Lecture 4. Lab this week: Cartridge valves Flow divider Properties of Hydraulic Fluids. Lab 8 Sequencing circuit Lab 9 Flow divider

Size: px
Start display at page:

Download "Lecture 4. Lab this week: Cartridge valves Flow divider Properties of Hydraulic Fluids. Lab 8 Sequencing circuit Lab 9 Flow divider"

Transcription

1 91 Lecture 4 Lab this week: Lab 8 Sequencing circuit Lab 9 Flow divider Cartridge valves Flow divider Properties of Hydraulic Fluids Viscosity friction and leakage Bulk modulus Inertance

2 Cartridge Valves 92 Integrate circuits with many components using a manifold Manifold = aluminum block with internal passages Standard configurations

3 93 Cartridge valves Screw-in types (smaller flow rates, single unit) [as in lab] Single valve performs the intended function screws into cavities in manifold cavities are generally common Slip-in type (larger flow rates) essentially a check valve versatile functions accomplished by different covers that provide for additional circuits. Area ratio play a role in the operation of both types of cartridge valves.

4 94 Screw-in Cartridge Valve Single piece implements the function Plugs into standard manifold porting manifold itself being custom built

5 Slip-in example: check valve 95 Possible leakage Preferred!

6 Slip-in Cartridge Valves Area Ratios 96 Closing force: P A P A A P + F s p Opening force: P A A A + P B A B Open! Open or closed?

7 Slip-in Cartridge Pilot Operated Check 97 x B A Slip-in part is just a poppet check valve

8 Slip-in Pilot Operated Relief Valve 98

9 Slip-in: Pilot Operated Directional Control Valve 99

10 Individually Controlled DCV configuration 100 Potential for better energy savings.

11 101 Identify flow measurement sensors What happens when Q left > Q right? What happens when Q right > Q left? Equilibrium position? Flow Divider Valve How to design a flow divider with 2:1 ratio? Some valves are flow combiner/divider? Can this one combine flow?

12 102 Modeling and Analysis of Flow Divider Qa = Qb+Qc Qb = C1(x)*SQRT(Pa-Pb) Qc = C2(x)*SQRT(Pa-Pc) P1 = Pa-(Qb/c1(x))^2 P2 = Pa-(Qc/c2(x))^2 Adjust x based on P 1 and P 2

13 A (fake) Car Talk Puzzle 103 You discovered that on your garage floor that your car is leaking oil. You took it in to the mechanic Joe. Joe was busy, so you had to leave the car at the shop s parking lot for the night. Next morning, Joe took your car into the shop and examined the car for leaks, and found nothing. You took your back home, but lo and behold, the car leaked again on your garage floor. Neither you nor Joe is delusional. What is going on?

14 104 Hydraulic Fluid in Fluid Power Systems Primary role is POWER TRANSMISSION Secondary roles Lubrication Enables moving parts prevents wear, metal/metal contact Load carrying ability parts spot welded together if lubrication film breaks down or too thin Sealing leaks Dimensional clearance may induce leak Certain property of fluid may prevent leak (viscosity) Heat transfer / cooling transfer of heat from work area to reservoir / heat exchanger some fluid properties may vary with temperature

15 105 From: M. Radhakrishnan, Hydraulic Fluids ASME Press

16 Some fluid properties 106 Dynamic Viscosity µ = τ v / N/(m^2s) = sec * kg m/sec ^2/m = kg / (m sec) = 1000 poise y Kinematic Viscosity Easy to measure. If density = 1000kg/m 3, Shear (N / m^2) Tangential speed gradient (1/sec) 1 poise = 10-3 kg /m/s 1 cp = centipoise = 0.01g/m/s υ = µ ρ y Shear force v (y) No shear when there is no velocity gradient normal to flow m 2 /sec = stoke 1 stoke (St) = cm 2 /sec 1 centi-stoke (cst) =0.01 St µ = 3.78 cp υ = 3.78 cst Density (kg/m^3)

17 107 SAE 40 Viscosity decreases with temperature 15 cs at 100degC (212F) 150 cs at 40degC (104F) SAE 10W 4 cs at 100 deg C(212F) 20 cs at 40 degc (104F) Usually data is given at two temperatures use linear interpolation to find intermediate values 5 to 10 times variation with 60degC variation! Water has much lower viscosity than hydraulic oil Which one for winter or for summer? Water: ~1cS for wide range of temperature!

