Proposed Nomenclature for Steady Shear Flow and Linear Viscoelastic Behavior
|
|
- Rosamond Elfreda Fowler
- 8 years ago
- Views:
Transcription
1 TRANSACTIONS OF THE SOCIETY OF RHEOLOGY 20:2, (1976) Proposed Nomenclature for Steady Shear Flow and Linear Viscoelastic Behavior C. L. SIEGLAFF, Diamond Shamrock Co., inesville, Ohio Eighteen years ago Leaderman [Trans. Sot. Rheol., I, 213 (1957)] published a nomenclature for linear viscoelasticity. Since that time the science of rheology has matured and its use in other disciplines has grown. In order to facilitate communication between these diverse disciplines, a systematic organization of names and symbols is very desirable. In 1970, F. R. Eirich, as vicepresident of the Society of Rheology, formed an ad hoc committee to review the status of rheological nomenclature. This committee first convened at the Princeton Annual Society meeting. The committee then agreed that a uniform system of nomenclature for material properties, such as moduli, viscosities, etc., was needed. It was also agreed that the existing prevalent usages should serve as guide lines for proposed nomenclature. Subsequent to the original meeting, several approaches to a uniform system of nomenclature were explored. The results were distilled down to the nomenclature list proposed in the Rheology Bulletin, Vol. 43. Several corrections and comments have been included in the final nomenclature published in this report. A major addition is the use of SI units, as well as the cgs system. The committee recommends that the Society of Rheology members adopt this nomenclature in their communications to the Society. The committee expressly recommends standardization of those symbols and notations representing material constants, material functions, and notations for the directions of shearing flow. The present committee did not consider it necessary or advisable to develop a dictionary of (phenomenological) behavior. A dictionary of this type by M. Reiner and G. W. Scott Blair is currently 1976 by The Society of Rheology, Inc. Published by John Wiley & Sons, Inc.
2 Nomenclature for Simple Steady Shear Flow vz = j(y) or VI = f(n) SI System cgs System Name Definition Name Symbol Dimensions Name geometric direction of 5ow direction of velocity change neutral direction shear stress in simple steady shear 5ow m1.kg.s dyne cm shear rate dv./d9 s1 s1 s1 s1 viscosity u/t second as ml. kg. sl or (N. s/m*) Poise dyne*s.cm first normal stress function m.&.s2 or (N/m ) dyne cm* second normal stress function S?Z 0a.d SC81 m1. kg. S2 or W/m) dyne cm*
3 first normal stress coefficient N+i=.9 m1. kg dyne. 9 + cm4 second normal stress coefficient s m1. kg dyne. 5%. cm2 70 limiting viscosity at zero shear rate iii (r/q) second s m1. kg. s1 Poise 40 dyne. s. cm4 limiting viscosity at infinite shear rate lim (u/q) second s,1. kg. s1 Poise +a, dyne.s.cm* la viscosity of solvent or continuous medium second s,i. kg. s1 Poise dyne.s*cm* 9a relative viscosity 9.P specific viscosity hl intrinsic viscosity ma. kgr gr.cma or specified units of concentration
4 Nomenclature for Small Amplitude Oscillatory Motion Unite SI System cgs System Symbol Name Name Symbol Dimensions Name w t time T relaxation time or retardation time 1)* complex dynamic shear viscosity I? I! B B' B" B(t) D* D' D" L'(t) angular frequency dynamic viscosit.y outofphase component of n* bulk dynamic complex compliance bulk storage compliance bulk loss compliance bulk creep compliince tensile dynamic complex compliance tensile storage compliance tensile loss compliance tensile creep compliance hertz or radians Hz s1 s1 per second rad/s second s second s second S second S second ss,i. kg. s2 poise dyne. s. cm2 or N.s/m* i m.kgl.s2 cm dynei or (m /N) i mkgr.s* or (m*/n) cm* dynei
5 E E E(t) G* G G G(t) J* J J JO) K tensile dynamic complex modulus tensile storage modulus tensile loss modulus tensile relaxation modulus complex dynamic shear modulus shear storage modulus shear loss modulus shear relaxation modulus complex dynamic shear compliance shear storage compliance shear loss compliance shear creep compliince bulk dynamic complex modulus K bulk storage modulus K bulk loss modulus K(t) bulk relaxation modulus Ir complex dynamic Poisson s ratio * inphase component of p* d outofphase component of p* rnr.kgsor (N/m ) dyne cm2 m *kgs* dyne cm* % rn*kgr.sz cm dyner isi or (mz/n) E 3 zz mrkg.0 dyne cm z g 2
6 Nomenclature for Small Deformation Linear Elasticity Unit.3 SI System cgs System Symbol Name Name Symbol Dimensions Name Simple Shear G J K B E D P shear modulus; modulus of rigidity shear compliance bulk modulus bulk compliance Young s modulus (tensile modulus) tensile compliance Poisson s ratio rni.kgsf dyne cm+ i makgi9 cm* dyner Bulk (Isotropic) Compression or (m*/n),i. kg. si dyne cm* 3 or (N/mx) i mkgid cm dynei Tensile Extension or (m*/n) ml.kgs* dyne cmor (N/m*) * mekgis* cm dyner or (m /N) z 5 j:
7 PROPOSED NOMENCLATURE 317 available (IZheoEogy, Vol. 4, Academic Press, New York, 1967). Also, the systemization of nonlinear nomenclature was considered to be premature. A future committee should be organized to consider this vital area of rheology. The chairman wished to thank the committee members: R. B. Bird F. R. Eirich R. R. Myers R. A. Dickie H. Markovitz for their diligent efforts in compiling the nomenclature list. Also, the committee wishes to express its gratitude to the Society members who made many thoughtful inputs to this endeavor.
