11. TRADITIONAL MEASUREMENT OF VOLUME FLOW RATE Volume flow rate deduced from velocity measurement data Application example

Size: px
Start display at page:

Download "11. TRADITIONAL MEASUREMENT OF VOLUME FLOW RATE Volume flow rate deduced from velocity measurement data Application example"

Transcription

1 11. TRADITIONAL MEASUREMENT OF VOLUME FLOW RATE Volume flow rate deduced from velocty measurement data Applcaton example Prncple and layouts = ' ' A V da v q = A da v = A da v A A n A v = 1 = = n A v 1 = = n v n A n 1 1 = v A

2 DISCRETISATION: For rectangular cross-sectons: k x k Log-ln method ISO

3 v = n = 1 n k = 1 v k weghtng

4 For crcular cross-sectons: 10-pont method ( r ) v = vmax 1 n r R s /D = 0.06; 0.08; 0.146; 0.6; 0.34; 0.658; 0.774; 0.854; 0.918; Accurate ntegraton: for nd order parabolod profle only!

5 Log-ln method ISO partal areas ( y) = A lg y + B y C v + s /D = 0.03; 0.135; 0.31; 0,679; 0.865; 0.968

6 General notes The nose of the probe s to be adjusted parallel to the wall of the duct p _dyn_ref Check of steadness ρ v ref 0 = p dyn _ ref _ 0 v ref _ = p ρ dyn _ ref _ v = ρ p dyn _ Correcton: v corr = v v v ref 0 = ref v p p dyn _ ref _ 0 dyn _ ref _ Obtanment of densty

7 Advantages and dsadvantages Quck scannng:

8 STANDARDS: the recent one, beng n effect, s to be used! Example: ISO 5801:007(E): Industral fans Performance testng usng standardzed arways

9

10

11

12 Calbraton of an AMCA type probe

13

14

15 K[-] 1,0 1, y = 0,9614x + 0,4445 R² = 0,9997 0,80 1 0,60 0,40 0,0 0, v[m/s] v Prandtl [m/s] v LDA [m/s] Velocty magntude wthn +/- 1 % at hgher veloctes; For ths uncertanty: drectonal nsenstvty wthn +/- 5 deg

16

17 11.. Volume flow rate measurements usng contracton elements Applcaton example Prncple and layouts Inlet orfce plate (nlet orfce meter)

18 Assumpton of deal flud: nvscd, ncompressble flow p q 0 v p + ρ ρ ρ = v = ( p0 p) = pm = d π d π v = 4 4 ρ V p m Realty: vscous, compressble flow A/ Effect of vscosty flow coeffcent α dependence on d/d_n, Re for the nlet orfce meter: α = 0.6 B/ Effect of compressblty expanson coeffcent ε dependence on d/d_n, p, p_n, κ for the nlet orfce meter: ε = 1 q d π = α ε 4 ρ V p m

19 Through-flow orfce plate (through-flow orfce meter) Standard n effect: ISO 5167 / 003

20 Standard n effect: Measurement of flud flow by means of pressure dfferental devces nserted n crcular cross-sectons runnng full ISO 5167 (003)

21

22 Geometry α, ε Installaton Examples Accuracy Examples Problems q d π = α ε 4 ρ V p m

23 Ventur meter ISO 5167

24 Inlet cone ISO (E) Re = 4q V πρdν 5 5 ( αε ) = ± 0.00 f 10 < Re < ( αε ) = ± f Re > 3 10

25 11.3. Other types of tradtonal flowmeters Example: Elbow meter

26 11.4. Comparson between volume flow rate measurement deduced from velocty data (VEL) and usng contracton elements (CON) ASPECT CON VEL 1/ Intrusveness Introduces consderable losses the operatng state may be modfed to be ncluded already n the system desgn state / Followng temporal changes n the operatonal state + Follows unsteady flow rate contnuously 3/ Requrements Strct (manufacturng, nstallaton, system s to be stopped ) + Neglgble ntrusveness (wall bores) Does not follow (surface ntegraton) ( correcton..?) + Moderate (no requrements, only recommendatons, system may run contnuously )

27 4/ Expenses Hgh (manufacturng, nstallaton, operaton: losses to be covered) 5/ Accuracy + Hgh (lmted uncertanty, guaranteed by the standard) Legally defensble! Moderate + Moderate (lmts of uncertanty are not guaranteed) Legally assalable! CON: hgh-precson, contnuous, legally defensble measurements (e.g. accountng, process control, etc.) VEL: occasonal (case study) measurements, bref estmaton (e.g. fault dagnostcs)

THE DANIEL SENIORSONIC MULTIPATH GAS FLOWMETER THE DANIEL SENIORSONIC METER AND FLOWCONDITIONERS

THE DANIEL SENIORSONIC MULTIPATH GAS FLOWMETER THE DANIEL SENIORSONIC METER AND FLOWCONDITIONERS Danel SenorSonc The Use of Flow Condtoners Page 1 THE DANIEL SENIORSONIC MULTIPATH GAS FLOWMETER THE DANIEL SENIORSONIC METER AND FLOWCONDITIONERS Danel SenorSonc The Use of Flow Condtoners Page 2 1. Introducton

More information

Uncertainty in measurements of power and energy on power networks

Uncertainty in measurements of power and energy on power networks Uncertanty n measurements of power and energy on power networks E. Manov, N. Kolev Department of Measurement and Instrumentaton, Techncal Unversty Sofa, bul. Klment Ohrdsk No8, bl., 000 Sofa, Bulgara Tel./fax:

More information

Lecture #06 Hotwire anemometry: Fundamentals and instrumentation

Lecture #06 Hotwire anemometry: Fundamentals and instrumentation AerE 344 Lecture otes Lecture #06 Hotwre anemometry: Fundamentals and nstrumentaton Dr. Hu Hu Department of Aerospace Engneerng Iowa State Unversty Ames, Iowa 500, U.S.A Thermal anemometers: Techncal Fundamentals