18 108 High viscosity Viscosity is a compromise reduce leak (better sealing) lower chance of oil break down parts spot welded to each other requires larger pressure to sustain flow (sluggish) pump may cavitate (air getting into system) oil / air separation difficult Low viscosity lower drag better efficiency possibility of thin film break down worse leakage (water hydraulics)

19 109 Dynamic viscosity = 4500 cp Diameter of pipe D = 0.05m Length of pipe L = 1 m Velocity at y = 0.5cm is 5m/s Velocity at y = 0cm is 0m/s Example v y Find a) shear drag on and b) pressure drop across the pipe Assume linear velocity profile shear = 4500cP / (1000 N/m^2/sec) * (5m/s / 0.005m) = 4.5 (N/m^2)*sec * 1000/sec = 4500 N/m^2 Drag force = 4500 * pi * D * L = 706 N Pressure drop = Drag force / Area = 4500*4*L/D = 360 kpa

20 Darcy laws: ΔP = Resistance in Pipes and Hoses f (Re) L ρv D 2 2 = f (Re) L D 8ρQ 2 π D 2 4 speed Re = vd v 110 Laminar f=64/re Δ 128µ L πd P = 4 Q Re < 2000 Kinematic viscosity Inertia versus viscous Turbulent Smooth pipe ΔP = / Re 1/ 4 L 8 ρq 2 D π D > Re > 4000

21 Friction Factor Moody Diagram 111

22 Example: 3MW Wind Turbine, 35MPa 112

23 Loss in Connectors 113 K-factor K factors ρv ΔP = K 2 Tee s deg elbow deg elbow 0.75 Ball check valve 4.0 Return bend 2.2 Example: Elbow Q = 15gpm, Pressure drop = 0.6psi Q = 37.5gpm, Pressure drop = 4psi 2 v = (outlet) velocity [m/sec] g = gravity const [m/sec^2] Note: K is unit-less and independent of units ΔP Equivalent formula: ρg 2 v H L = K 2g = H L 2 v = K 2g H L = head loss [m]

24 114 Leakage Leakage flow Q = 3 a w 12µ L ΔP P2 Example: a spool in a sleeve w = pi * D (circumference) L = length of land a Q L a = clearance P1 w Note high viscosity decreases leaks

25 115 Example L clearance = 0.1mm Cylindrical Spool P 90 deg elbow diameter = 0.5cm Sleeve Q = 30 LPM?1: Assuming small leakage, determine pressure P.?2: How long does L have to be for leakage to be less than 0.01% of the flow?

26 116 Efficiency vs Viscosity vs Temperature For hydraulic components (e.g. pumps, motors, actuators) with moving parts, there is always a trade-off between Volumetric efficiency [leakage] Mechanical Efficiency [friction] Total efficiencies for pumps and motors given by: Optimal viscosity Optimal viscosity exists for a given component (and system) However, viscosity changes dramatically by temperature!

27 High V-I Fluids 117 Viscosity Index (VI): measures temperature dependence of viscosity Modified using chemical additives High VI = low temperature dependence Low VI = large temperature dependence VI index is a measure of this slope! ( Defined relative to 2 standard fluids : VI=0, and VI=100 )

28 A (fake) Car Talk Puzzle 118 You discovered that on your garage floor that your car is leaking oil. You took it in to the mechanic Joe. Joe was busy, so you had to leave the car at the shop s parking lot for the night. Next morning, Joe took your car into the shop and examined the car for leaks, and found nothing. You took your back home, but lo and behold, the car leaked again on your garage floor. Neither you nor Joe is delusional. What is going on?

Lecture 5. Labs this week: Please review ME3281 Systems materials! Viscosity and pressure drop analysis Fluid Bulk modulus Fluid Inertance

Lecture 5. Labs this week: Please review ME3281 Systems materials! Viscosity and pressure drop analysis Fluid Bulk modulus Fluid Inertance Labs this week: Lab 10: Sequencing circuit Lecture 5 Lab 11/12: Asynchronous/Synchronous and Parallel/Tandem Operations Please review ME3281 Systems materials! 132 Viscosity and pressure drop analysis

More information

Lecture 5. Labs this week:

Lecture 5. Labs this week: Labs this week: Lab 10: Bleed-off Circuit Lecture 5 Lab 11/12: Asynchronous/Synchronous and Parallel/Tandem Operations Systems Review Homework (due 10/11) Participation is research lab Hydraulic Hybrid

