structure systems Maintenance activities panning and grouping for compex structure systems Hai Canh u, Phuc Do an, Anne Barros, Christophe Bérenguer To cite this version: Hai Canh u, Phuc Do an, Anne Barros, Christophe

More information

Computational Investigation of Arc Behavior in an Auto-Expansion Circuit Breaker with Gases of SF 6 and N 2 **

Computational Investigation of Arc Behavior in an Auto-Expansion Circuit Breaker with Gases of SF 6 and N 2 ** Computationa Investigation of Arc Behavior in an Auto-Expansion Circuit Breaker with Gases of SF 6 and N 2 ** Jining Zhang Abstract An eectric arc behavior in a fu-scae 245 kv autoexpansion circuit breaker

More information

Laboratory Exercise 1: Pendulum Acceleration Measurement and Prediction Laboratory Handout AME 20213: Fundamentals of Measurements and Data Analysis

Laboratory Exercise 1: Pendulum Acceleration Measurement and Prediction Laboratory Handout AME 20213: Fundamentals of Measurements and Data Analysis Laboratory Exercise 1: Penduum Acceeration Measurement and Prediction Laboratory Handout AME 20213: Fundamentas of Measurements and Data Anaysis Prepared by: Danie Van Ness Date exercises to be performed:

More information

General Certificate of Education Advanced Level Examination June 2010

General Certificate of Education Advanced Level Examination June 2010 Genera Certificate of Education Advanced Leve Examination June 2010 Human Bioogy HBI6T/P10/task Unit 6T A2 Investigative Skis Assignment Task Sheet The effect of temperature on the rate of photosynthesis

More information

Ultrasonic Measurements of Kinematic Viscosity for Analize of Engine Oil Parameters

Ultrasonic Measurements of Kinematic Viscosity for Analize of Engine Oil Parameters th European Conference on Non-Destructive Testing (ECNDT 04), October 6-0, 04, Prague, Czech Repubic More Info at Open Access Database www.ndt.net/?id=6344 Utrasonic Measurements of Kinematic Viscosity

More information

Calculating Alkalinity

Calculating Alkalinity Cacuating Akainity Overview How to cacuate acid:anion ratios at varying ionic strengths Use the Mixing Water cacuation as a ph titration apparatus Understand how weak acid chemistry affects akainity Compare

More information

Modal analysis of a multi-blade system undergoing rotational motion

Modal analysis of a multi-blade system undergoing rotational motion Journa of Mechanica Science and Technoogy 3 (9) 5~58 Journa of Mechanica Science and Technoogy www.springerin.com/content/738-494x DOI.7/s6-9-43-3 Moda anaysis of a muti-bade system undergoing rotationa

More information

Chemical Kinetics Part 2

Chemical Kinetics Part 2 Integrated Rate Laws Chemica Kinetics Part 2 The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates the rate

More information

Math 124B January 31, 2012

Math 124B January 31, 2012 Math 124B January 31, 212 Viktor Grigoryan 7 Inhomogeneous boundary vaue probems Having studied the theory of Fourier series, with which we successfuy soved boundary vaue probems for the homogeneous heat

More information

Stochastic Variational Inference with Gradient Linearization

Stochastic Variational Inference with Gradient Linearization Stochastic Variationa Inference with Gradient Linearization Suppementa Materia Tobias Pötz * Anne S Wannenwetsch Stefan Roth Department of Computer Science, TU Darmstadt Preface In this suppementa materia,

More information

MA 201: Partial Differential Equations Lecture - 10

MA 201: Partial Differential Equations Lecture - 10 MA 201: Partia Differentia Equations Lecture - 10 Separation of Variabes, One dimensiona Wave Equation Initia Boundary Vaue Probem (IBVP) Reca: A physica probem governed by a PDE may contain both boundary

More information

MAGNETIC INDUCTION. MISN MAGNETIC INDUCTION by J. S. Kovacs and P. Signell Michigan State University