1. Fluids Mechanics and Fluid Properties. 1.1 Objectives of this section. 1.2 Fluids
1. Fluids Mechanics and Fluid Properties What is fluid mechanics? As its name suggests it is the branch of applied mechanics concerned with the statics and dynamics of fluids - both liquids and gases.
More informationRheological Properties of Topical Formulations
Rheological Properties of Topical Formulations Hemi Nae, PhD Hydan Technologies, Inc. Key Words Complex Modulus, Creep/Recovery, Dilatant Flow, Dynamic Viscosity, Flow, Flow Curve, Flow Models, Frequency
More information3.3. Rheological Behavior of Vinyl Ester Resins
3.3. Rheological Behavior of Vinyl Ester Resins 3.3.1. Introduction Rheology is the study of the deformation and flow of matter 1. There has been significant appreciation of the importance of the rheological
More informationManufacturing Equipment Modeling
QUESTION 1 For a linear axis actuated by an electric motor complete the following: a. Derive a differential equation for the linear axis velocity assuming viscous friction acts on the DC motor shaft, leadscrew,
More informationXI / PHYSICS FLUIDS IN MOTION 11/PA
Viscosity It is the property of a liquid due to which it flows in the form of layers and each layer opposes the motion of its adjacent layer. Cause of viscosity Consider two neighboring liquid layers A
More informationDynamic wave dispersion and loss properties of conventional and negative Poisson's ratio polymeric cellular materials 1 INTRODUCTION
Chen and Lakes 1 Dynamic wave dispersion and loss properties of conventional and negative Poisson's ratio polymeric cellular materials by C. P. Chen and R. S. Lakes Adapted from Cellular Polymers, 8, 343-369,
More informationPhysics 41 HW Set 1 Chapter 15
Physics 4 HW Set Chapter 5 Serway 8 th OC:, 4, 7 CQ: 4, 8 P: 4, 5, 8, 8, 0, 9,, 4, 9, 4, 5, 5 Discussion Problems:, 57, 59, 67, 74 OC CQ P: 4, 5, 8, 8, 0, 9,, 4, 9, 4, 5, 5 Discussion Problems:, 57, 59,
More informationSimulation of 9C46-1125-A_DRUM-WHEEL BRAKE - 410 MM DIA
Simulation of 9C46-1125-A_DRUM-WHEEL BRAKE - 410 MM DIA Date: 21 Mayıs 2012 Pazartesi Designer: Solidworks Study name: Study 1 Analysis type: Frequency Description No Data Table of Contents Description...
More informationCBE 6333, R. Levicky 1 Review of Fluid Mechanics Terminology
CBE 6333, R. Levicky 1 Review of Fluid Mechanics Terminology The Continuum Hypothesis: We will regard macroscopic behavior of fluids as if the fluids are perfectly continuous in structure. In reality,
More informationOUTCOME 3 TUTORIAL 5 DIMENSIONAL ANALYSIS
Unit 41: Fluid Mechanics Unit code: T/601/1445 QCF Level: 4 Credit value: 15 OUTCOME 3 TUTORIAL 5 DIMENSIONAL ANALYSIS 3 Be able to determine the behavioural characteristics and parameters of real fluid
More informationChapter Outline. Mechanical Properties of Metals How do metals respond to external loads?