More information

Module 1 : The equation of continuity. Lecture 1: Equation of Continuity

Module 1 : The equation of continuity. Lecture 1: Equation of Continuity 1 Module 1 : The equaton of contnuty Lecture 1: Equaton of Contnuty 2 Advanced Heat and Mass Transfer: Modules 1. THE EQUATION OF CONTINUITY : Lectures 1-6 () () () (v) (v) Overall Mass Balance Momentum

More information

Simulation of Flow Pattern in Open Channels with Sudden Expansions

Simulation of Flow Pattern in Open Channels with Sudden Expansions Research Journal of Appled Scences, Engneerng and Technology 4(19): 3852-3857, 2012 ISSN: 2040-7467 Maxwell Scentfc Organzaton, 2012 Submtted: May 11, 2012 Accepted: June 01, 2012 Publshed: October 01,

More information

Principles of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer

Principles of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer Prncples of Food and Boprocess Engneerng (FS 31) Solutons to Example Problems on Heat Transfer 1. We start wth Fourer s law of heat conducton: Q = k A ( T/ x) Rearrangng, we get: Q/A = k ( T/ x) Here,

More information

EXAMPLES of THEORETICAL PROBLEMS in the COURSE MMV031 HEAT TRANSFER, version 2017

EXAMPLES of THEORETICAL PROBLEMS in the COURSE MMV031 HEAT TRANSFER, version 2017 EXAMPLES of THEORETICAL PROBLEMS n the COURSE MMV03 HEAT TRANSFER, verson 207 a) What s eant by sotropc ateral? b) What s eant by hoogeneous ateral? 2 Defne the theral dffusvty and gve the unts for the

More information

Introduction to Computational Fluid Dynamics

Introduction to Computational Fluid Dynamics Introducton to Computatonal Flud Dynamcs M. Zanub 1, T. Mahalakshm 2 1 (PG MATHS), Department of Mathematcs, St. Josephs College of Arts and Scence for Women-Hosur, Peryar Unversty 2 Assstance professor,

More information

is the calculated value of the dependent variable at point i. The best parameters have values that minimize the squares of the errors

is the calculated value of the dependent variable at point i. The best parameters have values that minimize the squares of the errors Multple Lnear and Polynomal Regresson wth Statstcal Analyss Gven a set of data of measured (or observed) values of a dependent varable: y versus n ndependent varables x 1, x, x n, multple lnear regresson

More information

THE CALCULATION OF THE PROFILE-LINEAR AVERAGE VELOCITY IN THE TRANSITION REGION FOR ULTRASONIC HEAT METER BASED ON THE METHOD OF LES *

THE CALCULATION OF THE PROFILE-LINEAR AVERAGE VELOCITY IN THE TRANSITION REGION FOR ULTRASONIC HEAT METER BASED ON THE METHOD OF LES * 89 11,3(1):89-94 DOI: 1.116/S11-658(1)69-3 THE CALCULATION OF THE PROFILE-LINEAR AVERAGE VELOCITY IN THE TRANSITION REGION FOR ULTRASONIC HEAT METER BASED ON THE METHOD OF LES * LIU Yong-hu, DU Guang-sheng,

More information

Turbulent Flow. Turbulent Flow

Turbulent Flow. Turbulent Flow http://www.youtube.com/watch?v=xoll2kedog&feature=related http://br.youtube.com/watch?v=7kkftgx2any http://br.youtube.com/watch?v=vqhxihpvcvu 1. Caothc fluctuatons wth a wde range of frequences and

More information

Aerodynamics. Finite Wings Lifting line theory Glauert s method

Aerodynamics. Finite Wings Lifting line theory Glauert s method α ( y) l Γ( y) r ( y) V c( y) β b 4 V Glauert s method b ( y) + r dy dγ y y dy Soluton procedure that transforms the lftng lne ntegro-dfferental equaton nto a system of algebrac equatons - Restrcted to

More information

Macroscopic Momentum Balances

Macroscopic Momentum Balances Lecture 13 F. Morrson CM3110 2013 10/22/2013 CM3110 Transport I Part I: Flud Mechancs Macroscopc Momentum Balances Professor Fath Morrson Department of Chemcal Engneerng Mchgan Technologcal Unersty 1 Macroscopc

More information

Flow equations To simulate the flow, the Navier-Stokes system that includes continuity and momentum equations is solved

Flow equations To simulate the flow, the Navier-Stokes system that includes continuity and momentum equations is solved Smulaton of nose generaton and propagaton caused by the turbulent flow around bluff bodes Zamotn Krll e-mal: krart@gmal.com, cq: 958886 Summary Accurate predctons of nose generaton and spread n turbulent

More information

Axial Turbine Analysis

Axial Turbine Analysis Axal Turbne Analyss From Euler turbomachnery (conservaton) equatons need to Nole understand change n tangental velocty to relate to forces on blades and power m W m rc e rc uc uc e Analye flow n a plane

More information

Supplementary Notes for Chapter 9 Mixture Thermodynamics

Supplementary Notes for Chapter 9 Mixture Thermodynamics Supplementary Notes for Chapter 9 Mxture Thermodynamcs Key ponts Nne major topcs of Chapter 9 are revewed below: 1. Notaton and operatonal equatons for mxtures 2. PVTN EOSs for mxtures 3. General effects

More information

Bulk Air Flow in a Duct. Hoods and Local Exhaust Ventilation. Inside a ventilation system. System Nomenclature

Bulk Air Flow in a Duct. Hoods and Local Exhaust Ventilation. Inside a ventilation system. System Nomenclature Bulk Ar Flow n a Duct Hoods and Local Exhaust Ventlaton Essental pressure and low relatonshps Ar movement always ollows the pressure gradent Flow goes rom hgher (abs) pressure to lower (abs) pressure regons