MAGNETIC INDUCTION. MISN MAGNETIC INDUCTION by J. S. Kovacs and P. Signell Michigan State University MAGNETIC INDUCTION V V in MISN-0-142 MAGNETIC INDUCTION by J. S. Kovacs and P. Signe Michigan State University 1. Introduction a. Overview................................................ 1 b. Magnetic

More information

A Comparison Study of the Test for Right Censored and Grouped Data

A Comparison Study of the Test for Right Censored and Grouped Data Communications for Statistica Appications and Methods 2015, Vo. 22, No. 4, 313 320 DOI: http://dx.doi.org/10.5351/csam.2015.22.4.313 Print ISSN 2287-7843 / Onine ISSN 2383-4757 A Comparison Study of the

More information

14 Separation of Variables Method

14 Separation of Variables Method 14 Separation of Variabes Method Consider, for exampe, the Dirichet probem u t = Du xx < x u(x, ) = f(x) < x < u(, t) = = u(, t) t > Let u(x, t) = T (t)φ(x); now substitute into the equation: dt

More information

Section 6: Magnetostatics

Section 6: Magnetostatics agnetic fieds in matter Section 6: agnetostatics In the previous sections we assumed that the current density J is a known function of coordinates. In the presence of matter this is not aways true. The

More information

Multivariate Rational Response Surface Approximation of Nodal Displacements of Truss Structures

Multivariate Rational Response Surface Approximation of Nodal Displacements of Truss Structures https://doi.org/10.1186/s10033-018-0219-4 Chinese Journa of Mechanica Engineering ORIGINAL ARTICLE Open Access Mutivariate Rationa Response Surface Approximation of Noda Dispacements of Truss Structures

More information

XSAT of linear CNF formulas

XSAT of linear CNF formulas XSAT of inear CN formuas Bernd R. Schuh Dr. Bernd Schuh, D-50968 Kön, Germany; bernd.schuh@netcoogne.de eywords: compexity, XSAT, exact inear formua, -reguarity, -uniformity, NPcompeteness Abstract. Open

More information

Componentwise Determination of the Interval Hull Solution for Linear Interval Parameter Systems

Componentwise Determination of the Interval Hull Solution for Linear Interval Parameter Systems Componentwise Determination of the Interva Hu Soution for Linear Interva Parameter Systems L. V. Koev Dept. of Theoretica Eectrotechnics, Facuty of Automatics, Technica University of Sofia, 1000 Sofia,

More information

Physics 111. Thursday, Dec. 9, 3-5pm and 7-9pm. Announcements. Tuesday, December 7, Stress Strain. For the rest of the semester

Physics 111. Thursday, Dec. 9, 3-5pm and 7-9pm. Announcements. Tuesday, December 7, Stress Strain. For the rest of the semester ics day, ember 7, 004 Ch 17: Kinetic Theory Stress Strain Ch 18: 1st Law of Thermodynamics nd Law of Thermodynamics or the rest of the semester Thursday,. 9, 3-5pm and 7-9pm Monday,. 13, 004 10:30 am 1:30

More information

Research on liquid sloshing performance in vane type tank under microgravity

Research on liquid sloshing performance in vane type tank under microgravity IOP Conference Series: Materias Science and Engineering PAPER OPEN ACCESS Research on iquid soshing performance in vane type tan under microgravity Reated content - Numerica simuation of fuid fow in the

More information

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES Separation of variabes is a method to sove certain PDEs which have a warped product structure. First, on R n, a inear PDE of order m is

More information

Gaussian Curvature in a p-orbital, Hydrogen-like Atoms

Gaussian Curvature in a p-orbital, Hydrogen-like Atoms Advanced Studies in Theoretica Physics Vo. 9, 015, no. 6, 81-85 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.1988/astp.015.5115 Gaussian Curvature in a p-orbita, Hydrogen-ike Atoms Sandro-Jose Berrio-Guzman