More information

Hydraulic Fundamentals Hydraulics Definition Advent of Oil Hydraulics Pascal s Law Pressure

Hydraulic Fundamentals Hydraulics Definition Advent of Oil Hydraulics Pascal s Law Pressure Fluidsys Training Centre, Bangalore offers an extensive range of skill-based and industry-relevant courses in the field of Pneumatics and Hydraulics. For more details, please visit the website: https://fluidsys.org

More information

Water Circuit Lab. The pressure drop along a straight pipe segment can be calculated using the following set of equations:

Water Circuit Lab. The pressure drop along a straight pipe segment can be calculated using the following set of equations: Water Circuit Lab When a fluid flows in a conduit, there is friction between the flowing fluid and the pipe walls. The result of this friction is a net loss of energy in the flowing fluid. The fluid pressure

More information

LECTURE 6- ENERGY LOSSES IN HYDRAULIC SYSTEMS SELF EVALUATION QUESTIONS AND ANSWERS

LECTURE 6- ENERGY LOSSES IN HYDRAULIC SYSTEMS SELF EVALUATION QUESTIONS AND ANSWERS LECTURE 6- ENERGY LOSSES IN HYDRAULIC SYSTEMS SELF EVALUATION QUESTIONS AND ANSWERS 1. What is the head loss ( in units of bars) across a 30mm wide open gate valve when oil ( SG=0.9) flow through at a

More information

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

Reynolds, an engineering professor in early 1880 demonstrated two different types of flow through an experiment: 7 STEADY FLOW IN PIPES 7.1 Reynolds Number Reynolds, an engineering professor in early 1880 demonstrated two different types of flow through an experiment: Laminar flow Turbulent flow Reynolds apparatus

More information

Pipe Flow. Lecture 17

Pipe Flow. Lecture 17 Pipe Flow Lecture 7 Pipe Flow and the Energy Equation For pipe flow, the Bernoulli equation alone is not sufficient. Friction loss along the pipe, and momentum loss through diameter changes and corners

More information

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)

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) ME 305 Fluid Mechanics I Flow in Pipes and Ducts Flow in closed conduits (circular pipes and non-circular ducts) are very common. Part 8 Viscous Flow in Pipes and Ducts These presentations are prepared

More information

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

FLUID MECHANICS D203 SAE SOLUTIONS TUTORIAL 2 APPLICATIONS OF BERNOULLI SELF ASSESSMENT EXERCISE 1 FLUID MECHANICS D203 SAE SOLUTIONS TUTORIAL 2 APPLICATIONS OF BERNOULLI SELF ASSESSMENT EXERCISE 1 1. A pipe 100 mm bore diameter carries oil of density 900 kg/m3 at a rate of 4 kg/s. The pipe reduces

More information

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

1. Introduction, fluid properties (1.1, 2.8, 4.1, and handouts) 1. Introduction, fluid properties (1.1, 2.8, 4.1, and handouts) Introduction, general information Course overview Fluids as a continuum Density Compressibility Viscosity Exercises: A1 Fluid mechanics Fluid

More information

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

ME 305 Fluid Mechanics I. Chapter 8 Viscous Flow in Pipes and Ducts ME 305 Fluid Mechanics I Chapter 8 Viscous Flow in Pipes and Ducts These presentations are prepared by Dr. Cüneyt Sert Department of Mechanical Engineering Middle East Technical University Ankara, Turkey

More information

Major and Minor Losses

Major and Minor Losses Abstract Major and Minor Losses Caitlyn Collazo, Team 2 (1:00 pm) A Technovate fluid circuit system was used to determine the pressure drop across a pipe section and across an orifice. These pressure drops

More information

HYDRAULIC CONTROL SYSTEMS

HYDRAULIC CONTROL SYSTEMS HYDRAULIC CONTROL SYSTEMS Noah D. Manring Mechanical and Aerospace Engineering Department University of Missouri-Columbia WILEY John Wiley & Sons, Inc. vii Preface Introduction xiii XV FUNDAMENTALS 1 Fluid

More information

Viscosity. appearance.