More information

Pressure Measurements Laboratory

Pressure Measurements Laboratory Lab # Pressure Measurements Laboratory Objectves:. To get hands-on experences on how to make pressure (surface pressure, statc pressure and total pressure nsde flow) measurements usng conventonal pressuremeasurng

More information

Sampling Theory MODULE V LECTURE - 17 RATIO AND PRODUCT METHODS OF ESTIMATION

Sampling Theory MODULE V LECTURE - 17 RATIO AND PRODUCT METHODS OF ESTIMATION Samplng Theory MODULE V LECTURE - 7 RATIO AND PRODUCT METHODS OF ESTIMATION DR. SHALABH DEPARTMENT OF MATHEMATICS AND STATISTICS INDIAN INSTITUTE OF TECHNOLOG KANPUR Propertes of separate rato estmator:

More information

Measurement of Pressure Distribution and Forces Acting on an Airfoil S. Ghosh, M. Muste, S. Breczinski, J. Johnson, S. Cook, and F.

Measurement of Pressure Distribution and Forces Acting on an Airfoil S. Ghosh, M. Muste, S. Breczinski, J. Johnson, S. Cook, and F. 57:00 Mechancs of Fluds and Transfer Processes Laboratory Experment #3 Measurement of Pressure Dstrbuton and Forces Actng on an Arfol S. Ghosh, M. Muste, S. Brecznsk, J. Johnson, S. Cook, and F. Stern

More information

Basic Statistical Analysis and Yield Calculations

Basic Statistical Analysis and Yield Calculations October 17, 007 Basc Statstcal Analyss and Yeld Calculatons Dr. José Ernesto Rayas Sánchez 1 Outlne Sources of desgn-performance uncertanty Desgn and development processes Desgn for manufacturablty A general

More information

Large Scale Electrostatic Precipitator

Large Scale Electrostatic Precipitator 11th Internatonal Conference on Electrostatc Precptaton 164 4BStudy and Applcaton of Numercal Calculaton Method for Gas Flow Dstrbuton of Large Scale Electrostatc Precptator DANG Xaoqng, HU Hongsheng,

More information

An Experimental and Numerical Study on Pressure Drop Coefficient of Ball Valves

An Experimental and Numerical Study on Pressure Drop Coefficient of Ball Valves A. Ozdomar, K. Turgut Gursel, Y. Pekbey, B. Celkag / Internatonal Energy Journal 8 (2007) An Expermental and Numercal Study on Pressure Drop Coeffcent of Ball Valves www.serd.at.ac.th/rerc A. Ozdamar*

More information

Numerical Analysis and Optimization on Vortex Shedder by the Linearity of Strouhal Number against Reynold Number

Numerical Analysis and Optimization on Vortex Shedder by the Linearity of Strouhal Number against Reynold Number Internatonal Journal of Materals, Mechancs and Manufacturng, Vol. 4, No. 3, August 2016 Numercal Analyss and Optmzaton on Vortex Shedder by the Lnearty of Strouhal Number aganst Reynold Number Su Myat

More information

Investigation of a New Monte Carlo Method for the Transitional Gas Flow

Investigation of a New Monte Carlo Method for the Transitional Gas Flow Investgaton of a New Monte Carlo Method for the Transtonal Gas Flow X. Luo and Chr. Day Karlsruhe Insttute of Technology(KIT) Insttute for Techncal Physcs 7602 Karlsruhe Germany Abstract. The Drect Smulaton

More information

Abstract. 1 Introduction

Abstract. 1 Introduction Numercal models for unsteady flow n ppe dvdng systems R. Klasnc," H. Knoblauch," R. Mader* ^ Department of Hydraulc Structures and Water Resources Management, Graz Unversty of Technology, A-8010, Graz,

More information

Regulation No. 117 (Tyres rolling noise and wet grip adhesion) Proposal for amendments to ECE/TRANS/WP.29/GRB/2010/3

Regulation No. 117 (Tyres rolling noise and wet grip adhesion) Proposal for amendments to ECE/TRANS/WP.29/GRB/2010/3 Transmtted by the expert from France Informal Document No. GRB-51-14 (67 th GRB, 15 17 February 2010, agenda tem 7) Regulaton No. 117 (Tyres rollng nose and wet grp adheson) Proposal for amendments to

More information

Introduction to Turbulence Modeling

Introduction to Turbulence Modeling Introducton to Turbulence Modelng Professor Ismal B. Celk West Vrgna nversty Ismal.Celk@mal.wvu.edu CFD Lab. - West Vrgna nversty I-1 Introducton to Turbulence CFD Lab. - West Vrgna nversty I-2 Introducton

More information

Computational Fluid Dynamics. Smoothed Particle Hydrodynamics. Simulations. Smoothing Kernels and Basis of SPH

Computational Fluid Dynamics. Smoothed Particle Hydrodynamics. Simulations. Smoothing Kernels and Basis of SPH Computatonal Flud Dynamcs If you want to learn a bt more of the math behnd flud dynamcs, read my prevous post about the Naver- Stokes equatons and Newtonan fluds. The equatons derved n the post are the

More information

PES 1120 Spring 2014, Spendier Lecture 6/Page 1

PES 1120 Spring 2014, Spendier Lecture 6/Page 1 PES 110 Sprng 014, Spender Lecture 6/Page 1 Lecture today: Chapter 1) Electrc feld due to charge dstrbutons -> charged rod -> charged rng We ntroduced the electrc feld, E. I defned t as an nvsble aura

More information

STUDY ON TWO PHASE FLOW IN MICRO CHANNEL BASED ON EXPERI- MENTS AND NUMERICAL EXAMINATIONS

STUDY ON TWO PHASE FLOW IN MICRO CHANNEL BASED ON EXPERI- MENTS AND NUMERICAL EXAMINATIONS Blucher Mechancal Engneerng Proceedngs May 0, vol., num. www.proceedngs.blucher.com.br/evento/0wccm STUDY ON TWO PHASE FLOW IN MICRO CHANNEL BASED ON EXPERI- MENTS AND NUMERICAL EXAMINATIONS Takahko Kurahash,