Mechanical Properties of Metals How do metals respond to external loads? Stress and Strain Tension Compression Shear Torsion Elastic deformation Plastic Deformation Yield Strength Tensile Strength Ductility
More informationOverview of Topics. Stress-Strain Behavior in Concrete. Elastic Behavior. Non-Linear Inelastic Behavior. Stress Distribution.
Stress-Strain Behavior in Concrete Overview of Topics EARLY AGE CONCRETE Plastic shrinkage shrinkage strain associated with early moisture loss Thermal shrinkage shrinkage strain associated with cooling
More informationElastic Properties of Polymer Melts Filled with Nanoparticles
Elastic Properties of Polymer Melts Filled with Nanoparticles Helmut Münstedt and Christian Triebel Citation: AIP Conf. Proc. 1375, 21 (211); doi: 1.163/1.364479 View online: http://dx.doi.org/1.163/1.364479
More informationMechanical Properties of Metals Mechanical Properties refers to the behavior of material when external forces are applied
Mechanical Properties of Metals Mechanical Properties refers to the behavior of material when external forces are applied Stress and strain fracture or engineering point of view: allows to predict the
More informationPolymer Melt Rheology. Introduction to Viscoelastic Behavior. Time-Temperature Equivalence
Topics to be Covered Polymer Melt Rheology Introduction to Viscoelastic Behavior Time-Temperature Equivalence Chapter 11 in CD (Polymer Science and Engineering) Polymer Melt Rheology δ τ xy Newton s Law
More informationPhysics Notes Class 11 CHAPTER 2 UNITS AND MEASUREMENTS
1 P a g e Physics Notes Class 11 CHAPTER 2 UNITS AND MEASUREMENTS The comparison of any physical quantity with its standard unit is called measurement. Physical Quantities All the quantities in terms of
More informationRheology of polymer systems/ Reologia dos sistemas poliméricos
Rheology of polymer systems/ Reologia dos sistemas poliméricos 1. Viscosity/Viscosidade Jorge Morgado, IST Polymers Molecular materials in nature COMPLEX behaviour Viscosity of concentrated solu1ons and
More informationFluids and Solids: Fundamentals
Fluids and Solids: Fundamentals We normally recognize three states of matter: solid; liquid and gas. However, liquid and gas are both fluids: in contrast to solids they lack the ability to resist deformation.
More informationEFFECTS ON NUMBER OF CABLES FOR MODAL ANALYSIS OF CABLE-STAYED BRIDGES
EFFECTS ON NUMBER OF CABLES FOR MODAL ANALYSIS OF CABLE-STAYED BRIDGES Yang-Cheng Wang Associate Professor & Chairman Department of Civil Engineering Chinese Military Academy Feng-Shan 83000,Taiwan Republic
More informationL r = L m /L p. L r = L p /L m
NOTE: In the set of lectures 19/20 I defined the length ratio as L r = L m /L p The textbook by Finnermore & Franzini defines it as L r = L p /L m To avoid confusion let's keep the textbook definition,
More informationPhysics 231 Lecture 15
Physics 31 ecture 15 Main points of today s lecture: Simple harmonic motion Mass and Spring Pendulum Circular motion T 1/f; f 1/ T; ω πf for mass and spring ω x Acos( ωt) v ωasin( ωt) x ax ω Acos( ωt)
More informationIntroduction to Mechanical Behavior of Biological Materials
Introduction to Mechanical Behavior of Biological Materials Ozkaya and Nordin Chapter 7, pages 127-151 Chapter 8, pages 173-194 Outline Modes of loading Internal forces and moments Stiffness of a structure
More informationNotes on Polymer Rheology Outline
1 Why is rheology important? Examples of its importance Summary of important variables Description of the flow equations Flow regimes - laminar vs. turbulent - Reynolds number - definition of viscosity
More informationMechanical Properties - Stresses & Strains
Mechanical Properties - Stresses & Strains Types of Deformation : Elasic Plastic Anelastic Elastic deformation is defined as instantaneous recoverable deformation Hooke's law : For tensile loading, σ =
More informationCh 2 Properties of Fluids - II. Ideal Fluids. Real Fluids. Viscosity (1) Viscosity (3) Viscosity (2)
Ch 2 Properties of Fluids - II Ideal Fluids 1 Prepared for CEE 3500 CEE Fluid Mechanics by Gilberto E. Urroz, August 2005 2 Ideal fluid: a fluid with no friction Also referred to as an inviscid (zero viscosity)
More informationViscoelasticity of Polymer Fluids.