Viscosity. appearance. Viscosity Viscosityit is probably bbl the single most important t property of a hydraulic fluid. It is a measure of a fluid's resistance to flow. When the viscosity is low, the fluid flows easily and is

More information

Lesson 6 Review of fundamentals: Fluid flow

Lesson 6 Review of fundamentals: Fluid flow Lesson 6 Review of fundamentals: Fluid flow The specific objective of this lesson is to conduct a brief review of the fundamentals of fluid flow and present: A general equation for conservation of mass

More information

REE 307 Fluid Mechanics II. Lecture 1. Sep 27, Dr./ Ahmed Mohamed Nagib Elmekawy. Zewail City for Science and Technology

REE 307 Fluid Mechanics II. Lecture 1. Sep 27, Dr./ Ahmed Mohamed Nagib Elmekawy. Zewail City for Science and Technology REE 307 Fluid Mechanics II Lecture 1 Sep 27, 2017 Dr./ Ahmed Mohamed Nagib Elmekawy Zewail City for Science and Technology Course Materials drahmednagib.com 2 COURSE OUTLINE Fundamental of Flow in pipes

More information

Check-Q-meter. Table of contents. Features. Functions. RE 27551/ /10 Replaces: Type FD

Check-Q-meter. Table of contents. Features. Functions. RE 27551/ /10 Replaces: Type FD Check-Q-meter RE /0.0 /0 Replaces: 09.9 Type FD Nominal size... Series ax. Operating pressure 0 bar ax. Flow 0 l/min K9/ Table of contents Contents Page Features Functions Ordering details Symbols Functional

More information

Piping Systems and Flow Analysis (Chapter 3)

Piping Systems and Flow Analysis (Chapter 3) Piping Systems and Flow Analysis (Chapter 3) 2 Learning Outcomes (Chapter 3) Losses in Piping Systems Major losses Minor losses Pipe Networks Pipes in series Pipes in parallel Manifolds and Distribution

More information

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

Hydraulics. B.E. (Civil), Year/Part: II/II. Tutorial solutions: Pipe flow. Tutorial 1 Hydraulics B.E. (Civil), Year/Part: II/II Tutorial solutions: Pipe flow Tutorial 1 -by Dr. K.N. Dulal Laminar flow 1. A pipe 200mm in diameter and 20km long conveys oil of density 900 kg/m 3 and viscosity

More information

LEAKLESS COOLING SYSTEM V.2 PRESSURE DROP CALCULATIONS AND ASSUMPTIONS

LEAKLESS COOLING SYSTEM V.2 PRESSURE DROP CALCULATIONS AND ASSUMPTIONS CH-1211 Geneva 23 Switzerland EDMS No. ST/CV - Cooling of Electronics & Detectors GUIDE LEAKLESS COOLING SYSTEM V.2 PRESSURE DROP CALCULATIONS AND ASSUMPTIONS Objectives Guide to Leakless Cooling System

More information

Chapter 6. Losses due to Fluid Friction

Chapter 6. Losses due to Fluid Friction Chapter 6 Losses due to Fluid Friction 1 Objectives ä To measure the pressure drop in the straight section of smooth, rough, and packed pipes as a function of flow rate. ä To correlate this in terms of

More information

Chapter 6. Hydraulic cylinders/rams (linear motors), and Lines/fittings. - Transforms the flow of a pressurized fluid into a push or pull of a rod.

Chapter 6. Hydraulic cylinders/rams (linear motors), and Lines/fittings. - Transforms the flow of a pressurized fluid into a push or pull of a rod. Chapter 6. Hydraulic cylinders/rams (linear motors), and Lines/fittings - Transforms the flow of a pressurized fluid into a push or pull of a rod. 6. Single cting Rams Gravity, spring, etc. can force piston

More information

FE Exam Fluids Review October 23, Important Concepts

FE Exam Fluids Review October 23, Important Concepts FE Exam Fluids Review October 3, 013 mportant Concepts Density, specific volume, specific weight, specific gravity (Water 1000 kg/m^3, Air 1. kg/m^3) Meaning & Symbols? Stress, Pressure, Viscosity; Meaning

More information

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

Figure 3: Problem 7. (a) 0.9 m (b) 1.8 m (c) 2.7 m (d) 3.6 m 1. For the manometer shown in figure 1, if the absolute pressure at point A is 1.013 10 5 Pa, the absolute pressure at point B is (ρ water =10 3 kg/m 3, ρ Hg =13.56 10 3 kg/m 3, ρ oil = 800kg/m 3 ): (a)

