Vocabulary: Viscosity Reynolds Number Laminar. Objectives:

Size: px
Start display at page:

Download "Vocabulary: Viscosity Reynolds Number Laminar. Objectives:"

Transcription

1 Fluid Mechanics for High School Author: Vishal Tandon Date Created: March 2010 Subject: Physics Level: High School Standards: New York State Physics Standards Standard 1 Analysis, Inquiry, and Design Standard 4 The Physical Setting Standard 7 Interdisciplinary Problem Solving Schedule: One 60-minute Lab Period Objectives: Students will learn about basic concepts in fluid mechanics, including turbulent vs. laminar flow, compressibility, and hydraulic resistance. Students will: Learn about viscosity by comparing glycerin to water Observe mixing at low and high Reynolds number by putting drops of dye into glycerin and water Do an experiment to see the (near) reversibility of low Re flow Determine the difference in compressibility between water and air Apply pressure by hand to actuate flow in 25 and 100 micron capillaries to observe the difference in hydraulic resistance in a tactile way Vocabulary: Viscosity Reynolds Number Laminar Materials: For Each Group (2-4): Water Food Coloring (or dyed water and dyed glycerin) Glycerin (honey or corn syrup can be used) Transfer Pipettes Stirring Sticks Gloves Safety: Compressibility Hydraulic Resistance Turbulent 5 ml Plastic Luer-Lok Syringes Luer-Lok fittings with plugs and PEEK fittings for capillaries (From LabSmith) Large Petri Dish Small Petri Dish 2 Beakers 1-25 µm Silica Capillary (polyimide coated), cut to about 5 cm in length µm Silica Capillary (polyimide coated), cut to about 5 cm in length ( Gloves should be worn at all times to prevent staining of hands. None of the chemicals involved are dangerous. The capillaries are sharp enough to prick skin (but not cut it).

2 Science Content for the Teacher: This lab is intended to give students a basic understanding of different ways in which fluids are characterized, and how flows can change dramatically depending on the nature of the fluid involved, the speed of flow, and the size of the system. Here, we assume that students have no knowledge of fluid mechanics. Fluid motion is described by utilizing continuum versions of conservation of momentum and conservation of mass, leading to the Cauchy Momentum and the continuity equations respectively. ρu x 0 Here represents the full stress tensor, is the fluid velocity vector, is the fluid density, and is the body force on the fluid per unit volume. These are the most general equations, but they simplify in certain situations (Newtonian fluid, incompressible flow, laminar flow, steady state, etc.) Formally, viscosity defines how a fluid responds to a shear stress. For Newtonian fluids, we assume that the deviatoric part of the stress tensor is linearly proportional to the velocity gradient tensor, and the viscosity defines the constant of proportionality. This is an excellent approximation for most common fluids (all of the fluids used in this lab). For Newtonian fluids, viscosity is associated with the thickness of the fluid, and the resistance to flow, making it somewhat analogous to friction for motion of solids. Students should gain this intuitive understanding of viscosity by going through the lab. The Cauchy momentum equation simplifies if the fluid is incompressible, i.e. its density is constant and uniform. Most common working liquids, such as water, are essentially incompressible, whereas gases, such as air, are compressible. For a steady, incompressible flow, the continuity equation becomes: x u 0 The momentum equation reduces to the steady-state, incompressible Navier- Stokes equations (for a Newtonian fluid). In non-dimensional form; - 2

3 1 Where non-dimensionalized parameters are indicated by * s, the velocity has been normalized by a characteristic velocity in the system, and distances have been normalized by a characteristic length scale. Re, the Reynolds number, is a non-dimensional parameter that arises from this analysis. It is defined as Where is the fluid density, U is a characteristic (sometimes the maximum) velocity of the system, L is a characteristic length scale, and is the kinematic viscosity of the fluid. Solving the Navier-Stokes equations for pressure-driven flow in a pipe shows that the flow rate for a given applied pressure gradient is inversely proportional to the fourth power of the radius of the pipe. Students will see the powerful dependence of flow rate on channel size in a tactile way when they work with the microfluidic capillaries in this lab. The Reynolds number can be understood as the ratio of inertial forces to viscous forces; at high Reynolds number inertia dominates, fluids tend to coast (they continue moving even after actuation is ceased), fluids mix, and flow can be chaotic; at low Reynolds number viscosity dominates, flow creeps, and mixing is slow and mainly due to diffusion. The Reynolds number is also an indicator of whether a flow is laminar or turbulent. The flow transitions to turbulence at approximately Re>2000. In this lab, students will examine cases of relatively high and very low Re, by examining water as compared to a fluid with very high viscosity, glycerin. At very low Reynolds number (formally Re = 0), the Navier-Stokes equations are well-approximated by the Stokes equations. 0 1 Two important properties of Stokes flow are: 1) Instantaneity: The properties of the flow do not depend on the time-history of the flow, unless there are timedependent boundary conditions, and 2) Time-reversibility: A time-reversed version of a solution to the Stokes Equations also solves the Stokes Equations, i.e. a flow can be reversed and reverted back to the original configuration by exactly reversing the actuation. Students will explore time-reversibility in this lab by recreating a simplified version of one of a famous experiment from one of G.I. - 3

