Fluid mechanics (wb1225)

Similar documents
PIPE FLOWS: LECTURE /04/2017. Yesterday, for the example problem Δp = f(v, ρ, μ, L, D) We came up with the non dimensional relation

ME 305 Fluid Mechanics I. Part 8 Viscous Flow in Pipes and Ducts. Flow in Pipes and Ducts. Flow in Pipes and Ducts (cont d)

Reynolds, an engineering professor in early 1880 demonstrated two different types of flow through an experiment:

OE4625 Dredge Pumps and Slurry Transport. Vaclav Matousek October 13, 2004

Fluid Mechanics II Viscosity and shear stresses

ME 305 Fluid Mechanics I. Chapter 8 Viscous Flow in Pipes and Ducts

DEVELOPED LAMINAR FLOW IN PIPE USING COMPUTATIONAL FLUID DYNAMICS M.

Mechanical Engineering Programme of Study

Basic Fluid Mechanics

Bernoulli and Pipe Flow

Lecture 30 Review of Fluid Flow and Heat Transfer

2, where dp is the constant, R is the radius of

Fluids. Fluids in Motion or Fluid Dynamics

Internal Forced Convection. Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

Viscous Flow in Ducts

Exercise 5: Exact Solutions to the Navier-Stokes Equations I

ME 331 Homework Assignment #6

Chapter 8: Flow in Pipes

Lectures on Applied Reactor Technology and Nuclear Power Safety. Lecture No 6

FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER

Lesson 6 Review of fundamentals: Fluid flow

Chapter 5 Principles of Convection heat transfer (Text: J. P. Holman, Heat Transfer, 8 th ed., McGraw Hill, NY)

Major and Minor Losses

Laminar Flow. Chapter ZERO PRESSURE GRADIENT

Masters in Mechanical Engineering. Problems of incompressible viscous flow. 2µ dx y(y h)+ U h y 0 < y < h,

Internal Flow: Heat Transfer in Pipes

Study fluid dynamics. Understanding Bernoulli s Equation.

Lecture 27 (Walker: ) Fluid Dynamics Nov. 9, 2009

ρg 998(9.81) LV 50 V. d2g 0.062(9.81)

SYSTEMS VS. CONTROL VOLUMES. Control volume CV (open system): Arbitrary geometric space, surrounded by control surfaces (CS)

Lesson 37 Transmission Of Air In Air Conditioning Ducts

Compressible Duct Flow with Friction

Pipe Flow. Lecture 17

FLUID MECHANICS. Lecture 7 Exact solutions

Introduction to Fluid Flow

FORMULA SHEET. General formulas:

FLUID MECHANICS D203 SAE SOLUTIONS TUTORIAL 2 APPLICATIONS OF BERNOULLI SELF ASSESSMENT EXERCISE 1

9. Pumps (compressors & turbines) Partly based on Chapter 10 of the De Nevers textbook.

Part A: 1 pts each, 10 pts total, no partial credit.

7.6 Example von Kármán s Laminar Boundary Layer Problem

MAXIMUM AND AVERAGE VELOCITIES IN PIPE FLOWS - AN EXPERIMENTAL STUDY

Chapter 6. Losses due to Fluid Friction

Piping Systems and Flow Analysis (Chapter 3)

Heat Transfer Convection

Convection. forced convection when the flow is caused by external means, such as by a fan, a pump, or atmospheric winds.

Convective Mass Transfer

Fundamental Concepts of Convection : Flow and Thermal Considerations. Chapter Six and Appendix D Sections 6.1 through 6.8 and D.1 through D.

ME19b. FINAL REVIEW SOLUTIONS. Mar. 11, 2010.

Lecture 30 (Walker: ) Fluid Dynamics April 15, 2009

Chapter 9. Flow over Immersed Bodies

PROBLEM SET 6. SOLUTIONS April 1, 2004

FE Exam Fluids Review October 23, Important Concepts

FE Fluids Review March 23, 2012 Steve Burian (Civil & Environmental Engineering)

BERNOULLI EQUATION. The motion of a fluid is usually extremely complex.

Exercise sheet 5 (Pipe flow)

External Flow and Boundary Layer Concepts

What s important: viscosity Poiseuille's law Stokes' law Demo: dissipation in flow through a tube

LECTURE 1 THE CONTENTS OF THIS LECTURE ARE AS FOLLOWS:

FLOW MEASUREMENT IN PIPES EXPERIMENT

Chapter 10: Flow Flow in in Conduits Conduits Dr Ali Jawarneh

Candidates must show on each answer book the type of calculator used. Only calculators permitted under UEA Regulations may be used.