More information

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

Introduction to Fluid Flow

Introduction to Fluid Flow Introduction to Fluid Flow Learning Outcomes After this lecture you should be able to Explain viscosity and how it changes with temperature Write the continuity equation Define laminar and turbulent flow

More information

Laboratory 9: The Viscosity of Liquids

Laboratory 9: The Viscosity of Liquids Laboratory 9: The Viscosity of Liquids Introduction The essential difference between solids and fluids lies in the nature of their response to the socalled shearing stress. In solids, an elastic force

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

Dynamic Modeling of Fluid Power Transmissions for Wind Turbines

Dynamic Modeling of Fluid Power Transmissions for Wind Turbines Dynamic Modeling of Fluid Power Transmissions for Wind Turbines EWEA OFFSHORE 211 N.F.B. Diepeveen, A. Jarquin Laguna n.f.b.diepeveen@tudelft.nl, a.jarquinlaguna@tudelft.nl Offshore Wind Group, TU Delft,

More information

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

P = 1 3 (σ xx + σ yy + σ zz ) = F A. It is created by the bombardment of the surface by molecules of fluid. CEE 3310 Thermodynamic Properties, Aug. 27, 2010 11 1.4 Review A fluid is a substance that can not support a shear stress. Liquids differ from gasses in that liquids that do not completely fill a container

More information

Chapter 6. Losses due to Fluid Friction

Chapter 6. Losses due to Fluid Friction Chapter 6 Losses due to Fluid Friction 1 Objectives To measure the pressure drop in the straight section of smooth, rough, and packed pipes as a function of flow rate. To correlate this in terms of the

More information

Fluids. Fluids in Motion or Fluid Dynamics

Fluids. Fluids in Motion or Fluid Dynamics Fluids Fluids in Motion or Fluid Dynamics Resources: Serway - Chapter 9: 9.7-9.8 Physics B Lesson 3: Fluid Flow Continuity Physics B Lesson 4: Bernoulli's Equation MIT - 8: Hydrostatics, Archimedes' Principle,

More information

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

Petroleum Engineering Dept. Fluid Mechanics Second Stage Dr. Ahmed K. Alshara Continents Chapter 1. Fluid Mechanics -Properties of fluids -Density, specific gravity, specific volume and Viscosity -Newtonian and non Newtonian fluids -Surface tension Compressibility -Pressure -Cavitations

More information

Visualization of flow pattern over or around immersed objects in open channel flow.

Visualization of flow pattern over or around immersed objects in open channel flow. EXPERIMENT SEVEN: FLOW VISUALIZATION AND ANALYSIS I OBJECTIVE OF THE EXPERIMENT: Visualization of flow pattern over or around immersed objects in open channel flow. II THEORY AND EQUATION: Open channel:

More information

CHAPTER 1 Fluids and their Properties

CHAPTER 1 Fluids and their Properties FLUID MECHANICS Gaza CHAPTER 1 Fluids and their Properties Dr. Khalil Mahmoud ALASTAL Objectives of this Chapter: Define the nature of a fluid. Show where fluid mechanics concepts are common with those

More information

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

OE4625 Dredge Pumps and Slurry Transport. Vaclav Matousek October 13, 2004 OE465 Vaclav Matousek October 13, 004 1 Dredge Vermelding Pumps onderdeel and Slurry organisatie Transport OE465 Vaclav Matousek October 13, 004 Dredge Vermelding Pumps onderdeel and Slurry organisatie

More information

Chapter 10 Flow in Conduits

Chapter 10 Flow in Conduits Chapter 10 Flow in Conduits 10.1 Classifying Flow Laminar Flow and Turbulent Flow Laminar flow Unpredictable Turbulent flow Near entrance: undeveloped developing flow In developing flow, the wall shear

More information

SECTION 5 EDI Cartridge Valves

SECTION 5 EDI Cartridge Valves SECTION Cartridge Valves Make Model Page Way Pilot Operated Poppet Style Way Pilot Operated Double Lock Way Direct cting 3 Way -Position Direct cting 4 Way -Position Direct cting Spool Style 4 Way 3-Position

More information

Lecture Slides. Chapter 12. Lubrication and Journal Bearings

Lecture Slides. Chapter 12. Lubrication and Journal Bearings Lecture Slides Chapter 12 Lubrication and Journal Bearings The McGraw-Hill Companies 2012 Chapter Outline Types of Lubrication Hydrodynamic Hydrostatic Elastohydrodynamic Boundary Solid film Viscosity

More information

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

Lecture 27 (Walker: ) Fluid Dynamics Nov. 9, 2009 Physics 111 Lecture 27 (Walker: 15.5-7) Fluid Dynamics Nov. 9, 2009 Midterm #2 - Monday Nov. 16 Chap. 7,Chap. 8 (not 8.5) Chap. 9 (not 9.6, 9.8) Chap. 10, Chap. 11 (not 11.8-9) Chap. 13 (not 13.6-8) Chap.