4 Taylor s lectures ( - see in particular, Low Reynolds Number Flow, about 15 min into the video). Preparation: 1. Photocopy print materials (Fluids_worksheet) 2. Distribute materials evenly to each lab group. 3. Pour chemicals into beakers and petri dishes as indicated in the lab handout. If more than one lab period is available, students can do this themselves (giving them a chance to see the differences in viscosity between the fluids). However, if only one lab period is available, all of the chemicals need to be in the appropriate containers for the experiment prior to the start of the lab period. - 4

5 Classroom Procedure: Engage (Time: 5 min) Allow students to play with the fluids using stirring sticks before they conduct any mixing experiments. Encourage them to discuss and write down their observations of differences between glycerin and water. Explore (Time: 25 min) Exploration and explanation are concurrent in this lab, owing to its many parts. Move students through each section of the lab, encouraging them to stop and observe flows before fully mixing fluids. When doing the annular shear flow experiment, encourage students to draw a design of their choosing, and to look at the effect of distance from the rotating petri dish. Explain (Time: 25 min) At each stage, ask directed questions about their observations (Are the flows the same? How are they different?) The students observations will immediately help them learn many fundamental aspects of fluid mechanics. Guide these observations with additional explanations; in particular point out fluid deformation, shear stress, increasing shear near the moving boundary, and turbulent/convective mixing vs. diffusive mixing. - 5

6 Assessment: The following rubric can be used to assess students during each part of the activity. The term expectations here refers to the content, process and attitudinal goals for this activity. Evidence for understanding may be in the form of oral as well as written communication, both with the teacher as well as observed communication with other students. Specifics are listed in the table below. 1= exceeds expectations 2= meets expectations consistently 3= meets expectations occasionally 4= not meeting expectations Engage Explore Explain 1 Shows leadership in discussion and engages others in making astute 2 Participates in working with fluids and makes 3 Participates in working with the fluids, but does not make any technical Completes experiments and writes down detailed observations of differences between different flows. Makes serious attempt at predicting outcomes. Completes experiments and writes down observations of flows. Completes experiments, but writes minimal Demonstrates understanding of differences between turbulent/laminar, and compressible/incompressible flows. Understands how predicted outcomes differed from the results (if at all). Demonstrates understanding of differences between flows, and documents outcomes. Wrote observations from experiments down, but does not necessarily understand how differences in experimental conditions led to different flows. 4 Does not participate at all. Does not participate at all. Does not participate at all. Supplemental Information: Fluids lectures at are useful. Safety: Gloves should be worn at all times to prevent staining from dye solutions. The capillaries are sharp enough to prick skin. Acknowledgments: Dr. Shivaun Archer, Dr. Chris Schaffer, Nevjinder Singhota - Cornell University. Walter Peck - Whitney Point High School, New York National Science Foundation Cornell GK-12 Program: DGE

Differential Relations for Fluid Flow. Acceleration field of a fluid. The differential equation of mass conservation

Differential Relations for Fluid Flow. Acceleration field of a fluid. The differential equation of mass conservation Differential Relations for Fluid Flow In this approach, we apply our four basic conservation laws to an infinitesimally small control volume. The differential approach provides point by point details of

More information

Basic Equations, Boundary Conditions and Dimensionless Parameters

Basic Equations, Boundary Conditions and Dimensionless Parameters Chapter 2 Basic Equations, Boundary Conditions and Dimensionless Parameters In the foregoing chapter, many basic concepts related to the present investigation and the associated literature survey were

More information

Fluids and Solids: Fundamentals

Fluids 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 information

Basic Principles in Microfluidics

Basic 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 information

4.What is the appropriate dimensionless parameter to use in comparing flow types? YOUR ANSWER: The Reynolds Number, Re.

4.What is the appropriate dimensionless parameter to use in comparing flow types? YOUR ANSWER: The Reynolds Number, Re. CHAPTER 08 1. What is most likely to be the main driving force in pipe flow? A. Gravity B. A pressure gradient C. Vacuum 2.What is a general description of the flow rate in laminar flow? A. Small B. Large

More information

NUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES

NUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES Vol. XX 2012 No. 4 28 34 J. ŠIMIČEK O. HUBOVÁ NUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES Jozef ŠIMIČEK email: jozef.simicek@stuba.sk Research field: Statics and Dynamics Fluids mechanics

More information

Viscous flow in pipe

Viscous flow in pipe Viscous flow in pipe Henryk Kudela Contents 1 Laminar or turbulent flow 1 2 Balance of Momentum - Navier-Stokes Equation 2 3 Laminar flow in pipe 2 3.1 Friction factor for laminar flow...........................