More information

Over-Temperature protection for IGBT modules

Over-Temperature protection for IGBT modules Over-Temperature protecton for IGBT modules Ke Wang 1, Yongjun Lao 2, Gaosheng Song 1, Xanku Ma 1 1 Mtsubsh Electrc & Electroncs (Shangha) Co., Ltd., Chna Room2202, Tower 3, Kerry Plaza, No.1-1 Zhongxns

More information

I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. ME 270 Fall 2012 Fnal Exam Please revew the followng statement: I certfy that I have not gven unauthorzed ad nor have I receved ad n the completon of ths exam. Sgnature: INSTRUCTIONS Begn each problem

More information

Airflow and Contaminant Simulation with CONTAM

Airflow and Contaminant Simulation with CONTAM Arflow and Contamnant Smulaton wth CONTAM George Walton, NIST CHAMPS Developers Workshop Syracuse Unversty June 19, 2006 Network Analogy Electrc Ppe, Duct & Ar Wre Ppe, Duct, or Openng Juncton Juncton

More information

An Application of Fuzzy Hypotheses Testing in Radar Detection

An Application of Fuzzy Hypotheses Testing in Radar Detection Proceedngs of the th WSES Internatonal Conference on FUZZY SYSEMS n pplcaton of Fuy Hypotheses estng n Radar Detecton.K.ELSHERIF, F.M.BBDY, G.M.BDELHMID Department of Mathematcs Mltary echncal Collage

More information

Equilibrium and stability of toroidal plasmas with flow in high-beta reduced MHD

Equilibrium and stability of toroidal plasmas with flow in high-beta reduced MHD Equlbrum and stablty of torodal plasmas wth flow n hgh-beta reduced MHD Atsush Ito and Noryosh Nakajma Natonal Insttute for Fuson Scence Equlbrum wth flow n extended MHD models of fuson plasmas Equlbrum

More information

#64. ΔS for Isothermal Mixing of Ideal Gases

#64. ΔS for Isothermal Mixing of Ideal Gases #64 Carnot Heat Engne ΔS for Isothermal Mxng of Ideal Gases ds = S dt + S T V V S = P V T T V PV = nrt, P T ds = v T = nr V dv V nr V V = nrln V V = - nrln V V ΔS ΔS ΔS for Isothermal Mxng for Ideal Gases

More information

INTERROGATING THE FLOW BEHAVIOUR IN A NOVEL MAGNETIC DESICCANT VENTILATION SYSTEM USING COMPUTATIONAL FLUID DYNAMICS (CFD)

INTERROGATING THE FLOW BEHAVIOUR IN A NOVEL MAGNETIC DESICCANT VENTILATION SYSTEM USING COMPUTATIONAL FLUID DYNAMICS (CFD) INTERROGATING THE FLOW BEHAVIOUR IN A NOVEL MAGNETIC DESICCANT VENTILATION SYSTEM USING COMPUTATIONAL FLUID DYNAMICS (CFD) Auwal Dodo*, Valente Hernandez-Perez, Je Zhu and Saffa Rffat Faculty of Engneerng,

More information

A Comparative Investigation into Aerodynamic Performances of Two Set Finned Bodies with Circular and Non Circular Cross Sections

A Comparative Investigation into Aerodynamic Performances of Two Set Finned Bodies with Circular and Non Circular Cross Sections A Comparatve Investgaton nto Aerodynamc Performances of Two Set Fnned Bodes wth Crcular and Non Crcular Cross Sectons MAHMOUD MANI and SHADI MAHJOOB Aerospace Engneerng Department Amrkabr Unversty of Technology

More information

Psychology 282 Lecture #24 Outline Regression Diagnostics: Outliers

Psychology 282 Lecture #24 Outline Regression Diagnostics: Outliers Psychology 282 Lecture #24 Outlne Regresson Dagnostcs: Outlers In an earler lecture we studed the statstcal assumptons underlyng the regresson model, ncludng the followng ponts: Formal statement of assumptons.

More information

ONE DIMENSIONAL TRIANGULAR FIN EXPERIMENT. Technical Advisor: Dr. D.C. Look, Jr. Version: 11/03/00

ONE DIMENSIONAL TRIANGULAR FIN EXPERIMENT. Technical Advisor: Dr. D.C. Look, Jr. Version: 11/03/00 ONE IMENSIONAL TRIANGULAR FIN EXPERIMENT Techncal Advsor: r..c. Look, Jr. Verson: /3/ 7. GENERAL OJECTIVES a) To understand a one-dmensonal epermental appromaton. b) To understand the art of epermental

More information

Lab 4: Two-level Random Intercept Model

Lab 4: Two-level Random Intercept Model BIO 656 Lab4 009 Lab 4: Two-level Random Intercept Model Data: Peak expratory flow rate (pefr) measured twce, usng two dfferent nstruments, for 17 subjects. (from Chapter 1 of Multlevel and Longtudnal

More information

Mathematical Preparations

Mathematical Preparations 1 Introducton Mathematcal Preparatons The theory of relatvty was developed to explan experments whch studed the propagaton of electromagnetc radaton n movng coordnate systems. Wthn expermental error the

More information

EURAMET.M.D-S2 Final Report Final report

EURAMET.M.D-S2 Final Report Final report Fnal report on ERAMET blateral comparson on volume of mass standards Project number: 1356 (ERAMET.M.D-S2) Volume of mass standards of 10g, 20 g, 200 g, 1 kg Zoltan Zelenka 1 ; Stuart Davdson 2 ; Cslla

More information

Analysis of Dynamic Cross Response between Spindles in a Dual Spindle Type Multi-Functional Turning Machine