Viscoelasticity of Polymer Fluids. Main Properties of Polymer Fluids. Entangled polymer fluids are polymer melts and concentrated or semidilute (above the concentration c) solutions. In these systems polymer
More informationPractice Test SHM with Answers
Practice Test SHM with Answers MPC 1) If we double the frequency of a system undergoing simple harmonic motion, which of the following statements about that system are true? (There could be more than one
More informationVISCOSITY OF A LIQUID. To determine the viscosity of a lubricating oil. Time permitting, the temperature variation of viscosity can also be studied.
VISCOSITY OF A LIQUID August 19, 004 OBJECTIVE: EQUIPMENT: To determine the viscosity of a lubricating oil. Time permitting, the temperature variation of viscosity can also be studied. Viscosity apparatus
More informationwww.mathsbox.org.uk Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx Acceleration Velocity (v) Displacement x
Mechanics 2 : Revision Notes 1. Kinematics and variable acceleration Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx differentiate a = dv = d2 x dt dt dt 2 Acceleration Velocity
More informationSolid Mechanics. Stress. What you ll learn: Motivation
Solid Mechanics Stress What you ll learn: What is stress? Why stress is important? What are normal and shear stresses? What is strain? Hooke s law (relationship between stress and strain) Stress strain
More informationLong term performance of polymers
1.0 Introduction Long term performance of polymers Polymer materials exhibit time dependent behavior. The stress and strain induced when a load is applied are a function of time. In the most general form
More informationTorsion Tests. Subjects of interest
Chapter 10 Torsion Tests Subjects of interest Introduction/Objectives Mechanical properties in torsion Torsional stresses for large plastic strains Type of torsion failures Torsion test vs.tension test
More informationFor Water to Move a driving force is needed
RECALL FIRST CLASS: Q K Head Difference Area Distance between Heads Q 0.01 cm 0.19 m 6cm 0.75cm 1 liter 86400sec 1.17 liter ~ 1 liter sec 0.63 m 1000cm 3 day day day constant head 0.4 m 0.1 m FINE SAND
More informationSpring Simple Harmonic Oscillator. Spring constant. Potential Energy stored in a Spring. Understanding oscillations. Understanding oscillations
Spring Simple Harmonic Oscillator Simple Harmonic Oscillations and Resonance We have an object attached to a spring. The object is on a horizontal frictionless surface. We move the object so the spring
More informationFluid Mechanics: Static s Kinematics Dynamics Fluid
Fluid Mechanics: Fluid mechanics may be defined as that branch of engineering science that deals with the behavior of fluid under the condition of rest and motion Fluid mechanics may be divided into three
More informationUnderstanding Rheology
Understanding Rheology Ross Clark Distinguished Research Fellow San Diego R&D Page 1 Background CP Kelco makes carbohydrate based water soluble polymers Fermentation Xanthan Gellan Plant derived Pectin
More informationSIZE OF A MOLECULE FROM A VISCOSITY MEASUREMENT
Experiment 8, page 1 Version of April 25, 216 Experiment 446.8 SIZE OF A MOLECULE FROM A VISCOSITY MEASUREMENT Theory Viscous Flow. Fluids attempt to minimize flow gradients by exerting a frictional force,
More informationHW Set VI page 1 of 9 PHYSICS 1401 (1) homework solutions
HW Set VI page 1 of 9 10-30 A 10 g bullet moving directly upward at 1000 m/s strikes and passes through the center of mass of a 5.0 kg block initially at rest (Fig. 10-33 ). The bullet emerges from the
More informationphysics 1/12/2016 Chapter 20 Lecture Chapter 20 Traveling Waves
Chapter 20 Lecture physics FOR SCIENTISTS AND ENGINEERS a strategic approach THIRD EDITION randall d. knight Chapter 20 Traveling Waves Chapter Goal: To learn the basic properties of traveling waves. Slide
More informationSimple Harmonic Motion(SHM) Period and Frequency. Period and Frequency. Cosines and Sines
Simple Harmonic Motion(SHM) Vibration (oscillation) Equilibrium position position of the natural length of a spring Amplitude maximum displacement Period and Frequency Period (T) Time for one complete