More information

EXAMPLE: Water Flow in a Pipe

EXAMPLE: Water Flow in a Pipe EXAMPLE: Water Flow in a Pipe P 1 > P 2 Velocity profile is parabolic (we will learn why it is parabolic later, but since friction comes from walls the shape is intuitive) The pressure drops linearly along

More information

1. Fluids Mechanics and Fluid Properties. 1.1 Objectives of this section. 1.2 Fluids

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 information

11 Navier-Stokes equations and turbulence

11 Navier-Stokes equations and turbulence 11 Navier-Stokes equations and turbulence So far, we have considered ideal gas dynamics governed by the Euler equations, where internal friction in the gas is assumed to be absent. Real fluids have internal

More information

INTRODUCTION TO FLUID MECHANICS

INTRODUCTION TO FLUID MECHANICS INTRODUCTION TO FLUID MECHANICS SIXTH EDITION ROBERT W. FOX Purdue University ALAN T. MCDONALD Purdue University PHILIP J. PRITCHARD Manhattan College JOHN WILEY & SONS, INC. CONTENTS CHAPTER 1 INTRODUCTION

More information

Contents. Microfluidics - Jens Ducrée Physics: Navier-Stokes Equation 1

Contents. Microfluidics - Jens Ducrée Physics: Navier-Stokes Equation 1 Contents 1. Introduction 2. Fluids 3. Physics of Microfluidic Systems 4. Microfabrication Technologies 5. Flow Control 6. Micropumps 7. Sensors 8. Ink-Jet Technology 9. Liquid Handling 10.Microarrays 11.Microreactors

More information

1 The basic equations of fluid dynamics

1 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 information

For Water to Move a driving force is needed

For 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 information

FLUID MECHANICS IM0235 DIFFERENTIAL EQUATIONS - CB0235 2014_1

FLUID MECHANICS IM0235 DIFFERENTIAL EQUATIONS - CB0235 2014_1 COURSE CODE INTENSITY PRE-REQUISITE CO-REQUISITE CREDITS ACTUALIZATION DATE FLUID MECHANICS IM0235 3 LECTURE HOURS PER WEEK 48 HOURS CLASSROOM ON 16 WEEKS, 32 HOURS LABORATORY, 112 HOURS OF INDEPENDENT

More information

Notes on Polymer Rheology Outline

Notes 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 information

Adaptation of General Purpose CFD Code for Fusion MHD Applications*

Adaptation of General Purpose CFD Code for Fusion MHD Applications* Adaptation of General Purpose CFD Code for Fusion MHD Applications* Andrei Khodak Princeton Plasma Physics Laboratory P.O. Box 451 Princeton, NJ, 08540 USA akhodak@pppl.gov Abstract Analysis of many fusion

More information

FLUID DYNAMICS. Intrinsic properties of fluids. Fluids behavior under various conditions

FLUID DYNAMICS. Intrinsic properties of fluids. Fluids behavior under various conditions FLUID DYNAMICS Intrinsic properties of fluids Fluids behavior under various conditions Methods by which we can manipulate and utilize the fluids to produce desired results TYPES OF FLUID FLOW Laminar or

More information

The Viscosity of Fluids

The Viscosity of Fluids Experiment #11 The Viscosity of Fluids References: 1. Your first year physics textbook. 2. D. Tabor, Gases, Liquids and Solids: and Other States of Matter (Cambridge Press, 1991). 3. J.R. Van Wazer et

More information

Differential Balance Equations (DBE)

Differential Balance Equations (DBE) Differential Balance Equations (DBE) Differential Balance Equations Differential balances, although more complex to solve, can yield a tremendous wealth of information about ChE processes. General balance

More information

CBE 6333, R. Levicky 1 Review of Fluid Mechanics Terminology

CBE 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 information

Distinguished Professor George Washington University. Graw Hill

Distinguished Professor George Washington University. Graw Hill Mechanics of Fluids Fourth Edition Irving H. Shames Distinguished Professor George Washington University Graw Hill Boston Burr Ridge, IL Dubuque, IA Madison, Wl New York San Francisco St. Louis Bangkok

More information

Contents. Microfluidics - Jens Ducrée Physics: Fluid Dynamics 1

Contents. Microfluidics - Jens Ducrée Physics: Fluid Dynamics 1 Contents 1. Introduction 2. Fluids 3. Physics of Microfluidic Systems 4. Microfabrication Technologies 5. Flow Control 6. Micropumps 7. Sensors 8. Ink-Jet Technology 9. Liquid Handling 10.Microarrays 11.Microreactors

More information

Introduction to Microfluidics. Date: 2013/04/26. Dr. Yi-Chung Tung. Outline

Introduction to Microfluidics. Date: 2013/04/26. Dr. Yi-Chung Tung. Outline Introduction to Microfluidics Date: 2013/04/26 Dr. Yi-Chung Tung Outline Introduction to Microfluidics Basic Fluid Mechanics Concepts Equivalent Fluidic Circuit Model Conclusion What is Microfluidics Microfluidics