More information

V/ t = 0 p/ t = 0 ρ/ t = 0. V/ s = 0 p/ s = 0 ρ/ s = 0

V/ t = 0 p/ t = 0 ρ/ t = 0. V/ s = 0 p/ s = 0 ρ/ s = 0 UNIT III FLOW THROUGH PIPES 1. List the types of fluid flow. Steady and unsteady flow Uniform and non-uniform flow Laminar and Turbulent flow Compressible and incompressible flow Rotational and ir-rotational

More information

Calculation of Pipe Friction Loss

Calculation of Pipe Friction Loss Doc.No. 6122-F3T071 rev.2 Calculation of Pipe Friction Loss Engineering Management Group Development Planning Department Standard Pump Business Division EBARA corporation October 16th, 2013 1 / 33 2 /

More information

The Mechatronics Design for Measuring Fluid Friction Losses in Pipe Flows Rıza Gurbuz

The Mechatronics Design for Measuring Fluid Friction Losses in Pipe Flows Rıza Gurbuz Solid State Phenomena Vol. 113 (2006) pp 603-608 Online available since 2006/Jun/15 at www.scientific.net (2006) Trans Tech Publications, Switzerland doi:10.4028/www.scientific.net/ssp.113.603 The Mechatronics

More information

Hydraulic Design Of Polyethylene Pipes

Hydraulic Design Of Polyethylene Pipes Hydraulic Design Of Polyethylene Pipes Waters & Farr polyethylene pipes offer a hydraulically smooth bore that provides excellent flow characteristics. Other advantages of Waters & Farr polyethylene pipes,

More information

FLOW IN PIPES. Mark J McCready University of Notre Dame July 24, chemeprof.com

FLOW IN PIPES. Mark J McCready University of Notre Dame July 24, chemeprof.com FLOW IN PIPES Mark J McCready University of Notre Dame July 24, 2017 OVERVIEW This lecture will provide the simplest framework to explain The three forces at that are important to fluid flow in pipes The

More information

Chapter 8: Flow in Pipes

Chapter 8: Flow in Pipes 8-1 Introduction 8-2 Laminar and Turbulent Flows 8-3 The Entrance Region 8-4 Laminar Flow in Pipes 8-5 Turbulent Flow in Pipes 8-6 Fully Developed Pipe Flow 8-7 Minor Losses 8-8 Piping Networks and Pump

More information

ME 309 Fluid Mechanics Fall 2010 Exam 2 1A. 1B.

ME 309 Fluid Mechanics Fall 2010 Exam 2 1A. 1B. Fall 010 Exam 1A. 1B. Fall 010 Exam 1C. Water is flowing through a 180º bend. The inner and outer radii of the bend are 0.75 and 1.5 m, respectively. The velocity profile is approximated as C/r where C

More information

HYDRAULICS STAFF SELECTION COMMISSION CIVIL ENGINEERING STUDY MATERIAL HYDRAULICS

HYDRAULICS STAFF SELECTION COMMISSION CIVIL ENGINEERING STUDY MATERIAL HYDRAULICS 1 STAFF SELECTION COMMISSION CIVIL ENGINEERING STUDY MATERIAL Syllabus Hydraulics ( Fluid Mechanics ) Fluid properties, hydrostatics, measurements of flow, Bernoulli's theorem and its application, flow

More information

A Model Answer for. Problem Set #7

A Model Answer for. Problem Set #7 A Model Answer for Problem Set #7 Pipe Flow and Applications Problem.1 A pipeline 70 m long connects two reservoirs having a difference in water level of 6.0 m. The pipe rises to a height of 3.0 m above

