Chapter 1 Fluid Characteristics

Similar documents
Introduction to Marine Hydrodynamics

Part II Fundamentals of Fluid Mechanics By Munson, Young, and Okiishi

HYDRAULICS STAFF SELECTION COMMISSION CIVIL ENGINEERING STUDY MATERIAL HYDRAULICS

Review of Fluid Mechanics

Fluid Mechanics Introduction

Fluid Properties and Units

CHAPTER 1 Fluids and their Properties

We may have a general idea that a solid is hard and a fluid is soft. This is not satisfactory from

Fluid Mechanics Abdusselam Altunkaynak

1. The Properties of Fluids

2. For a S.H.O. determine, (a) the total energy (E), the kinetic and potential energies. of half amplitude:

1. Introduction, fluid properties (1.1, 2.8, 4.1, and handouts)

Liquids and solids are essentially incompressible substances and the variation of their density with pressure is usually negligible.

Lecturer, Department t of Mechanical Engineering, SVMIT, Bharuch

P = 1 3 (σ xx + σ yy + σ zz ) = F A. It is created by the bombardment of the surface by molecules of fluid.

CHAPTER (2) FLUID PROPERTIES SUMMARY DR. MUNZER EBAID MECH.ENG.DEPT.

University of Hail Faculty of Engineering DEPARTMENT OF MECHANICAL ENGINEERING. ME Fluid Mechanics Lecture notes. Chapter 1

[5] Stress and Strain

Summary PHY101 ( 2 ) T / Hanadi Al Harbi

Continuum Mechanics. Continuum Mechanics and Constitutive Equations

Chapter 5. The Differential Forms of the Fundamental Laws

Basic Equations of Elasticity

Non-Newtonian fluids is the fluids in which shear stress is not directly proportional to deformation rate, such as toothpaste,

Chapter 1: Basic Concepts

Welcome to MECH 280. Ian A. Frigaard. Department of Mechanical Engineering, University of British Columbia. Mech 280: Frigaard

CHARACTERISTIC OF FLUIDS. A fluid is defined as a substance that deforms continuously when acted on by a shearing stress at any magnitude.

1 FLUIDS AND THEIR PROPERTIES

Notes 4: Differential Form of the Conservation Equations

PEAT SEISMOLOGY Lecture 2: Continuum mechanics

Rock Rheology GEOL 5700 Physics and Chemistry of the Solid Earth

INTRODUCTION DEFINITION OF FLUID. U p F FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION

Fluid Mechanics-61341

Chapter 9: Differential Analysis of Fluid Flow

NDT&E Methods: UT. VJ Technologies CAVITY INSPECTION. Nondestructive Testing & Evaluation TPU Lecture Course 2015/16.

AMME2261: Fluid Mechanics 1 Course Notes

BFC FLUID MECHANICS BFC NOOR ALIZA AHMAD

Chapter 9: Differential Analysis

Introduction to Fluid Mechanics

Chapter 9: Solids and Fluids

A drop forms when liquid is forced out of a small tube. The shape of the drop is determined by a balance of pressure, gravity, and surface tension

Lecture 3. Properties of Fluids 11/01/2017. There are thermodynamic properties of fluids like:

Class Notes Fall 2014

Differential relations for fluid flow

AE/ME 339. Computational Fluid Dynamics (CFD) K. M. Isaac. Momentum equation. Computational Fluid Dynamics (AE/ME 339) MAEEM Dept.

ESS314. Basics of Geophysical Fluid Dynamics by John Booker and Gerard Roe. Conservation Laws

Fluid Mechanics. Spring 2009

Lecture 8: Tissue Mechanics

OCN/ATM/ESS 587. The wind-driven ocean circulation. Friction and stress. The Ekman layer, top and bottom. Ekman pumping, Ekman suction

In this section, mathematical description of the motion of fluid elements moving in a flow field is

Numerical Heat and Mass Transfer

MECHANICAL PROPERTIES OF FLUIDS:

Continuum mechanism: Stress and strain

Fundamentals of Fluid Dynamics: Elementary Viscous Flow

V (r,t) = i ˆ u( x, y,z,t) + ˆ j v( x, y,z,t) + k ˆ w( x, y, z,t)

SOLIDS AND LIQUIDS - Here's a brief review of the atomic picture or gases, liquids, and solids GASES

12. Stresses and Strains

Future coaching Institute Tirupur

COURSE NUMBER: ME 321 Fluid Mechanics I. Fluid: Concept and Properties

3D Elasticity Theory

EKC314: TRANSPORT PHENOMENA Core Course for B.Eng.(Chemical Engineering) Semester II (2008/2009)

Mechanics of Earthquakes and Faulting

Viscous Flow and Convective Heat Transfer (EGFD 7041) Fall 2018

Stress, Strain, Mohr s Circle

Please remember all the unit that you use in your calculation. There are no marks for correct answer without unit.