More information

Chapter 8: Flow in Pipes

Chapter 8: Flow in Pipes Objectives 1. Have a deeper understanding of laminar and turbulent flow in pipes and the analysis of fully developed flow 2. Calculate the major and minor losses associated with pipe flow in piping networks

More information

4 Microscopic dynamics

4 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 information

FLUID FLOW STREAMLINE LAMINAR FLOW TURBULENT FLOW REYNOLDS NUMBER

FLUID FLOW STREAMLINE LAMINAR FLOW TURBULENT FLOW REYNOLDS NUMBER VISUAL PHYSICS School of Physics University of Sydney Australia FLUID FLOW STREAMLINE LAMINAR FLOW TURBULENT FLOW REYNOLDS NUMBER? What type of fluid flow is observed? The above pictures show how the effect

More information

CE 204 FLUID MECHANICS

CE 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 information

Dimensional Analysis

Dimensional 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 information

Lecture 5 Hemodynamics. Description of fluid flow. The equation of continuity

Lecture 5 Hemodynamics. Description of fluid flow. The equation of continuity 1 Lecture 5 Hemodynamics Description of fluid flow Hydrodynamics is the part of physics, which studies the motion of fluids. It is based on the laws of mechanics. Hemodynamics studies the motion of blood

More information

Dimensional analysis is a method for reducing the number and complexity of experimental variables that affect a given physical phenomena.

Dimensional analysis is a method for reducing the number and complexity of experimental variables that affect a given physical phenomena. Dimensional Analysis and Similarity Dimensional analysis is very useful for planning, presentation, and interpretation of experimental data. As discussed previously, most practical fluid mechanics problems

More information

Fundamentals of Fluid Mechanics

Fundamentals of Fluid Mechanics Sixth Edition. Fundamentals of Fluid Mechanics International Student Version BRUCE R. MUNSON DONALD F. YOUNG Department of Aerospace Engineering and Engineering Mechanics THEODORE H. OKIISHI Department

More information

VISUAL PHYSICS School of Physics University of Sydney Australia. Why do cars need different oils in hot and cold countries?

VISUAL PHYSICS School of Physics University of Sydney Australia. Why do cars need different oils in hot and cold countries? VISUAL PHYSICS School of Physics University of Sydney Australia FLUID FLOW VISCOSITY POISEUILLE'S LAW? Why do cars need different oils in hot and cold countries? Why does the engine runs more freely as

More information

du u U 0 U dy y b 0 b

du u U 0 U dy y b 0 b BASIC CONCEPTS/DEFINITIONS OF FLUID MECHANICS (by Marios M. Fyrillas) 1. Density (πυκνότητα) Symbol: 3 Units of measure: kg / m Equation: m ( m mass, V volume) V. Pressure (πίεση) Alternative definition:

More information

Fluid Dynamics Viscosity. Dave Foster Department of Chemical Engineering University of Rochester Email: dafoster@che

Fluid Dynamics Viscosity. Dave Foster Department of Chemical Engineering University of Rochester Email: dafoster@che Fluid Dynamics Viscosity Dave Foster Department of Chemical Engineering University of Rochester Email: dafoster@che che.rochester.eduedu 1 Chemical Engineering What do Chemical Engineers Do? Manufacturing

More information

XI / PHYSICS FLUIDS IN MOTION 11/PA

XI / 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 information

SIZE OF A MOLECULE FROM A VISCOSITY MEASUREMENT

SIZE 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 information

Dynamic Process Modeling. Process Dynamics and Control

Dynamic Process Modeling. Process Dynamics and Control Dynamic Process Modeling Process Dynamics and Control 1 Description of process dynamics Classes of models What do we need for control? Modeling for control Mechanical Systems Modeling Electrical circuits

More information

The ratio of inertial to viscous forces is commonly used to scale fluid flow, and is called the Reynolds number, given as:

The ratio of inertial to viscous forces is commonly used to scale fluid flow, and is called the Reynolds number, given as: 12.001 LAB 3C: STOKES FLOW DUE: WEDNESDAY, MARCH 9 Lab Overview and Background The viscosity of a fluid describes its resistance to deformation. Water has a very low viscosity; the force of gravity causes

More information

Introduction to COMSOL. The Navier-Stokes Equations

Introduction to COMSOL. The Navier-Stokes Equations Flow Between Parallel Plates Modified from the COMSOL ChE Library module rev 10/13/08 Modified by Robert P. Hesketh, Chemical Engineering, Rowan University Fall 2008 Introduction to COMSOL The following

More information

Physics for the Life Sciences: Fall 2008 Lecture #25

Physics for the Life Sciences: Fall 2008 Lecture #25 Physics for the Life Sciences: Fall 2008 Lecture #25 Real fluids: As we have mentioned several times, real fluids are more complex than the ideal fluids described by the continuity equation and Bernoulli