More informationTRAVELING WAVE EFFECTS ON NONLINEAR SEISMIC BEHAVIOR OF CONCRETE GRAVITY DAMS
TRAVELING WAVE EFFECTS ON NONLINEAR SEISMIC BEHAVIOR OF CONCRETE GRAVITY DAMS H. Mirzabozorg 1, M. R. Kianoush 2 and M. Varmazyari 3 1,3 Assistant Professor and Graduate Student respectively, Department
More informationOscillations. Vern Lindberg. June 10, 2010
Oscillations Vern Lindberg June 10, 2010 You have discussed oscillations in Vibs and Waves: we will therefore touch lightly on Chapter 3, mainly trying to refresh your memory and extend the concepts. 1
More information1 The basic equations of fluid dynamics
1 The basic equations of fluid dynamics The main task in fluid dynamics is to find the velocity field describing the flow in a given domain. To do this, one uses the basic equations of fluid flow, which
More informationCE 204 FLUID MECHANICS
CE 204 FLUID MECHANICS Onur AKAY Assistant Professor Okan University Department of Civil Engineering Akfırat Campus 34959 Tuzla-Istanbul/TURKEY Phone: +90-216-677-1630 ext.1974 Fax: +90-216-677-1486 E-mail:
More informationIntroduction to Data Analysis. Q-Sense Basic Training, April 4-5, 2006
Introduction to Data Analysis Q-Sense Basic Training, April 4-5, 2006 Outline Different types of data evaluation Functions in QTools Introduction to viscoelastic modeling Analysis Methods 1) Qualitative
More informationTesting and appraisal of Lucobit polymer effect as an additive on asphalt mixture performance
Abstract Testing and appraisal of polymer effect as an additive on asphalt mixture performance Hamid Sabbagh mollahosseini*,golazin Yadollahi**, Ershad Amoosoltani*** *, ***Executive of Engineering and
More informationAsphalt Institute Technical Bulletin. Laboratory Mixing and Compaction Temperatures
ASPHALT INSTITUTE EXECUTIVE OFFICES AND RESEARCH CENTER Research Park Drive P.O. Box 14052 Lexington, KY 40512-4052 USA Telephone 859-288-4960 FAX No. 859-288-4999 Asphalt Institute Technical Bulletin
More informationSolution for Homework #1
Solution for Homework #1 Chapter 2: Multiple Choice Questions (2.5, 2.6, 2.8, 2.11) 2.5 Which of the following bond types are classified as primary bonds (more than one)? (a) covalent bonding, (b) hydrogen
More information4.3 Results... 27 4.3.1 Drained Conditions... 27 4.3.2 Undrained Conditions... 28 4.4 References... 30 4.5 Data Files... 30 5 Undrained Analysis of
Table of Contents 1 One Dimensional Compression of a Finite Layer... 3 1.1 Problem Description... 3 1.1.1 Uniform Mesh... 3 1.1.2 Graded Mesh... 5 1.2 Analytical Solution... 6 1.3 Results... 6 1.3.1 Uniform
More informationENS 07 Paris, France, 3-4 December 2007
ENS 7 Paris, France, 3-4 December 7 FRICTION DRIVE SIMULATION OF A SURFACE ACOUSTIC WAVE MOTOR BY NANO VIBRATION Minoru Kuribayashi Kurosawa, Takashi Shigematsu Tokyou Institute of Technology, Yokohama
More information18 Q0 a speed of 45.0 m/s away from a moving car. If the car is 8 Q0 moving towards the ambulance with a speed of 15.0 m/s, what Q0 frequency does a
First Major T-042 1 A transverse sinusoidal wave is traveling on a string with a 17 speed of 300 m/s. If the wave has a frequency of 100 Hz, what 9 is the phase difference between two particles on the
More informationA Beginner s Guide DMA
FREQUENTLY ASKED QUESTIONS Dynamic Mechanical Analysis (DMA) A Beginner s Guide This booklet provides an introduction to the concepts of Dynamic Mechanical Analysis (DMA). It is written for the materials
More informationStress Relaxation Study of Paper and Plastic Film based Packaging Material
Master's Degree Thesis ISRN: BTH-AMT-EX--2009/D-02--SE Stress Relaxation Study of Paper and Plastic Film based Packaging Material Rajdip Roy Lu Qi Department of Mechanical Engineering Blekinge Institute
More informationMOLECULAR DYNAMICS INVESTIGATION OF DEFORMATION RESPONSE OF THIN-FILM METALLIC NANOSTRUCTURES UNDER HEATING
NANOSYSTEMS: PHYSICS, CHEMISTRY, MATHEMATICS, 2011, 2 (2), P. 76 83 UDC 538.97 MOLECULAR DYNAMICS INVESTIGATION OF DEFORMATION RESPONSE OF THIN-FILM METALLIC NANOSTRUCTURES UNDER HEATING I. S. Konovalenko
More informationPeriodical meeting CO2Monitor. Leakage characterization at the Sleipner injection site