More information

8 Digifl'.11 Cth:uits and devices

8 Digifl'.11 Cth:uits and devices 8 Digif'. Cth:uits and devices 8. Introduction In anaog eectronics, votage is a continuous variabe. This is usefu because most physica quantities we encounter are continuous: sound eves, ight intensity,

More information

Kinetics of cation adsorption on charged soil mineral as strong electrostatic force presence or absence

Kinetics of cation adsorption on charged soil mineral as strong electrostatic force presence or absence J Sois Sediments () :53 6 DOI.7/s368--83-6 SOILS, SEC GLOBAL CHANGE, ENVIRON RISK ASSESS, SUSTAINABLE LAND USE RESEARCH ARTICLE Kinetics of cation adsorption on charged soi minera as strong eectrostatic

More information

Torsion and shear stresses due to shear centre eccentricity in SCIA Engineer Delft University of Technology. Marijn Drillenburg

Torsion and shear stresses due to shear centre eccentricity in SCIA Engineer Delft University of Technology. Marijn Drillenburg Torsion and shear stresses due to shear centre eccentricity in SCIA Engineer Deft University of Technoogy Marijn Drienburg October 2017 Contents 1 Introduction 2 1.1 Hand Cacuation....................................

More information

Discrete Techniques. Chapter Introduction

Discrete Techniques. Chapter Introduction Chapter 3 Discrete Techniques 3. Introduction In the previous two chapters we introduced Fourier transforms of continuous functions of the periodic and non-periodic (finite energy) type, as we as various

More information

CS229 Lecture notes. Andrew Ng

CS229 Lecture notes. Andrew Ng CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view

More information

Applied Nuclear Physics (Fall 2006) Lecture 7 (10/2/06) Overview of Cross Section Calculation

Applied Nuclear Physics (Fall 2006) Lecture 7 (10/2/06) Overview of Cross Section Calculation 22.101 Appied Nucear Physics (Fa 2006) Lecture 7 (10/2/06) Overview of Cross Section Cacuation References P. Roman, Advanced Quantum Theory (Addison-Wesey, Reading, 1965), Chap 3. A. Foderaro, The Eements

More information

17 Lecture 17: Recombination and Dark Matter Production

17 Lecture 17: Recombination and Dark Matter Production PYS 652: Astrophysics 88 17 Lecture 17: Recombination and Dark Matter Production New ideas pass through three periods: It can t be done. It probaby can be done, but it s not worth doing. I knew it was

More information

Error Floor Approximation for LDPC Codes in the AWGN Channel

Error Floor Approximation for LDPC Codes in the AWGN Channel submitted to IEEE TRANSACTIONS ON INFORMATION THEORY VERSION: JUNE 4, 2013 1 Error Foor Approximation for LDPC Codes in the AWGN Channe Brian K. Buter, Senior Member, IEEE, Pau H. Siege, Feow, IEEE arxiv:1202.2826v2

More information

Mixed Volume Computation, A Revisit

Mixed Volume Computation, A Revisit Mixed Voume Computation, A Revisit Tsung-Lin Lee, Tien-Yien Li October 31, 2007 Abstract The superiority of the dynamic enumeration of a mixed ces suggested by T Mizutani et a for the mixed voume computation

More information

A MODEL FOR ESTIMATING THE LATERAL OVERLAP PROBABILITY OF AIRCRAFT WITH RNP ALERTING CAPABILITY IN PARALLEL RNAV ROUTES

A MODEL FOR ESTIMATING THE LATERAL OVERLAP PROBABILITY OF AIRCRAFT WITH RNP ALERTING CAPABILITY IN PARALLEL RNAV ROUTES 6 TH INTERNATIONAL CONGRESS OF THE AERONAUTICAL SCIENCES A MODEL FOR ESTIMATING THE LATERAL OVERLAP PROBABILITY OF AIRCRAFT WITH RNP ALERTING CAPABILITY IN PARALLEL RNAV ROUTES Sakae NAGAOKA* *Eectronic