More information

Diffusion and Fluid Flow

Diffusion and Fluid Flow Diffusion and Fluid Flow What determines the diffusion coefficient? What determines fluid flow? 1. Diffusion: Diffusion refers to the transport of substance against a concentration gradient. ΔS>0 Mass

More information

Objectives: Vocabulary:

Objectives: Vocabulary: Introduction to Agarose Gel Electrophoresis: A Precursor to Cornell Institute for Biology Teacher s lab Author: Jennifer Weiser and Laura Austen Date Created: 2010 Subject: Molecular Biology and Genetics

More information

FLUID FLOW Introduction General Description

FLUID FLOW Introduction General Description FLUID FLOW Introduction Fluid flow is an important part of many processes, including transporting materials from one point to another, mixing of materials, and chemical reactions. In this experiment, you

More information

Scalars, Vectors and Tensors

Scalars, Vectors and Tensors Scalars, Vectors and Tensors A scalar is a physical quantity that it represented by a dimensional number at a particular point in space and time. Examples are hydrostatic pressure and temperature. A vector

More information

OUTCOME 3 TUTORIAL 5 DIMENSIONAL ANALYSIS

OUTCOME 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 information

Chapter 10. Flow Rate. Flow Rate. Flow Measurements. The velocity of the flow is described at any

Chapter 10. Flow Rate. Flow Rate. Flow Measurements. The velocity of the flow is described at any Chapter 10 Flow Measurements Material from Theory and Design for Mechanical Measurements; Figliola, Third Edition Flow Rate Flow rate can be expressed in terms of volume flow rate (volume/time) or mass

More information

Experiment 3 Pipe Friction

Experiment 3 Pipe Friction EML 316L Experiment 3 Pipe Friction Laboratory Manual Mechanical and Materials Engineering Department College of Engineering FLORIDA INTERNATIONAL UNIVERSITY Nomenclature Symbol Description Unit A cross-sectional

More information

Distance Learning Program

Distance Learning Program Distance Learning Program Leading To Master of Engineering or Master of Science In Mechanical Engineering Typical Course Presentation Format Program Description Clarkson University currently offers a Distance

More information

The Viscosity of Fluids

The Viscosity of Fluids Experiment #11 The Viscosity of Fluids References: 1. Your first year physics textbook. 2. D. Tabor, Gases, Liquids and Solids: and Other States of Matter (Cambridge Press, 1991). 3. J.R. Van Wazer et

More information

CHEMICAL ENGINEERING AND CHEMICAL PROCESS TECHNOLOGY - Vol. I - Interphase Mass Transfer - A. Burghardt

CHEMICAL ENGINEERING AND CHEMICAL PROCESS TECHNOLOGY - Vol. I - Interphase Mass Transfer - A. Burghardt INTERPHASE MASS TRANSFER A. Burghardt Institute of Chemical Engineering, Polish Academy of Sciences, Poland Keywords: Turbulent flow, turbulent mass flux, eddy viscosity, eddy diffusivity, Prandtl mixing

More information

When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid.

When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid. Fluid Statics When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid. Consider a small wedge of fluid at rest of size Δx, Δz, Δs

More information

HEAVY OIL FLOW MEASUREMENT CHALLENGES

HEAVY OIL FLOW MEASUREMENT CHALLENGES HEAVY OIL FLOW MEASUREMENT CHALLENGES 1 INTRODUCTION The vast majority of the world s remaining oil reserves are categorised as heavy / unconventional oils (high viscosity). Due to diminishing conventional

More information

Fluid Mechanics: Static s Kinematics Dynamics Fluid

Fluid 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 information

Lecture 8 - Turbulence. Applied Computational Fluid Dynamics

Lecture 8 - Turbulence. Applied Computational Fluid Dynamics Lecture 8 - Turbulence Applied Computational Fluid Dynamics Instructor: André Bakker http://www.bakker.org André Bakker (2002-2006) Fluent Inc. (2002) 1 Turbulence What is turbulence? Effect of turbulence

More information

VISCOSITY 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. 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 information

CE 6303 MECHANICS OF FLUIDS L T P C QUESTION BANK PART - A

CE 6303 MECHANICS OF FLUIDS L T P C QUESTION BANK PART - A CE 6303 MECHANICS OF FLUIDS L T P C QUESTION BANK 3 0 0 3 UNIT I FLUID PROPERTIES AND FLUID STATICS PART - A 1. Define fluid and fluid mechanics. 2. Define real and ideal fluids. 3. Define mass density

More information

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

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 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 forces. 2 Objectives Have a working knowledge of the basic

More information

Lecture 4 Classification of Flows. Applied Computational Fluid Dynamics

Lecture 4 Classification of Flows. Applied Computational Fluid Dynamics Lecture 4 Classification of Flows Applied Computational Fluid Dynamics Instructor: André Bakker http://www.bakker.org André Bakker (00-006) Fluent Inc. (00) 1 Classification: fluid flow vs. granular flow

More information

1.Name the four types of motion that a fluid element can experience. YOUR ANSWER: Translation, linear deformation, rotation, angular deformation.