Periodical meeting CO2Monitor Leakage characterization at the Sleipner injection site Stefano Picotti, Davide Gei, Jose Carcione Objective Modelling of the Sleipner overburden to study the sensitivity
More informationMathematical Model of Blood Flow in Carotid Bifurcation. Phd student: Eng. Emanuel Muraca. 16/10/09 Milan
Presented at the COMSOL Conference 2009 Milan Mathematical Model of Blood Flow in Carotid Bifurcation Phd student: Eng. Emanuel Muraca 16/10/09 Milan 1 Research s s goal The goal of this research is to
More informationSOLUTIONS TO CONCEPTS CHAPTER 15
SOLUTIONS TO CONCEPTS CHAPTER 15 1. v = 40 cm/sec As velocity of a wave is constant location of maximum after 5 sec = 40 5 = 00 cm along negative x-axis. [(x / a) (t / T)]. Given y = Ae a) [A] = [M 0 L
More informationThermal Analysis Excellence
Thermal Analysis Excellence DMA/SDTA861 e STAR e System Innovative Technology Versatile Modularity Swiss Quality Dynamic Mechanical Analysis Sets New Standards DMA/SDTA861 e Precise Measurement Technology
More informationPhysics 9e/Cutnell. correlated to the. College Board AP Physics 1 Course Objectives
Physics 9e/Cutnell correlated to the College Board AP Physics 1 Course Objectives Big Idea 1: Objects and systems have properties such as mass and charge. Systems may have internal structure. Enduring
More informationSIESMIC SLOSHING IN CYLINDRICAL TANKS WITH FLEXIBLE BAFFLES
SIESMIC SLOSHING IN CYLINDRICAL TANKS WITH FLEXIBLE BAFFLES Kayahan AKGUL 1, Yasin M. FAHJAN 2, Zuhal OZDEMIR 3 and Mhamed SOULI 4 ABSTRACT Sloshing has been one of the major concerns for engineers in
More informationProperties of Fluids
CHAPTER Properties of Fluids 1 1.1 INTRODUCTION A fluid can be defined as a substance which deforms or yields continuously when shear stress is applied to it, no matter how small it is. Fluids can be subdivided
More informationAP1 Oscillations. 1. Which of the following statements about a spring-block oscillator in simple harmonic motion about its equilibrium point is false?
1. Which of the following statements about a spring-block oscillator in simple harmonic motion about its equilibrium point is false? (A) The displacement is directly related to the acceleration. (B) The
More information226 Chapter 15: OSCILLATIONS
Chapter 15: OSCILLATIONS 1. In simple harmonic motion, the restoring force must be proportional to the: A. amplitude B. frequency C. velocity D. displacement E. displacement squared 2. An oscillatory motion
More informationChapter 10 Rotational Motion. Copyright 2009 Pearson Education, Inc.
Chapter 10 Rotational Motion Angular Quantities Units of Chapter 10 Vector Nature of Angular Quantities Constant Angular Acceleration Torque Rotational Dynamics; Torque and Rotational Inertia Solving Problems
More informationLecture 9: Annealing and Tempering
IMI-NFG Course on Processing in Glass Spring 2015 (available online www.lehigh.edu/imi) Lecture 9: Annealing and Tempering Mathieu Hubert, PhD CelSian Glass & Solar Eindhoven, The Netherlands mathieu.hubert@celsian.nl
More informationBasic Principles in Microfluidics
Basic Principles in Microfluidics 1 Newton s Second Law for Fluidics Newton s 2 nd Law (F= ma) : Time rate of change of momentum of a system equal to net force acting on system!f = dp dt Sum of forces
More informationDetermination of source parameters from seismic spectra
Topic Determination of source parameters from seismic spectra Authors Michael Baumbach, and Peter Bormann (formerly GeoForschungsZentrum Potsdam, Telegrafenberg, D-14473 Potsdam, Germany); E-mail: pb65@gmx.net
More informationGENERAL PROPERTIES //////////////////////////////////////////////////////
ALLOY 625 DATA SHEET //// Alloy 625 (UNS designation N06625) is a nickel-chromium-molybdenum alloy possessing excellent resistance to oxidation and corrosion over a broad range of corrosive conditions,
More informationStructural Integrity Analysis
Structural Integrity Analysis 1. STRESS CONCENTRATION Igor Kokcharov 1.1 STRESSES AND CONCENTRATORS 1.1.1 Stress An applied external force F causes inner forces in the carrying structure. Inner forces
More information7.2.4 Seismic velocity, attenuation and rock properties