Determination of Pressure Losses in Hydraulic Pipeline Systems by Considering Temperature and Pressure

EXPERIMENT II - FRICTION LOSS ALONG PIPE AND LOSSES AT PIPE FITTINGS

External Flows. Dye streak. turbulent. laminar transition

SIMPLE Algorithm for Two-Dimensional Channel Flow. Fluid Flow and Heat Transfer

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

The Shallow Water Equations

6. Laminar and turbulent boundary layers

Chapter 6. Losses due to Fluid Friction

FLUID MECHANICS. Chapter 9 Flow over Immersed Bodies

When water (fluid) flows in a pipe, for example from point A to point B, pressure drop will occur due to the energy losses (major and minor losses).

Chapter 8: Flow in Pipes

Chapter (6) Energy Equation and Its Applications

FLUID MECHANICS. Dynamics of Viscous Fluid Flow in Closed Pipe: Darcy-Weisbach equation for flow in pipes. Major and minor losses in pipe lines.

Fluid Mechanics Discussion. Prepared By: Dr.Khalil M. Al-Astal Eng.Ahmed S. Al-Agha Eng.Ruba M. Awad

5.8 Laminar Boundary Layers

FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER

Applied Fluid Mechanics

2 Internal Fluid Flow

Chemical Reaction Engineering. Lecture 7

Empirical Co - Relations approach for solving problems of convection 10:06:43

PIPE FLOW. General Characteristic of Pipe Flow. Some of the basic components of a typical pipe system are shown in Figure 1.

ρ mixture = m mixture /V = (SG antifreeze ρ water V antifreeze + SG water ρ water V water )/V, so we get

Two Phase Flows (Section 3) The Basic Model

Chapter 10. Solids and Fluids

Pressure in stationary and moving fluid. Lab-On-Chip: Lecture 2

Pressure in stationary and moving fluid Lab- Lab On- On Chip: Lecture 2

Chapter 7: Natural Convection

External Forced Convection. Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

Engineers Edge, LLC PDH & Professional Training

CFD Analysis of Forced Convection Flow and Heat Transfer in Semi-Circular Cross-Sectioned Micro-Channel

Hydraulics. B.E. (Civil), Year/Part: II/II. Tutorial solutions: Pipe flow. Tutorial 1

Sourabh V. Apte. 308 Rogers Hall

Phy 212: General Physics II. Daniel Bernoulli ( )

R09. d water surface. Prove that the depth of pressure is equal to p +.

Introduction to Heat and Mass Transfer. Week 14

Fluid Mechanics Answer Key of Objective & Conventional Questions

Figure 3: Problem 7. (a) 0.9 m (b) 1.8 m (c) 2.7 m (d) 3.6 m

BOUNDARY LAYER ANALYSIS WITH NAVIER-STOKES EQUATION IN 2D CHANNEL FLOW

Chapter 14. Lecture 1 Fluid Mechanics. Dr. Armen Kocharian

Transcription:

Fluid mechanics (wb225) Lecture 8: flows through pipes and ducts

Examples of pipe flows [] [2] [3] [4] 2

Flow states in pipe flow [5] Re crit 2300 3

Laminar vs turbulent [5] [6] 4

Pipe flow transition [5] 5

Pipe entrance length laminar flow: L e d 0.06 Re turbulent flow: L e d 4.4 Re 6 [5] 6

Flow with energy losses p + ρv 2 2 + ρgz p 2 ρv 2 2 2 ρgz 2 = 0 [5] p + ρv 2 2 + ρgz p 2 ρv 2 2 2 ρgz 2 = p loss 7

Flow in a circular pipe [5] 8

Control volume analysis continuity: Q = Q 2 V = V 2 steady-flow energy equation: p + ρv 2 2 + ρgz = p 2 + ρv 2 2 2 + ρgz 2 + ρgh f [5] h f = z + p ρg z + p 2 2 ρg = z + p ρg h f = z + p ρg momentum equation: p π R 2 + ρg( π R 2 ) L sinφ τ w ( 2π R) L = &m ( V 2 V )= 0 z + p ρg = h f = 2τ w ρg L R with: z = L sinφ 9

Dimensional analysis h f = 2τ w ρg L R, τ w 8τ w ρv = f = F Re, ε 2 d = F ( ρ,v, µ, d,ε), ε = wall roughness ρgh f = f L d ρv 2 2, f = Darcy friction factor 0

Equations of motion continuity equation: ( r r ru r )+ ( r θ u θ )+ u x x = 0 ( r r ru r )= 0 ru r = const BC: u r = 0, r = R u r = 0 momentum equation: u = u x (r) ρ u t r + ρu u x = dp r rτ ( ) = d dx τ (r) = 2 r d p dx dx + ρg x + r r rτ ( ) ( p ρgx sinφ) = d dx p 4 2 ρgz 43 p ( )