Contents. I Introduction 1. Preface. xiii

ME3250 Fluid Dynamics I

Chapter 1. Continuum mechanics review. 1.1 Definitions and nomenclature

Finite Element Method in Geotechnical Engineering

Macroscopic theory Rock as 'elastic continuum'

CHARACTERISTIC OF FLUIDS. A fluid is defined as a substance that deforms continuously when acted on by a shearing stress at any magnitude.

Unit 4: Gas Laws. Matter and Phase Changes

PHYSICS. Course Structure. Unit Topics Marks. Physical World and Measurement. 1 Physical World. 2 Units and Measurements.

PRACTICE QUESTION PAPER WITH SOLUTION CLASS XI PHYSICS

Chapter 1. Viscosity and the stress (momentum flux) tensor

Solid to liquid. Liquid to gas. Gas to solid. Liquid to solid. Gas to liquid. +energy. -energy

Chapter 12. Static Equilibrium and Elasticity

Lecture Outline Chapter 17. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

MULTIPLE-CHOICE PROBLEMS:(Two marks per answer) (Circle the Letter Beside the Most Correct Answer in the Questions Below.)

Way to Success Model Question Paper. Answer Key

Physics 141 Rotational Motion 2 Page 1. Rotational Motion 2

Petroleum Engineering Dept. Fluid Mechanics Second Stage Dr. Ahmed K. Alshara

DIVIDED SYLLABUS ( ) - CLASS XI PHYSICS (CODE 042) COURSE STRUCTURE APRIL

Modelling of dispersed, multicomponent, multiphase flows in resource industries. Section 3: Examples of analyses conducted for Newtonian fluids

Navier-Stokes Equation: Principle of Conservation of Momentum

Petroleum Engineering Department Fluid Mechanics Second Stage Assist Prof. Dr. Ahmed K. Alshara

Fluid Mechanics II Viscosity and shear stresses

Dynamic Meteorology - Introduction

Middle East Technical University Department of Mechanical Engineering ME 305 Fluid Mechanics I Fall 2018 Section 4 (Dr.

Chapter 26 Elastic Properties of Materials

The Physics of Non-Newtonian Fluids

9 MECHANICAL PROPERTIES OF SOLIDS

Rheology of Soft Materials. Rheology

Chapter 9. Solids and Fluids. States of Matter. Solid. Liquid. Gas

Exercise: concepts from chapter 8

ENGR 292 Fluids and Thermodynamics

Chapter 1: Basic Concepts of Thermodynamics. Thermodynamics and Energy. Dimensions and Units

Chapter 6: Momentum Analysis

AE/ME 339. K. M. Isaac Professor of Aerospace Engineering. 12/21/01 topic7_ns_equations 1

Equilibrium. the linear momentum,, of the center of mass is constant

CE MECHANICS OF FLUIDS UNIT I

Transcription:

Chapter 1 Fluid Characteristics 1.1 Introduction 1.1.1 Phases Solid increasing increasing spacing and intermolecular liquid latitude of cohesive Fluid gas (vapor) molecular force plasma motion 1.1.2 Fluidity Fluid deform continuously under shearing (tangential) stresses no matter how small the stress stress time rate of angular deformation (strain, displacement) Newtonian fluid shear stress is linearly proportional to rate of angular deformation starting with zero stress and zero deformation constant of proportionality, namic viscosity Fig. 1.1 water, air [Cf] Analogy between Newtonian fluid and solids obeying Hooke's law of constant modulus of elasticity Solid deform by an amount proportional to the stress applied stress magnitude of the angular deformation (total strain) Non-Newtonian fluid variable (nonlinear) proportionality between stress and deformation rate proportionality = f (length of time of exposure to stress, magnitude of stress) plastics: paint, jelly, polymer solutions Rheology 1 1

solid fluid Elastic Solid perfect memory Plastic partial memory Fluid zero memory 1 2

1.1.3 Compressibility 1) compressible fluid: gases, vapors thermonamics 2) incompressible fluid: liquid (small compressibility), water 1.1.4 Continuum approach - dimensions in fluid space are large compared to the molecular spacing to ignore discrete molecular structure - neglect void - Consider a small volume of fluid V containing a large number of molecules, and let m and v be the mass and velocity of any individual molecule u lim V lim V m V vm m = volume which is sufficiently small compared with the smallest significant length scale in the flow field but is sufficiently large that it contains a large number of molecules [Cf] Molecular approach - molecular point of view - well developed for light gases 1 3

1 4 Ch 1. Fluid Characteristics

1.1.5 No-slip condition at rigid boundary 1) behavior of continuum - type viscous fluids 2) zero relative velocity at the boundary surface (proven by experiments) v 0 ideal fluid real fluid 1.1.6 Multiphase system Single phase fluid combination of liquid gas combination of liquid vapor Multiphase systems cavitation problem combination of liquid solid combination of gas - solid sediment/pollutant transport 1.2 Units of Measurement SI system: metric system English system: ft-lb system * Newton's 2nd law of motion F ma 1 5