7.2.4 Seismic velocity, attenuation and rock properties Rock properties that affect seismic velocity Porosity Lithification Pressure Fluid saturation Velocity in unconsolidated near surface soils (the
More informationA Simulation Study on Joint Velocities and End Effector Deflection of a Flexible Two Degree Freedom Composite Robotic Arm
International Journal of Advanced Mechatronics and Robotics (IJAMR) Vol. 3, No. 1, January-June 011; pp. 9-0; International Science Press, ISSN: 0975-6108 A Simulation Study on Joint Velocities and End
More informationApplications of Second-Order Differential Equations
Applications of Second-Order Differential Equations Second-order linear differential equations have a variety of applications in science and engineering. In this section we explore two of them: the vibration
More information11. Rotation Translational Motion: Rotational Motion:
11. Rotation Translational Motion: Motion of the center of mass of an object from one position to another. All the motion discussed so far belongs to this category, except uniform circular motion. Rotational
More informationCorning HPFS 7979, 7980, 8655 Fused Silica. Optical Materials Product Information Specialty Materials Division
Corning HPFS 7979, 7980, 8655 Fused Silica Optical Materials Product Information Specialty Materials Division HPFS 7979, 7980 and 8655 Fused Silica HPFS Fused Silica glasses are known throughout the industry
More informationStructural Dynamics, Dynamic Force and Dynamic System
Structural Dynamics, Dynamic Force and Dynamic System Structural Dynamics Conventional structural analysis is based on the concept of statics, which can be derived from Newton s 1 st law of motion. This
More informationCHAPTER 2: LIQUID VISCOSITY MEASUREMENT
CHAPTER 2: LIQUID VISCOSITY MEASUREMENT Objective Calculate viscosity (dynamic or absolute, and kinematic) and determine how this property varies with changes in temperature for a constant-composition
More informationVARIATIONS IN ASPHALT ADHESION AS A FUNCTION OF AGGREGATE TYPE
VARIATIONS IN ASPHALT ADHESION AS A FUNCTION OF AGGREGATE TYPE Shin-Che Huang, Raymond E. Robertson, and Troy A. Pauli 2005 Pavement Performance Prediction Symposium Adhesion and Cohesion in Asphalt Pavement
More information4 Microscopic dynamics
4 Microscopic dynamics In this section we will look at the first model that people came up with when they started to model polymers from the microscopic level. It s called the Oldroyd B model. We will
More informationAPPLIED FLUID MECHANICS. TUTORIAL No.6 DIMENSIONAL ANALYSIS. When you have completed this tutorial you should be able to do the following.
APPLIED FLUID MECHANICS TUTORIAL No.6 DIMENSIONAL ANALYSIS When you have completed this tutorial you should be able to do the following. Explain the basic system of dimensions. Find the relationship between
More informationOperating Instructions, version 1.20. Manual No. M/94-310-F699
BROOKFIELD CAP VISCOMETERS MODELS CAP 1000 and CAP 2000 Operating Instructions, version 1.20 Manual No. M/94-310-F699 SPECIALISTS IN THE MEASUREMENT AND CONTROL OF VISCOSITY BROOKFIELD ENGINEERING LABORATORIES,
More informationLOW TEMPERATURE TESTING OF ELASTOMERS
LOW TEMPERATURE TESTING OF ELASTOMERS Presented at the Spring Technical Meeting of the New York Rubber Group Thursday, March 25, 1999 By, Andrew C. Farinella and Daniel L. Hertz, Jr. LOW TEMPERATURE DATA
More informationPhasors. Phasors. by Prof. Dr. Osman SEVAİOĞLU Electrical and Electronics Engineering Department. ^ V cos (wt + θ) ^ V sin (wt + θ)
V cos (wt θ) V sin (wt θ) by Prof. Dr. Osman SEVAİOĞLU Electrical and Electronics Engineering Department EE 209 Fundamentals of Electrical and Electronics Engineering, Prof. Dr. O. SEVAİOĞLU, Page 1 Vector
More informationDEVELOPMENT AND APPLICATIONS OF TUNED/HYBRID MASS DAMPERS USING MULTI-STAGE RUBBER BEARINGS FOR VIBRATION CONTROL OF STRUCTURES
13 th World Conference on Earthquake Engineering Vancouver, B.C., Canada August 1-6, 2004 Paper No. 2243 DEVELOPMENT AND APPLICATIONS OF TUNED/HYBRID MASS DAMPERS USING MULTI-STAGE RUBBER BEARINGS FOR
More informationω h (t) = Ae t/τ. (3) + 1 = 0 τ =.