1.Name the four types of motion that a fluid element can experience. YOUR ANSWER: Translation, linear deformation, rotation, angular deformation. CHAPTER 06 1.Name the four types of motion that a fluid element can experience. YOUR ANSWER: Translation, linear deformation, rotation, angular deformation. 2.How is the acceleration of a particle described?

More information

Teil I. Student Laboratory Manuals

Teil I. Student Laboratory Manuals Teil I Student Laboratory Manuals 1 IR1 5. Fluid friction in liquids 5.1 Introduction Generally the term fluid is understood to be matter either in the gaseous or liquid state. The physics involved on

More information

Lecture 6 - Boundary Conditions. Applied Computational Fluid Dynamics

Lecture 6 - Boundary Conditions. Applied Computational Fluid Dynamics Lecture 6 - Boundary Conditions Applied Computational Fluid Dynamics Instructor: André Bakker http://www.bakker.org André Bakker (2002-2006) Fluent Inc. (2002) 1 Outline Overview. Inlet and outlet boundaries.

More information

DISTANCE DEGREE PROGRAM CURRICULUM NOTE:

DISTANCE DEGREE PROGRAM CURRICULUM NOTE: Bachelor of Science in Electrical Engineering DISTANCE DEGREE PROGRAM CURRICULUM NOTE: Some Courses May Not Be Offered At A Distance Every Semester. Chem 121C General Chemistry I 3 Credits Online Fall

More information

Pressure drop in pipes...

Pressure drop in pipes... Pressure drop in pipes... PRESSURE DROP CALCULATIONS Pressure drop or head loss, occurs in all piping systems because of elevation changes, turbulence caused by abrupt changes in direction, and friction

More information

Open channel flow Basic principle

Open channel flow Basic principle Open channel flow Basic principle INTRODUCTION Flow in rivers, irrigation canals, drainage ditches and aqueducts are some examples for open channel flow. These flows occur with a free surface and the pressure

More information

Salem Community College Course Syllabus. Course Title: Physics I. Course Code: PHY 101. Lecture Hours: 2 Laboratory Hours: 4 Credits: 4

Salem Community College Course Syllabus. Course Title: Physics I. Course Code: PHY 101. Lecture Hours: 2 Laboratory Hours: 4 Credits: 4 Salem Community College Course Syllabus Course Title: Physics I Course Code: PHY 101 Lecture Hours: 2 Laboratory Hours: 4 Credits: 4 Course Description: The basic principles of classical physics are explored

More information

Free Convection Film Flows and Heat Transfer

Free Convection Film Flows and Heat Transfer Deyi Shang Free Convection Film Flows and Heat Transfer With 109 Figures and 69 Tables < J Springer Contents 1 Introduction 1 1.1 Scope 1 1.2 Application Backgrounds 1 1.3 Previous Developments 2 1.3.1

More information

Dynamics in nanoworlds

Dynamics in nanoworlds Dynamics in nanoworlds Interplay of energy, diffusion and friction in (sub)cellular world 1 NB Queste diapositive sono state preparate per il corso di Biofisica tenuto dal Dr. Attilio V. Vargiu presso

More information

A LAMINAR FLOW ELEMENT WITH A LINEAR PRESSURE DROP VERSUS VOLUMETRIC FLOW. 1998 ASME Fluids Engineering Division Summer Meeting

A LAMINAR FLOW ELEMENT WITH A LINEAR PRESSURE DROP VERSUS VOLUMETRIC FLOW. 1998 ASME Fluids Engineering Division Summer Meeting TELEDYNE HASTINGS TECHNICAL PAPERS INSTRUMENTS A LAMINAR FLOW ELEMENT WITH A LINEAR PRESSURE DROP VERSUS VOLUMETRIC FLOW Proceedings of FEDSM 98: June -5, 998, Washington, DC FEDSM98 49 ABSTRACT The pressure

More information

240EQ014 - Transportation Science

240EQ014 - Transportation Science Coordinating unit: 240 - ETSEIB - Barcelona School of Industrial Engineering Teaching unit: 713 - EQ - Department of Chemical Engineering Academic year: Degree: 2015 MASTER'S DEGREE IN CHEMICAL ENGINEERING

More information

INVESTIGATION OF FALLING BALL VISCOMETRY AND ITS ACCURACY GROUP R1 Evelyn Chou, Julia Glaser, Bella Goyal, Sherri Wykosky

INVESTIGATION OF FALLING BALL VISCOMETRY AND ITS ACCURACY GROUP R1 Evelyn Chou, Julia Glaser, Bella Goyal, Sherri Wykosky INVESTIGATION OF FALLING BALL VISCOMETRY AND ITS ACCURACY GROUP R1 Evelyn Chou, Julia Glaser, Bella Goyal, Sherri Wykosky ABSTRACT: A falling ball viscometer and its associated equations were studied in