More information

Friction Factors and Drag Coefficients

Friction Factors and Drag Coefficients Levicky 1 Friction Factors and Drag Coefficients Several equations that we have seen have included terms to represent dissipation of energy due to the viscous nature of fluid flow. For example, in the

More information

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

Empirical Co - Relations approach for solving problems of convection 10:06:43 Empirical Co - Relations approach for solving problems of convection 10:06:43 10:06:44 Empirical Corelations for Free Convection Use T f or T b for getting various properties like Re = VL c / ν β = thermal

More information

Microfluidics 1 Basics, Laminar flow, shear and flow profiles

Microfluidics 1 Basics, Laminar flow, shear and flow profiles MT-0.6081 Microfluidics and BioMEMS Microfluidics 1 Basics, Laminar flow, shear and flow profiles 11.1.2017 Ville Jokinen Outline of the next 3 weeks: Today: Microfluidics 1: Laminar flow, flow profiles,

More information

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

What s important: viscosity Poiseuille's law Stokes' law Demo: dissipation in flow through a tube PHYS 101 Lecture 29x - Viscosity 29x - 1 Lecture 29x Viscosity (extended version) What s important: viscosity Poiseuille's law Stokes' law Demo: dissipation in flow through a tube Viscosity We introduced

More information

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

Middle East Technical University Department of Mechanical Engineering ME 305 Fluid Mechanics I Fall 2018 Section 4 (Dr. Middle East Technical University Department of Mechanical Engineering ME 305 Fluid Mechanics I Fall 2018 Section 4 (Dr. Sert) Study Set 7 Reading Assignment R1. Read the section Common Dimensionless Groups

More information

Custom Search Sponsored Links

Custom Search Sponsored Links Dynamic, Absolute and Kinematic Viscosity An introduction to dynamic, absolute and kinematic viscosity and how to convert between CentiStokes (cst), CentiPoises (cp), Saybolt Universal Seconds (SSU), degree

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 3 i i 2 1 INTRODUCTION Property:

More information

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).

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). PRESSURE DROP AND OSSES IN PIPE When water (luid) lows in a pipe, or example rom point A to point B, pressure drop will occur due to the energy losses (major and minor losses). A B Bernoulli equation:

More information

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

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 /04/07 ECTURE 4 PIPE FOWS: Yesterday, for the example problem Δp = f(v, ρ, μ,, ) We came up with the non dimensional relation f (, ) 3 V or, p f(, ) You can plot π versus π with π 3 as a parameter. Or,

More information

Hydraulic (Fluid) Systems

Hydraulic (Fluid) Systems Hydraulic (Fluid) Systems Basic Modeling Elements Resistance apacitance Inertance Pressure and Flow Sources Interconnection Relationships ompatibility Law ontinuity Law Derive Input/Output Models ME375

More information

n = Kinematic viscosity (cst) SG = specific gravity or 1 Poise = 100 cp 1 Stoke = 100 cst Q = capacity (m 3 /s) A = tube area (m 2 ) or

n = Kinematic viscosity (cst) SG = specific gravity or 1 Poise = 100 cp 1 Stoke = 100 cst Q = capacity (m 3 /s) A = tube area (m 2 ) or Fmulas Designation Fmula Comments Product Viscosity n = m r n = Kinematic viscosity (mm /s) m = Absolute viscosity (mpa.s) n = m SG n = Kinematic viscosity (cst) m = Absolute viscosity (cp) m = n SG 1

More information

MYcsvtu Notes HEAT TRANSFER BY CONVECTION

MYcsvtu Notes HEAT TRANSFER BY CONVECTION www.mycsvtunotes.in HEAT TRANSFER BY CONVECTION CONDUCTION Mechanism of heat transfer through a solid or fluid in the absence any fluid motion. CONVECTION Mechanism of heat transfer through a fluid in

More information

Non Newtonian Fluid Dynamics

Non Newtonian Fluid Dynamics PDHonline Course M417 (3 PDH) Non Newtonian Fluid Dynamics Instructor: Paul G. Conley, PE 2012 PDH Online PDH Center 5272 Meadow Estates Drive Fairfax, VA 22030-6658 Phone & Fax: 703-988-0088 www.pdhonline.org

More information

Applied Fluid Mechanics

Applied Fluid Mechanics Applied Fluid Mechanics 1. The Nature of Fluid and the Study of Fluid Mechanics 2. Viscosity of Fluid 3. Pressure Measurement 4. Forces Due to Static Fluid 5. Buoyancy and Stability 6. Flow of Fluid and