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Mechanical Engineering 2.004 Dynamics and Control II Fall 2007 Lecture 2 Solving the Equation of Motion Goals for today Modeling of the 2.004 La s rotational
More informationSoil Properties soil texture and classes heat capacity, conductivity and thermal diffusivity moisture conductivity
Lecture 33 Lecture on Soil Physics, part 1 Soil Properties soil texture and classes heat capacity, conductivity and thermal diffusivity moisture conductivity porosity and diffusion i Theory, Heat Transfer
More informationEDEXCEL NATIONAL CERTIFICATE/DIPLOMA MECHANICAL PRINCIPLES OUTCOME 2 ENGINEERING COMPONENTS TUTORIAL 1 STRUCTURAL MEMBERS
ENGINEERING COMPONENTS EDEXCEL NATIONAL CERTIFICATE/DIPLOMA MECHANICAL PRINCIPLES OUTCOME ENGINEERING COMPONENTS TUTORIAL 1 STRUCTURAL MEMBERS Structural members: struts and ties; direct stress and strain,
More informationMagnetic / Gravity Loading Analysis
Magnetic / Gravity Loading Analysis 2 ELEMENTS JUL 7 2006 ELEMENTS MAT NUM 2:5:0 MAT NUM POR Design JUL 7 2006 2:5:0 L2 L L q Assumed Location of Gap Encoder(s) ELEMENTS MAT NUM JUL 7 2006 2:5:0 Materials:
More informationPhysics Notes Class 11 CHAPTER 6 WORK, ENERGY AND POWER
1 P a g e Work Physics Notes Class 11 CHAPTER 6 WORK, ENERGY AND POWER When a force acts on an object and the object actually moves in the direction of force, then the work is said to be done by the force.
More informationPHYS 101-4M, Fall 2005 Exam #3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
PHYS 101-4M, Fall 2005 Exam #3 Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A bicycle wheel rotates uniformly through 2.0 revolutions in
More informationFundamental Concepts in Fluid Mechanics
A significant portion of these notes summarizes various sections of Massey, but additional material from other sources is also included. Note that the notes are incomplete; they will be completed during
More informationSTUDY PACKAGE. Available Online : www.mathsbysuhag.com
fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks] j?kqcj jk[ks VsdAA jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth
More informationPhysics 1120: Simple Harmonic Motion Solutions
Questions: 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 Physics 1120: Simple Harmonic Motion Solutions 1. A 1.75 kg particle moves as function of time as follows: x = 4cos(1.33t+π/5) where distance is measured
More informationEXPERIMENT 10 CONSTANT HEAD METHOD
EXPERIMENT 10 PERMEABILITY (HYDRAULIC CONDUCTIVITY) TEST CONSTANT HEAD METHOD 106 Purpose: The purpose of this test is to determine the permeability (hydraulic conductivity) of a sandy soil by the constant
More informationCourse in. Nonlinear FEM
Course in Introduction Outline Lecture 1 Introduction Lecture 2 Geometric nonlinearity Lecture 3 Material nonlinearity Lecture 4 Material nonlinearity continued Lecture 5 Geometric nonlinearity revisited
More informationDimensional Analysis
Dimensional Analysis An Important Example from Fluid Mechanics: Viscous Shear Forces V d t / / / / / / / / / / / / / / / / / / / / / / / / / / / / / / / / / Ƭ = F/A = μ V/d More generally, the viscous
More informationSOLUTIONS TO CONCEPTS CHAPTER 17
1. Given that, 400 m < < 700 nm. 1 1 1 700nm 400nm SOLUTIONS TO CONCETS CHATER 17 1 1 1 3 10 c 3 10 (Where, c = spee of light = 3 10 m/s) 7 7 7 7 7 10 4 10 7 10 4 10 4.3 10 14 < c/ < 7.5 10 14 4.3 10 14
More informationMODELING THE EFFECT OF TEMPERATURE AND FREQUENCY ON BITUMEN-COATED HELICAL CABLE ELEMENTS
MODELING THE EFFECT OF TEMPERATURE AND FREQUENCY ON BITUMEN-COATED HELICAL CABLE ELEMENTS Bjørn Konradsen 1 Technological Analyses Centre, Hybrid Underwater Cables, Nexans Norway Steinar V. Ouren Material
More informationStanford Rock Physics Laboratory - Gary Mavko. Basic Geophysical Concepts
Basic Geophysical Concepts 14 Body wave velocities have form: velocity= V P = V S = V E = K + (4 /3)µ ρ µ ρ E ρ = λ + µ ρ where ρ density K bulk modulus = 1/compressibility µ shear modulus λ Lamé's coefficient
More informationSolved with COMSOL Multiphysics 4.3
Vibrating String Introduction In the following example you compute the natural frequencies of a pre-tensioned string using the 2D Truss interface. This is an example of stress stiffening ; in fact the
More information