Analysis of Dynamic Cross Response between Spindles in a Dual Spindle Type Multi-Functional Turning Machine Journal of Power and Energy Engneerng, 2013, 1, 20-24 http://dx.do.org/10.4236/jpee.2013.17004 Publshed Onlne December 2013 (http://www.scrp.org/journal/jpee) Analyss of Dynamc Cross Response between Spndles

More information

PY2101 Classical Mechanics Dr. Síle Nic Chormaic, Room 215 D Kane Bldg

PY2101 Classical Mechanics Dr. Síle Nic Chormaic, Room 215 D Kane Bldg PY2101 Classcal Mechancs Dr. Síle Nc Chormac, Room 215 D Kane Bldg s.ncchormac@ucc.e Lectures stll some ssues to resolve. Slots shared between PY2101 and PY2104. Hope to have t fnalsed by tomorrow. Mondays

More information

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient 58:080 Expermental Engneerng 1 OBJECTIVE Lab 2e Thermal System Response and Effectve Heat Transfer Coeffcent Warnng: though the experment has educatonal objectves (to learn about bolng heat transfer, etc.),

More information

AP Physics 1 & 2 Summer Assignment

AP Physics 1 & 2 Summer Assignment AP Physcs 1 & 2 Summer Assgnment AP Physcs 1 requres an exceptonal profcency n algebra, trgonometry, and geometry. It was desgned by a select group of college professors and hgh school scence teachers

More information

Phase I Monitoring of Nonlinear Profiles

Phase I Monitoring of Nonlinear Profiles Phase I Montorng of Nonlnear Profles James D. Wllams Wllam H. Woodall Jeffrey B. Brch May, 003 J.D. Wllams, Bll Woodall, Jeff Brch, Vrgna Tech 003 Qualty & Productvty Research Conference, Yorktown Heghts,

More information

A Cartesian-grid integrated-rbf method for viscoelastic flows

A Cartesian-grid integrated-rbf method for viscoelastic flows Home Search Collectons Journals About Contact us My IOPscence A Cartesan-grd ntegrated-rbf method for vscoelastc flows Ths artcle has been downloaded from IOPscence. Please scroll down to see the full

More information

FEASIBILITY STUDY OF ACTIVE MICRO-VIBRATION CONTROL SYSTEM USING PIEZOELECTRIC ACTUATORS FOR FLOOR STRUCTURE OF PRECISION MANUFACTURING FACILITIES

FEASIBILITY STUDY OF ACTIVE MICRO-VIBRATION CONTROL SYSTEM USING PIEZOELECTRIC ACTUATORS FOR FLOOR STRUCTURE OF PRECISION MANUFACTURING FACILITIES October -7, 8, Bejng, Chna FEASIBILITY STUDY OF ACTIVE MICRO-VIBRATION CONTROL SYSTEM USING PIEZOELECTRIC ACTUATORS FOR FLOOR STRUCTURE OF PRECISION MANUFACTURING FACILITIES Hrokazu Hora, Masash Yasuda,

More information

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. Please revew the followng statement: I certfy that I have not gven unauthorzed ad nor have I receved ad n the completon of ths exam. Sgnature: Instructor s Name and Secton: (Crcle Your Secton) Sectons:

More information

NUMERICAL SIMULATION OF FLOW OVER STEPPED SPILLWAYS

NUMERICAL SIMULATION OF FLOW OVER STEPPED SPILLWAYS ISSN: 345-3109 RCEE Research n Cvl and Envronmental Engneerng www.rcee.com Research n Cvl and Envronmental Engneerng 014 (04) 190-198 NUMERICAL SIMULATION OF FLOW OVER STEPPED SPILLWAYS Rasoul Daneshfaraz

More information

A Numerical Study of Heat Transfer and Fluid Flow past Single Tube

A Numerical Study of Heat Transfer and Fluid Flow past Single Tube A Numercal Study of Heat ransfer and Flud Flow past Sngle ube ZEINAB SAYED ABDEL-REHIM Mechancal Engneerng Natonal Research Center El-Bohos Street, Dokk, Gza EGYP abdelrehmz@yahoo.com Abstract: - A numercal

More information

Multiline Overview. Karl Bois, PhD Lead SI Engineer Servers & Blades. December 5th, 2016

Multiline Overview. Karl Bois, PhD Lead SI Engineer Servers & Blades. December 5th, 2016 Multlne Overvew Karl Bos, PhD Lead SI Engneer Servers & Blades December 5th, 216 Why are we here? Orgnal Equpment Manufacturers (OEMs) and Orgnal Desgn Manufacturers (ODMs) have desgns that requre that

More information

A Self-Consistent Gibbs Excess Mixing Rule for Cubic Equations of State: derivation and fugacity coefficients

A Self-Consistent Gibbs Excess Mixing Rule for Cubic Equations of State: derivation and fugacity coefficients A Self-Consstent Gbbs Excess Mxng Rule for Cubc Equatons of State: dervaton and fugacty coeffcents Paula B. Staudt, Rafael de P. Soares Departamento de Engenhara Químca, Escola de Engenhara, Unversdade

More information

A Robust Method for Calculating the Correlation Coefficient

A Robust Method for Calculating the Correlation Coefficient A Robust Method for Calculatng the Correlaton Coeffcent E.B. Nven and C. V. Deutsch Relatonshps between prmary and secondary data are frequently quantfed usng the correlaton coeffcent; however, the tradtonal

More information

(Online First)A Lattice Boltzmann Scheme for Diffusion Equation in Spherical Coordinate

(Online First)A Lattice Boltzmann Scheme for Diffusion Equation in Spherical Coordinate Internatonal Journal of Mathematcs and Systems Scence (018) Volume 1 do:10.494/jmss.v1.815 (Onlne Frst)A Lattce Boltzmann Scheme for Dffuson Equaton n Sphercal Coordnate Debabrata Datta 1 *, T K Pal 1