More information

Ch 2 Properties of Fluids - II. Ideal Fluids. Real Fluids. Viscosity (1) Viscosity (3) Viscosity (2)

Ch 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 information

Practice Problems on Boundary Layers. Answer(s): D = 107 N D = 152 N. C. Wassgren, Purdue University Page 1 of 17 Last Updated: 2010 Nov 22

Practice Problems on Boundary Layers. Answer(s): D = 107 N D = 152 N. C. Wassgren, Purdue University Page 1 of 17 Last Updated: 2010 Nov 22 BL_01 A thin flat plate 55 by 110 cm is immersed in a 6 m/s stream of SAE 10 oil at 20 C. Compute the total skin friction drag if the stream is parallel to (a) the long side and (b) the short side. D =

More information

Abaqus/CFD Sample Problems. Abaqus 6.10

Abaqus/CFD Sample Problems. Abaqus 6.10 Abaqus/CFD Sample Problems Abaqus 6.10 Contents 1. Oscillatory Laminar Plane Poiseuille Flow 2. Flow in Shear Driven Cavities 3. Buoyancy Driven Flow in Cavities 4. Turbulent Flow in a Rectangular Channel

More information

Open Channel Flow. M. Siavashi. School of Mechanical Engineering Iran University of Science and Technology

Open Channel Flow. M. Siavashi. School of Mechanical Engineering Iran University of Science and Technology M. Siavashi School of Mechanical Engineering Iran University of Science and Technology W ebpage: webpages.iust.ac.ir/msiavashi Email: msiavashi@iust.ac.ir Landline: +98 21 77240391 Fall 2013 Introduction

More information

Physics 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 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 information

Rheological Properties of Topical Formulations

Rheological 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 information

CHEG 3128 Heat, Mass, & Kinetics Laboratory Diffusion in Laminar Flow Regimes Modeling and COMSOL Tutorial Tutorial by Andrea Kadilak

CHEG 3128 Heat, Mass, & Kinetics Laboratory Diffusion in Laminar Flow Regimes Modeling and COMSOL Tutorial Tutorial by Andrea Kadilak CHEG 3128 Heat, Mass, & Kinetics Laboratory Diffusion in Laminar Flow Regimes Modeling and COMSOL Tutorial Tutorial by Andrea Kadilak Introduction COMSOL is a computer modeling software package that will

More information

Laminar Flow and Heat Transfer of Herschel-Bulkley Fluids in a Rectangular Duct; Finite-Element Analysis

Laminar Flow and Heat Transfer of Herschel-Bulkley Fluids in a Rectangular Duct; Finite-Element Analysis Tamkang Journal of Science and Engineering, Vol. 12, No. 1, pp. 99 107 (2009) 99 Laminar Flow and Heat Transfer of Herschel-Bulkley Fluids in a Rectangular Duct; Finite-Element Analysis M. E. Sayed-Ahmed

More information

Chapter 2. Derivation of the Equations of Open Channel Flow. 2.1 General Considerations

Chapter 2. Derivation of the Equations of Open Channel Flow. 2.1 General Considerations Chapter 2. Derivation of the Equations of Open Channel Flow 2.1 General Considerations Of interest is water flowing in a channel with a free surface, which is usually referred to as open channel flow.

More information

ENV5056 Numerical Modeling of Flow and Contaminant Transport in Rivers. Equations. Asst. Prof. Dr. Orhan GÜNDÜZ

ENV5056 Numerical Modeling of Flow and Contaminant Transport in Rivers. Equations. Asst. Prof. Dr. Orhan GÜNDÜZ ENV5056 Numerical Modeling of Flow and Contaminant Transport in Rivers Derivation of Flow Equations Asst. Prof. Dr. Orhan GÜNDÜZ General 3-D equations of incompressible fluid flow Navier-Stokes Equations

More information

Viscosity: A Property of fluids 307-6 Compare the viscosity of various liquids 307-7 Describe factors that can modify the viscosity of a liquid 208-6

Viscosity: A Property of fluids 307-6 Compare the viscosity of various liquids 307-7 Describe factors that can modify the viscosity of a liquid 208-6 Viscosity: A Property of fluids 307-6 Compare the viscosity of various liquids 307-7 Describe factors that can modify the viscosity of a liquid 208-6 Design an experiment to test the viscosity of various

More information

Lecture 24 - Surface tension, viscous flow, thermodynamics

Lecture 24 - Surface tension, viscous flow, thermodynamics Lecture 24 - Surface tension, viscous flow, thermodynamics Surface tension, surface energy The atoms at the surface of a solid or liquid are not happy. Their bonding is less ideal than the bonding of atoms