More information

MARKOV CHAINS AND MARKOV DECISION THEORY. Contents

MARKOV CHAINS AND MARKOV DECISION THEORY. Contents MARKOV CHAINS AND MARKOV DECISION THEORY ARINDRIMA DATTA Abstract. In this paper, we begin with a forma introduction to probabiity and expain the concept of random variabes and stochastic processes. After

More information

Sarabjeet Singh (1), Colin H. Hansen (2) and Carl Q. Howard (2)

Sarabjeet Singh (1), Colin H. Hansen (2) and Carl Q. Howard (2) Acoustics 8 Geeong, Victoria, Austraia 4 to 6 November 8 Acoustics and ustainabiity: How shoud acoustics adapt to meet future demands? A detaied tutoria for evauating in-duct net acoustic power transmission

More information

Biometrics Unit, 337 Warren Hall Cornell University, Ithaca, NY and. B. L. Raktoe

Biometrics Unit, 337 Warren Hall Cornell University, Ithaca, NY and. B. L. Raktoe NONISCMORPHIC CCMPLETE SETS OF ORTHOGONAL F-SQ.UARES, HADAMARD MATRICES, AND DECCMPOSITIONS OF A 2 4 DESIGN S. J. Schwager and w. T. Federer Biometrics Unit, 337 Warren Ha Corne University, Ithaca, NY

More information

arxiv:nlin/ v2 [nlin.cd] 30 Jan 2006

arxiv:nlin/ v2 [nlin.cd] 30 Jan 2006 expansions in semicassica theories for systems with smooth potentias and discrete symmetries Hoger Cartarius, Jörg Main, and Günter Wunner arxiv:nin/0510051v [nin.cd] 30 Jan 006 1. Institut für Theoretische

More information

Improving the Reliability of a Series-Parallel System Using Modified Weibull Distribution

Improving the Reliability of a Series-Parallel System Using Modified Weibull Distribution Internationa Mathematica Forum, Vo. 12, 217, no. 6, 257-269 HIKARI Ltd, www.m-hikari.com https://doi.org/1.12988/imf.217.611155 Improving the Reiabiity of a Series-Parae System Using Modified Weibu Distribution

More information

Quantum Mechanical Models of Vibration and Rotation of Molecules Chapter 18

Quantum Mechanical Models of Vibration and Rotation of Molecules Chapter 18 Quantum Mechanica Modes of Vibration and Rotation of Moecues Chapter 18 Moecuar Energy Transationa Vibrationa Rotationa Eectronic Moecuar Motions Vibrations of Moecues: Mode approximates moecues to atoms

More information

C. Fourier Sine Series Overview

C. Fourier Sine Series Overview 12 PHILIP D. LOEWEN C. Fourier Sine Series Overview Let some constant > be given. The symboic form of the FSS Eigenvaue probem combines an ordinary differentia equation (ODE) on the interva (, ) with a

More information

1. Measurements and error calculus

1. Measurements and error calculus EV 1 Measurements and error cacuus 11 Introduction The goa of this aboratory course is to introduce the notions of carrying out an experiment, acquiring and writing up the data, and finay anayzing the

More information

Short Circuit Detection Utilization Analysis under Uniprocessor EDF Scheduling

Short Circuit Detection Utilization Analysis under Uniprocessor EDF Scheduling Short Circuit Detection Utiization Anaysis under Uniprocessor EDF Scheduing Aaron Wicock Department of Computer Science Wayne State University Detroit, Michigan 48202 aaron.wicock@wayne.edu Abstract Accounting

More information

FRIEZE GROUPS IN R 2

FRIEZE GROUPS IN R 2 FRIEZE GROUPS IN R 2 MAXWELL STOLARSKI Abstract. Focusing on the Eucidean pane under the Pythagorean Metric, our goa is to cassify the frieze groups, discrete subgroups of the set of isometries of the