More information

Higher Order Wall Boundary Conditions for Incompressible Flow Simulations

Higher Order Wall Boundary Conditions for Incompressible Flow Simulations THE 5 TH ASIAN COMPUTAITIONAL FLUID DYNAMICS BUSAN KOREA OCTOBER 7-30 003 Hgher Order Wall Boundary Condtons for Incompressble Flow Smulatons Hdetosh Nshda. Department of Mechancal and System Engneerng

More information

A PAPER CLOCK MODEL FOR THE CESIUM CLOCK ENSEMBLE OF TL

A PAPER CLOCK MODEL FOR THE CESIUM CLOCK ENSEMBLE OF TL A PAPER CLOCK MODEL FOR THE CESIUM CLOCK ESEMBLE OF TL Shnn Yan Ln and Hsn Mn Peng atonal Standard Tme and Frequency Lab., TL, Chunghwa Telecom Co., Ltd. o. Lane 55, Mn-Tsu Rd. Sec. 5, YangMe, TaoYuan,

More information

LNG CARGO TRANSFER CALCULATION METHODS AND ROUNDING-OFFS

LNG CARGO TRANSFER CALCULATION METHODS AND ROUNDING-OFFS CARGO TRANSFER CALCULATION METHODS AND ROUNDING-OFFS CONTENTS 1. Method for determnng transferred energy durng cargo transfer. Calculatng the transferred energy.1 Calculatng the gross transferred energy.1.1

More information

Fiber Optic Gyroscope Dynamic North-Finder Algorithm Modeling and Analysis Based on Simulink

Fiber Optic Gyroscope Dynamic North-Finder Algorithm Modeling and Analysis Based on Simulink PHOTONIC SENSORS / Vol. 7, No. 3, 17: 83 88 Fber Optc Gyroscope Dynamc North-Fnder Algorthm Modelng and Analyss Based on Smulnk Zhengy ZHANG * and Chuntong LIU Department Two, Rocket Force Unversty of

More information

Simulation and experiment of the effect of clearance of impeller wear-rings on the performance of centrifugal pump

Simulation and experiment of the effect of clearance of impeller wear-rings on the performance of centrifugal pump IOP Conference Seres: Earth and Envronmental Scence Smulaton and experment of the effect of clearance of mpeller wear-rngs on the performance of centrfugal pump To cte ths artcle: S X Chen et al 01 IOP

More information

Flow Induced Vibration

Flow Induced Vibration Flow Induced Vbraton Project Progress Report Date: 16 th November, 2005 Submtted by Subhrajt Bhattacharya Roll no.: 02ME101 Done under the gudance of Prof. Anrvan Dasgupta Department of Mechancal Engneerng,

More information

Chapter 4. Velocity analysis

Chapter 4. Velocity analysis 1 Chapter 4 Velocty analyss Introducton The objectve of velocty analyss s to determne the sesmc veloctes of layers n the subsurface. Sesmc veloctes are used n many processng and nterpretaton stages such

More information

DETERMINATION OF UNCERTAINTY ASSOCIATED WITH QUANTIZATION ERRORS USING THE BAYESIAN APPROACH

DETERMINATION OF UNCERTAINTY ASSOCIATED WITH QUANTIZATION ERRORS USING THE BAYESIAN APPROACH Proceedngs, XVII IMEKO World Congress, June 7, 3, Dubrovn, Croata Proceedngs, XVII IMEKO World Congress, June 7, 3, Dubrovn, Croata TC XVII IMEKO World Congress Metrology n the 3rd Mllennum June 7, 3,

More information

DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM

DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM Ganj, Z. Z., et al.: Determnaton of Temperature Dstrbuton for S111 DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM by Davood Domr GANJI

More information

OF THE IN FIRE RESISTANCE TESTING

OF THE IN FIRE RESISTANCE TESTING SUMMARISED REPORT OF THE EGOLF ROUND-ROBIN NR. TC 9- IN FIRE RESISTANCE TESTING Prepared by Faben Dumont Qualty Manager Fre testng laboratory Unversty of Lège on behalf of EGOLF CONTENTS SCOPE... PART

More information

Durban Watson for Testing the Lack-of-Fit of Polynomial Regression Models without Replications

Durban Watson for Testing the Lack-of-Fit of Polynomial Regression Models without Replications Durban Watson for Testng the Lack-of-Ft of Polynomal Regresson Models wthout Replcatons Ruba A. Alyaf, Maha A. Omar, Abdullah A. Al-Shha ralyaf@ksu.edu.sa, maomar@ksu.edu.sa, aalshha@ksu.edu.sa Department

More information

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850)

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850) hermal-fluds I Chapter 18 ransent heat conducton Dr. Prmal Fernando prmal@eng.fsu.edu Ph: (850) 410-6323 1 ransent heat conducton In general, he temperature of a body vares wth tme as well as poston. In

More information

Lecture # 02: Pressure measurements and Measurement Uncertainties

Lecture # 02: Pressure measurements and Measurement Uncertainties AerE 3L & AerE343L Lecture Notes Lecture # 0: Pressure measurements and Measurement Uncertantes Dr. Hu H Hu Deartment of Aerosace Engneerng Iowa State Unversty Ames, Iowa 500, U.S.A Mechancal Pressure

More information

Lecture 5.8 Flux Vector Splitting

Lecture 5.8 Flux Vector Splitting Lecture 5.8 Flux Vector Splttng 1 Flux Vector Splttng The vector E n (5.7.) can be rewrtten as E = AU (5.8.1) (wth A as gven n (5.7.4) or (5.7.6) ) whenever, the equaton of state s of the separable form

More information

Statistics Chapter 4

Statistics Chapter 4 Statstcs Chapter 4 "There are three knds of les: les, damned les, and statstcs." Benjamn Dsrael, 1895 (Brtsh statesman) Gaussan Dstrbuton, 4-1 If a measurement s repeated many tmes a statstcal treatment