More information

Written By Kelly Lundstrom & Kennda Lynch January 31, 2012 Milk Dye ACTIVITY PLAN

Written By Kelly Lundstrom & Kennda Lynch January 31, 2012 Milk Dye ACTIVITY PLAN Milk Dye ACTIVITY PLAN Objective: Students will use the scientific method to test the difference between using whole milk and skim milk in this milk and food dye experiment. Students will explore ideas

More information

Compressible Fluids. Faith A. Morrison Associate Professor of Chemical Engineering Michigan Technological University November 4, 2004

Compressible Fluids. Faith A. Morrison Associate Professor of Chemical Engineering Michigan Technological University November 4, 2004 94 c 2004 Faith A. Morrison, all rights reserved. Compressible Fluids Faith A. Morrison Associate Professor of Chemical Engineering Michigan Technological University November 4, 2004 Chemical engineering

More information

Viscosity experiments: physical controls and implications for volcanic hazards. Ben Edwards Dept of Geology, Dickinson College

Viscosity experiments: physical controls and implications for volcanic hazards. Ben Edwards Dept of Geology, Dickinson College Viscosity experiments: physical controls and implications for volcanic hazards Student Name: Ben Edwards Dept of Geology, Dickinson College OBJECTIVES OF LAB Learn about the rheological property called

More information

Transport Phenomena. The Art of Balancing. Harry Van den Akker Robert F. Mudde. Delft Academic Press

Transport Phenomena. The Art of Balancing. Harry Van den Akker Robert F. Mudde. Delft Academic Press Transport Phenomena The Art of Balancing Harry Van den Akker Robert F. Mudde Delft Academic Press Delft Academic Press First edition 2014 Published by Delft Academic Press /VSSD Leeghwaterstraat, 2628

More information

جامعة البلقاء التطبيقية

جامعة البلقاء التطبيقية AlBalqa Applied University تا سست عام 997 The curriculum of associate degree in Air Conditioning, Refrigeration and Heating Systems consists of (7 credit hours) as follows: Serial No. Requirements First

More information

Experiment # 3: Pipe Flow

Experiment # 3: Pipe Flow ME 05 Mechanical Engineering Lab Page ME 05 Mechanical Engineering Laboratory Spring Quarter 00 Experiment # 3: Pipe Flow Objectives: a) Calibrate a pressure transducer and two different flowmeters (paddlewheel

More information

Microfluidic Principles Part 1

Microfluidic Principles Part 1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 1 Companion lecture to the textbook: Fundamentals of BioMEMS and Medical Microdevices, by Dr. Steven S. Saliterman www.tc.umn.edu/~drsteve

More information

PUMPS STEAM TURBINES BUILDING & FIRE WASTEWATER SERVICE PUMP CLINIC 22 VISCOSITY

PUMPS STEAM TURBINES BUILDING & FIRE WASTEWATER SERVICE PUMP CLINIC 22 VISCOSITY PUMP CLINIC 22 VISCOSITY The viscosity of a fluid is that property which tends to resist a shearing force. It can be thought of as the internal friction resulting when one layer of fluid is made to move

More information

PHYSICS FUNDAMENTALS-Viscosity and flow

PHYSICS FUNDAMENTALS-Viscosity and flow PHYSICS FUNDAMENTALS-Viscosity and flow The origin of viscosity When a force is applied to a solid, it will yield slightly, and then resist further movement. However, when we apply force to a fluid, it

More information

Lecture 17. Last time we saw that the rotational analog of Newton s 2nd Law is

Lecture 17. Last time we saw that the rotational analog of Newton s 2nd Law is Lecture 17 Rotational Dynamics Rotational Kinetic Energy Stress and Strain and Springs Cutnell+Johnson: 9.4-9.6, 10.1-10.2 Rotational Dynamics (some more) Last time we saw that the rotational analog of

More information

Fluid Dynamics and the Navier-Stokes Equation

Fluid Dynamics and the Navier-Stokes Equation Fluid Dynamics and the Navier-Stokes Equation CMSC498A: Spring 12 Semester By: Steven Dobek 5/17/2012 Introduction I began this project through a desire to simulate smoke and fire through the use of programming

More information

Collision of a small bubble with a large falling particle

Collision of a small bubble with a large falling particle EPJ Web of Conferences 67, 212 (214) DOI: 1.11/ epjconf/ 21467212 C Owned by the authors, published by EDP Sciences, 214 Collision of a small bubble with a large falling particle Jiri Vejrazka 1,a, Martin

More information

Chapter 10 Rotational Motion. Copyright 2009 Pearson Education, Inc.

Chapter 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 information

Practice Problems on the Navier-Stokes Equations

Practice Problems on the Navier-Stokes Equations ns_0 A viscous, incompressible, Newtonian liquid flows in stead, laminar, planar flow down a vertical wall. The thickness,, of the liquid film remains constant. Since the liquid free surface is eposed

More information

L r = L m /L p. L r = L p /L m

L 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 information