F m a 2 force(n) ; mass(kg) ; acceleration(m / sec ) 2 F 1kgm /sec 1N W W mg weight ; g gravitational acceleration 1.3 Properties and States of Fluids 1) extensive properties ~ depend on amount of substance total volume, total energy, total weight 2) intensive properties ~ independent of the amount present volume per unit mass, energy per unit mass weight per unit volume (specific weight, γ ) pressure, viscosity, surface, tension 1.3.1 Properties of importances in fluid namics (1) Pressure, p ~ scalar 2 p F / A (N/m ) p p p gauge absolute atm Forces on a fluid element Bo force: act without physical contact Surface force: require physical contact for transmission 1 6

1) bo force gravity force centrifugal force Coriolis force 2) surface forces normal stress tensile stress (unusual for fluid) pressure tangential stress shear stress (2) Temperature, T two bodies in thermal equilibrium same temperature (3) Density, = mass / volume = M V volume (pressure, temperature) (4) Specific weight, = weight / volume [Re] Flow of a continuous medium ~ Fluids are treated as homogeneous materials. ~ Molecular effects are disregarded. mass density ( xyzt,,, ) lim V 0 M V velocity vector s v lim t 0 t 1 7

(5) Viscosity, ~ due to molecular mobility ~ whenever a fluid moves such that a relative motion exists between adjacent volumes (different velocity) yx shear flow Stress, time rate of angular deformation i) displacement of AB relative to CD in t du du u y tut yt ii) strain = relative displacement = angular displacement du du yt / y t 1 8

iii) time rate of strain ( = time rate of angular displacement of AC) du t/ t du du yx du where yx shear stress acting in the x - direction on a plane whose normal is y - direction 2 (N / m ) du rate of angular deformation(1/ sec) namic molecular viscosity du ms m 2 N/m N s m 2 s m 2 (kg m / s ) kg / m sec kg/m s 2 Kinematic viscosity, kg / m s kg / m 2 m /s kinematic dimensions Fig. 1.4 3 1 9

[Cf] namic: F, L, T kinematic: L, T shear stress deformation viscosity links two Types of Fluid Newtonian fluid constant and unique value of linear relation between and du Non-Newtonian fluid ~ non-linear du n Rheology, plastic 1 10

[Cf] Stress-strain relationship for solid yx d G d relative station displacement of AB d angular deformation ( shear strain) G = modulus of elasticity in torsion fluid solid velocity du d displacement = function of (temperature, pressure) major factor for viscosity when temperature is increasing Liquid intermolecular cohesion decrease cohesive force decrease viscosity Gas exchange of momentum increase molecular activity increase shear stress 1 11

[Re] Exchange of momentum fast-speed layer (FSL) molecules from FSL speed up molecules in LSL molecules from LSL slow down molecules in FSL Two layers tend to stick together as if there is some viscosity between two. low-speed layer (LSL) Water: 1.0 10 3 N 2 s m 1 12

decreases as T increases increases as T increases 1 13

(6) Specific heat, c = ratio of the quantity of heat flowing into a substance per unit mass to the change in temperature (7) Internal energy, u specific internal energy = energy per unit mass, Jkg kinetic + potential energy internal energy (8) Enthalpy specific enthalpy u p/ (9) Bulk modulus of elasticity and Compressibility 1) Compressibility, C = measure of change of volume and density when a substance is subjected to normal pressures or tensions = % change in volume (or density) for a given pressure change dvol C vol / dp d 1 dp 2) Bulk modulus of elasticity, E v E v 1 dp dp C dvol/ vol d / 1 14

p F / A dvol V1 V (10)Vapor pressure, pv = pressure at which liquids boil = equilibrium partial pressure which escaping liquid molecules will exert above any free surface ~ increases with temperature ~ The more volatile the liquid, the higher its vapor pressure. (11) Surface energy and surface tension, At boundaries between gas and liquid phase, molecular attraction introduce forces which cause the interface to behave like a membrane under tension. (force) (distance) work force area area length ~ water: decrease with temperature 1 15

Increase decrease then decrease decrease decrease increase 1 16

[Appendix 1] Coordinate Systems i) Cartesian ( x, yz, ) ii) Cylindrical ( R,, z) x Rcos y Rsin z z iii) Spherical (, r, ) x r sin cos y rsin sin z r cos x R cos R rsin 1 17

[Appendix 2] Tensor Scalar quantity with magnitude only Vector quantity with magnitude and direction Tensor an order array of entities which is invariant under coordinate transformation, this includes scalars and vectors Rank (order) of tensors 0th order 1 component, scalar (e.g., mass, length, pressure) 1st order 3 components, vector (e.g., velocity, force, acceleration) 2nd order 9 components, (e.g., stress, rate of strain, turbulent diffusion coeff.) Example of 2nd order tensor ~ stress acting on a fluid element Stress tensor xx xy xz yx yy yz zx zy zz = normal stress, = shear stress yx = shear stress in xz - plane and in x - direction 1 18