More information

CFD VALIDATION OF STRATIFIED TWO-PHASE FLOWS IN A HORIZONTAL CHANNEL

CFD VALIDATION OF STRATIFIED TWO-PHASE FLOWS IN A HORIZONTAL CHANNEL CFD VALIDATION OF STRATIFIED TWO-PHASE FLOWS IN A HORIZONTAL CHANNEL 1. Introducton Chrstophe Vallée and Thomas Höhne In dfferent scenaros of small break Loss of Coolant Accdent (SB-LOCA), stratfed twophase

More information

COMPUTATIONAL STUDY OF SUPERSONIC FLOW THROUGH A CONVERGING DIVERGING NOZZLE

COMPUTATIONAL STUDY OF SUPERSONIC FLOW THROUGH A CONVERGING DIVERGING NOZZLE Engneerng e-transacton (ISSN 183-6379) Vol. 6, No. 1, June 011, pp 37-4 Onlne at http://eum.fsktm.um.edu.my Receved 5 October, 010; Accepted 30 December, 010 COMPUTATIONAL STUDY OF SUPERSONIC FLOW THROUGH

More information

Autonomous On-orbit Calibration Approaches for Star Trackers. D. Todd Griffith

Autonomous On-orbit Calibration Approaches for Star Trackers. D. Todd Griffith Autonomous On-orbt Calbraton Approaches for Star racers D. odd Grffth Colleagues Dr. John L. Junns (Graduate Adsor) Mala Samaan Puneet Sngla eas A&M Unerst Department of Aerospace Engneerng AMU College

More information

HEAT TRANSFER THROUGH ANNULAR COMPOSITE FINS

HEAT TRANSFER THROUGH ANNULAR COMPOSITE FINS Journal of Mechancal Engneerng and Technology (JMET) Volume 4, Issue 1, Jan-June 2016, pp. 01-10, Artcle ID: JMET_04_01_001 Avalable onlne at http://www.aeme.com/jmet/ssues.asp?jtype=jmet&vtype=4&itype=1

More information

A NEW FILTERED DYNAMIC SUBGRID-SCALE MODEL FOR LARGE EDDY SIMULATION OF INDOOR AIRFLOW

A NEW FILTERED DYNAMIC SUBGRID-SCALE MODEL FOR LARGE EDDY SIMULATION OF INDOOR AIRFLOW A NEW FILTERED DYNAMIC SUBGRID-SCALE MODEL FOR LARGE EDDY SIMULATION OF INDOOR AIRFLOW We Zhang and Qngyan Chen Buldng Technology Program Massachusetts Insttute of Technology 77 Mass. Ave., Cambrdge, MA

More information

Solution of the Navier-Stokes Equations

Solution of the Navier-Stokes Equations Numercal Flud Mechancs Fall 2011 Lecture 25 REVIEW Lecture 24: Soluton of the Naver-Stokes Equatons Dscretzaton of the convectve and vscous terms Dscretzaton of the pressure term Conservaton prncples Momentum

More information

I have not received unauthorized aid in the completion of this exam.

I have not received unauthorized aid in the completion of this exam. ME 270 Sprng 2013 Fnal Examnaton Please read and respond to the followng statement, I have not receved unauthorzed ad n the completon of ths exam. Agree Dsagree Sgnature INSTRUCTIONS Begn each problem

More information

Interconnect Modeling

Interconnect Modeling Interconnect Modelng Modelng of Interconnects Interconnect R, C and computaton Interconnect models umped RC model Dstrbuted crcut models Hgher-order waveform n dstrbuted RC trees Accuracy and fdelty Prepared

More information

Multi degree of freedom measurement of machine tool movements. W. Knapp, S.Weikert Institute for Machine Tools and Manufacturing (IWF), Swiss Federal

Multi degree of freedom measurement of machine tool movements. W. Knapp, S.Weikert Institute for Machine Tools and Manufacturing (IWF), Swiss Federal Mult degree of freedom measurement of machne tool movements W. Knapp, S.Wekert Insttute for Machne Tools and Manufacturng (IWF), Swss Federal \ ^r Az. ca, we z'tz rf @ z w/: Agpr. graz. ca Abstract The

More information

Energy, Entropy, and Availability Balances Phase Equilibria. Nonideal Thermodynamic Property Models. Selecting an Appropriate Model

Energy, Entropy, and Availability Balances Phase Equilibria. Nonideal Thermodynamic Property Models. Selecting an Appropriate Model Lecture 4. Thermodynamcs [Ch. 2] Energy, Entropy, and Avalablty Balances Phase Equlbra - Fugactes and actvty coeffcents -K-values Nondeal Thermodynamc Property Models - P-v-T equaton-of-state models -

More information

Operating conditions of a mine fan under conditions of variable resistance

Operating conditions of a mine fan under conditions of variable resistance Paper No. 11 ISMS 216 Operatng condtons of a mne fan under condtons of varable resstance Zhang Ynghua a, Chen L a, b, Huang Zhan a, *, Gao Yukun a a State Key Laboratory of Hgh-Effcent Mnng and Safety

More information

Comparison of the Population Variance Estimators. of 2-Parameter Exponential Distribution Based on. Multiple Criteria Decision Making Method

Comparison of the Population Variance Estimators. of 2-Parameter Exponential Distribution Based on. Multiple Criteria Decision Making Method Appled Mathematcal Scences, Vol. 7, 0, no. 47, 07-0 HIARI Ltd, www.m-hkar.com Comparson of the Populaton Varance Estmators of -Parameter Exponental Dstrbuton Based on Multple Crtera Decson Makng Method

More information

Modeling of Dynamic Systems

Modeling of Dynamic Systems Modelng of Dynamc Systems Ref: Control System Engneerng Norman Nse : Chapters & 3 Chapter objectves : Revew the Laplace transform Learn how to fnd a mathematcal model, called a transfer functon Learn how

More information

Amplification and Relaxation of Electron Spin Polarization in Semiconductor Devices

Amplification and Relaxation of Electron Spin Polarization in Semiconductor Devices Amplfcaton and Relaxaton of Electron Spn Polarzaton n Semconductor Devces Yury V. Pershn and Vladmr Prvman Center for Quantum Devce Technology, Clarkson Unversty, Potsdam, New York 13699-570, USA Spn Relaxaton

More information

arxiv: v1 [physics.flu-dyn] 16 Sep 2013

arxiv: v1 [physics.flu-dyn] 16 Sep 2013 Three-Dmensonal Smoothed Partcle Hydrodynamcs Method for Smulatng Free Surface Flows Rzal Dw Prayogo a,b, Chrstan Fredy Naa a a Faculty of Mathematcs and Natural Scences, Insttut Teknolog Bandung, Jl.