More information

LIKELIHOOD RATIO TEST FOR THE HYPER- BLOCK MATRIX SPHERICITY COVARIANCE STRUCTURE CHARACTERIZATION OF THE EXACT

LIKELIHOOD RATIO TEST FOR THE HYPER- BLOCK MATRIX SPHERICITY COVARIANCE STRUCTURE CHARACTERIZATION OF THE EXACT LIKELIHOOD RATIO TEST FOR THE HYPER- BLOCK MATRIX SPHERICITY COVARIACE STRUCTURE CHARACTERIZATIO OF THE EXACT DISTRIBUTIO AD DEVELOPMET OF EAR-EXACT DISTRIBUTIOS FOR THE TEST STATISTIC Authors: Bárbara

More information

Lecture Note 3: Stationary Iterative Methods

Lecture Note 3: Stationary Iterative Methods MATH 5330: Computationa Methods of Linear Agebra Lecture Note 3: Stationary Iterative Methods Xianyi Zeng Department of Mathematica Sciences, UTEP Stationary Iterative Methods The Gaussian eimination (or

More information

Chemical Kinetics Part 2. Chapter 16

Chemical Kinetics Part 2. Chapter 16 Chemica Kinetics Part 2 Chapter 16 Integrated Rate Laws The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates

More information

A polynomial chaos-based kalman filter approach for parameter estimation of mechanical systems

A polynomial chaos-based kalman filter approach for parameter estimation of mechanical systems University of Woongong Research Onine Facuty of Engineering - Papers (Archive) Facuty of Engineering and Information Sciences 00 A poynomia chaos-based aman fiter approach for parameter estimation of mechanica

More information

Nonlinear Analysis of Spatial Trusses

Nonlinear Analysis of Spatial Trusses Noninear Anaysis of Spatia Trusses João Barrigó October 14 Abstract The present work addresses the noninear behavior of space trusses A formuation for geometrica noninear anaysis is presented, which incudes

More information

Introduction. Figure 1 W8LC Line Array, box and horn element. Highlighted section modelled.

Introduction. Figure 1 W8LC Line Array, box and horn element. Highlighted section modelled. imuation of the acoustic fied produced by cavities using the Boundary Eement Rayeigh Integra Method () and its appication to a horn oudspeaer. tephen Kirup East Lancashire Institute, Due treet, Bacburn,

More information

IE 361 Exam 1. b) Give *&% confidence limits for the bias of this viscometer. (No need to simplify.)

IE 361 Exam 1. b) Give *&% confidence limits for the bias of this viscometer. (No need to simplify.) October 9, 00 IE 6 Exam Prof. Vardeman. The viscosity of paint is measured with a "viscometer" in units of "Krebs." First, a standard iquid of "known" viscosity *# Krebs is tested with a company viscometer

More information

University of Huddersfield Repository

University of Huddersfield Repository University of Huddersfied Repository Hardaupas, Y., Souopouos, N., Stetsyuk, V. and Tayor, A. M. K. P. Experimenta Assessment of subgrid scae Probabiity Density Function Modes for Large Eddy Simuation

More information

Discrete Applied Mathematics

Discrete Applied Mathematics Discrete Appied Mathematics 159 (2011) 812 825 Contents ists avaiabe at ScienceDirect Discrete Appied Mathematics journa homepage: www.esevier.com/ocate/dam A direct barter mode for course add/drop process

More information

TRAVEL TIME ESTIMATION FOR URBAN ROAD NETWORKS USING LOW FREQUENCY PROBE VEHICLE DATA

TRAVEL TIME ESTIMATION FOR URBAN ROAD NETWORKS USING LOW FREQUENCY PROBE VEHICLE DATA TRAVEL TIME ESTIMATIO FOR URBA ROAD ETWORKS USIG LOW FREQUECY PROBE VEHICLE DATA Erik Jeneius Corresponding author KTH Roya Institute of Technoogy Department of Transport Science Emai: erik.jeneius@abe.kth.se

More information