Laminar flow solution τ = µ du dr = rk K = d p 2 dx integrate: u(r) = 4 r 2 K µ + C BC: u = 0, r = R C = R 2 K 4µ u(r) = K 4µ R 2 r 2 ( ) u max = KR 2 4 µ [5] Q = u(r)2π r dr Q = 0 R Kπ R 4 8µ V = Q A = Q π R 2 = 2 u max 2

Laminar flow solution (cont d) Q = Kπ R 4 8µ Q = π R 4 8µ p L p = 8µ LQ π R 4 τ w = µ du dr r= R = 2µu max R = 2 R p L u(r) = u ( max r 2 R 2 ) u max = KR 2 4 µ = pr 2 4 µl p = f L d ρv 2 2 p = 8µLQ = 8µL π R 4 π R π R 2 V = 8 2 2µ L 4 2 R 2R = 64 L ρvd µ d 2 ρv 2 f = 64 Re π R 2 π R 2 ρv 2 2 ρv 2 3

Example 6.4 An oil with ρ = 900 kg/m 3 and ν = 2x0-4 m 2 /s flows upward through an inclined pipe as shown in the diagram. The pressure and elevation ar given at sections and 2, 0 m apart. Assuming steady laminar flow: a) verify that the flow is up; b) compute h f between and 2; c) compute Q, V, and Re d. d) Is the flow laminar? [5] 4

Bore diameter u = K 4µ R 2 r 2 ( ) Q = u(r) 2π r dr a 0 = Kπ 8µ R 4 = P / L 28µ / π D 4 P = 28 π = 64 Re µ L D L D Q D = 28 3 π µ L D ρu 2 2 π / 4 D 2 U = 28 2 D 3 4 ν UD L D ρu 2 2 Q = P / L 28µ / π D 4 δq ~ 0.% δ P ~ 0.% δ D D 4 δq Q + δ P P 0.05% D = 50 µm δ D 75 nm 5

Stenosis [5] 6

Vascular networks [7] [9] [8] [0] 7

Tube networks n= n=2 n=3 D L D 2 L 2 D 3 L3 D 2 = α D D 3 = α D 2 = α 2 D L 2 = β L L 3 = β L 2 = β 2 L Q = Q = 2 Q 2 = 4 Q 3 = P = P + P 2 + P 3 + 8

P = 28ηQ L π D 4 + 28ηQ 2L 2 π D 2 4 + 28ηQ 3L 3 π D 3 4 +... = 28η π = 28ηQ π Q L + Q 2 L 2 + Q 3L 3 +... 4 4 4 D D 2 D 3 L D 4 + 2 = 28ηQ L + 4 2 π D L 2 D 2 4 + 4 L 2 L D + 4 4 D 2 4 L 3 D +... 4 3 L 3 L D +... 4 D 3 4 = 28ηQ L β + 4 2 π D α + β 2 4 4 α +... 8 = P + 2 β + ( β ) 2 α 4 2 +... α 4 = P 2 β 2 α 4 β α 4 < 9

Optimal Value volume β surface pressure α 20

Vascular network Distance (mm) Distance (mm) [5] Distance (mm) Distance (mm) 2

Summary Chapter 6: 6.-6.2, 6.4 Examples: 6.4-6.5 Problems: see BlackBoard 22

Source. Trans Alaska Oil Pipeline, http://www.bloomberg.com, photo courtesy of Daniel Acker/Bloomberg 2. Suncor refinery, Montreal, http://www.flickr.com/photos/manualcrank/446758550/, photo courtesy of manuel crank 3. Heart Disease, http://bruisedfruits.net/378/heart-disease.html 4. Waterleiding verdeler (waterworks distributor), http://www.hetkapottehuis.nl/album2/2005/2005-0- 05/slides/Waterleiding%20verdeler.html, photo courtesy of Het Kapotte Huis 5. Frank M. White, Fluid Mechanics, McGraw-Hill Series in Mechanical Engineering 6. Multimedia Fluid Mechanics DVD-ROM, G. M. Homsy, University of California, Santa Barbara 7. The vascular system of a bat wing, http://archive.org/stream/archivfrmikros07berl#page/n400/mode/up, photo courtesy of Internet Archive 8. Lungs, http://commons.wikimedia.org/wiki/file:lungs_(animated).gif, photo courtesy of Mikael Häggström 9. Poplar leaf - Feuille de tremble, http://www.flickr.com/photos/monteregina/4998677623/, photo courtesy of monteregina 0. Structure in leaf, http://dsdn04robchesney.blogspot.nl/20/05/precedent-images.html, photo courtesy of Rob Chesney 23