More information

x i1 =1 for all i (the constant ).

x i1 =1 for all i (the constant ). Chapter 5 The Multple Regresson Model Consder an economc model where the dependent varable s a functon of K explanatory varables. The economc model has the form: y = f ( x,x,..., ) xk Approxmate ths by

More information

ELE B7 Power Systems Engineering. Power Flow- Introduction

ELE B7 Power Systems Engineering. Power Flow- Introduction ELE B7 Power Systems Engneerng Power Flow- Introducton Introducton to Load Flow Analyss The power flow s the backbone of the power system operaton, analyss and desgn. It s necessary for plannng, operaton,

More information

Physics 607 Exam 1. ( ) = 1, Γ( z +1) = zγ( z) x n e x2 dx = 1. e x2

Physics 607 Exam 1. ( ) = 1, Γ( z +1) = zγ( z) x n e x2 dx = 1. e x2 Physcs 607 Exam 1 Please be well-organzed, and show all sgnfcant steps clearly n all problems. You are graded on your wor, so please do not just wrte down answers wth no explanaton! Do all your wor on

More information

See Book Chapter 11 2 nd Edition (Chapter 10 1 st Edition)

See Book Chapter 11 2 nd Edition (Chapter 10 1 st Edition) Count Data Models See Book Chapter 11 2 nd Edton (Chapter 10 1 st Edton) Count data consst of non-negatve nteger values Examples: number of drver route changes per week, the number of trp departure changes

More information

Mixed Convection of the Stagnation-point Flow Towards a Stretching Vertical Permeable Sheet

Mixed Convection of the Stagnation-point Flow Towards a Stretching Vertical Permeable Sheet Malaysan Mxed Journal Convecton of Mathematcal of Stagnaton-pont Scences 1(): Flow 17 - Towards 6 (007) a Stretchng Vertcal Permeable Sheet Mxed Convecton of the Stagnaton-pont Flow Towards a Stretchng

More information

A large scale tsunami run-up simulation and numerical evaluation of fluid force during tsunami by using a particle method

A large scale tsunami run-up simulation and numerical evaluation of fluid force during tsunami by using a particle method A large scale tsunam run-up smulaton and numercal evaluaton of flud force durng tsunam by usng a partcle method *Mtsuteru Asa 1), Shoch Tanabe 2) and Masaharu Isshk 3) 1), 2) Department of Cvl Engneerng,

More information

DETERMINATION OF ERRANT RUN-OUT OF THE AXIS OF ROTATION OF OBJECTS, PERFORMING ACCURATE ROTATIONAL MOVEMENTS

DETERMINATION OF ERRANT RUN-OUT OF THE AXIS OF ROTATION OF OBJECTS, PERFORMING ACCURATE ROTATIONAL MOVEMENTS DETERMINATION OF ERRANT RUN-OUT OF THE AXIS OF ROTATION OF OBJECTS, PERFORMING ACCURATE ROTATIONAL MOVEMENTS Hrsto K. RADEV, Vassl J. BOGEV, Velzar A. VASSILEV Techncal Unversty of Sofa, Bulgara Abstract.

More information

On Higher Order Dynamics in Lattice-based Models Using Chapman-Enskog Method

On Higher Order Dynamics in Lattice-based Models Using Chapman-Enskog Method NASA/CR-1999-209346 ICASE Report No. 99-21 On Hgher Order Dynamcs n Lattce-based Models Usng Chapman-Enskog Method Yue-Hong Qan Columba Unversty, New York, New York Ye Zhou IBM, Yorktown Heghts, New York

More information

Torsion Stiffness of Thin-walled Steel Beams with Web Holes

Torsion Stiffness of Thin-walled Steel Beams with Web Holes Torson Stffness of Thn-walled Steel Beams wth Web Holes MARTN HORÁČEK, JNDŘCH MELCHER Department of Metal and Tmber Structures Brno Unversty of Technology, Faculty of Cvl Engneerng Veveří 331/95, 62 Brno

More information

The Finite Element Method

The Finite Element Method The Fnte Element Method GENERAL INTRODUCTION Read: Chapters 1 and 2 CONTENTS Engneerng and analyss Smulaton of a physcal process Examples mathematcal model development Approxmate solutons and methods of

More information

POLYMER MELT FLOW IN SUDDEN EXPANSIONS: THE EFFECTS OF VISCOUS HEATING

POLYMER MELT FLOW IN SUDDEN EXPANSIONS: THE EFFECTS OF VISCOUS HEATING POLYMER MELT FLOW IN SUDDEN EXPANSIONS: THE EFFECTS OF VISCOUS HEATING P. S. B. Zdansk a, M. Vaz. Jr. a, and A. P. C. Das a a Unversdade do Estado de Santa Catarna Departamento de Engenhara Mecânca Barro

More information

Supporting information

Supporting information Supportng nformaton S1. Sample characterzaton S1.1. Hall coeffcent and resstvty measurements Hall and resstvty measurements on sample B have been performed wth a PPMS (Physcal Property Measurement System)

More information