More information

Sliding Contact Bearings

Sliding Contact Bearings Sliding Contact Bearings Classification of Bearings 1. According to the direction of load to be supported. The bearings under this group are classified as: (a) Radial bearings (b) Thrust bearings. In radial

More information

1-Reynold s Experiment

1-Reynold s Experiment Lect.No.8 2 nd Semester Flow Dynamics in Closed Conduit (Pipe Flow) 1 of 21 The flow in closed conduit ( flow in pipe ) is differ from this occur in open channel where the flow in pipe is at a pressure

More information

MM303 FLUID MECHANICS I PROBLEM SET 1 (CHAPTER 2) FALL v=by 2 =-6 (1/2) 2 = -3/2 m/s

MM303 FLUID MECHANICS I PROBLEM SET 1 (CHAPTER 2) FALL v=by 2 =-6 (1/2) 2 = -3/2 m/s MM303 FLUID MECHANICS I PROBLEM SET 1 (CHAPTER ) FALL 018 1) For the velocity fields given below, determine: i) Whether the flow field is one-, two-, or three-dimensional, and why. ii) Whether the flow

More information

Northern Lesson 2 Gear Pump Terminology. Gear Pump 101. Lesson 2: Gear Pump Terminology. When your reputation depends on it!

Northern Lesson 2 Gear Pump Terminology. Gear Pump 101. Lesson 2: Gear Pump Terminology. When your reputation depends on it! Gear Pump 101 Lesson 2: Gear Pump Terminology When your reputation depends on it! Symbol Term Metric Unit Abbreviation US Customary Unit Abbreviation Conversion factor a A Area square millimeter mm2 square

More information

AP Physics Laboratory #6.1: Analyzing Terminal Velocity Using an Interesting Version of Atwood s Machine

AP Physics Laboratory #6.1: Analyzing Terminal Velocity Using an Interesting Version of Atwood s Machine AP Physics Laboratory #6.1: Analyzing Terminal Velocity Using an Interesting Version of Atwood s Machine Name: Date: Lab Partners: PURPOSE The purpose of this Laboratory is to study a system as it approaches

More information

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

Part A: 1 pts each, 10 pts total, no partial credit. Part A: 1 pts each, 10 pts total, no partial credit. 1) (Correct: 1 pt/ Wrong: -3 pts). The sum of static, dynamic, and hydrostatic pressures is constant when flow is steady, irrotational, incompressible,

More information

where = rate of change of total energy of the system, = rate of heat added to the system, = rate of work done by the system

where = rate of change of total energy of the system, = rate of heat added to the system, = rate of work done by the system The Energy Equation for Control Volumes Recall, the First Law of Thermodynamics: where = rate of change of total energy of the system, = rate of heat added to the system, = rate of work done by the system

More information

EXPERIMENT No.1 FLOW MEASUREMENT BY ORIFICEMETER

EXPERIMENT No.1 FLOW MEASUREMENT BY ORIFICEMETER EXPERIMENT No.1 FLOW MEASUREMENT BY ORIFICEMETER 1.1 AIM: To determine the co-efficient of discharge of the orifice meter 1.2 EQUIPMENTS REQUIRED: Orifice meter test rig, Stopwatch 1.3 PREPARATION 1.3.1

More information

Dynamic (absolute) Viscosity

Dynamic (absolute) Viscosity Viscosity Taken from: http://www.engineeringtoolbox.com/dynamic-absolute-kinematic-viscosity-d_412.html The viscosity of a fluid is an important property in the analysis of liquid behavior and fluid motion

More information

Use N 1, if sizing the valve for a flow rate in volumetric units (gpm or m 3 /h).

Use N 1, if sizing the valve for a flow rate in volumetric units (gpm or m 3 /h). ANSI/ISA/IEC Valve Sizing Catalog 2 March 202 Page 2 Introduction Standardization activities for control valve sizing can be traced back to the early 960's when an American trade association, the Fluids

More information

CVE 372 HYDROMECHANICS EXERCISE PROBLEMS

CVE 372 HYDROMECHANICS EXERCISE PROBLEMS VE 37 HYDROMEHNIS EXERISE PROLEMS 1. pump that has the characteristic curve shown in the accompanying graph is to be installed in the system shown. What will be the discharge of water in the system? Take

More information

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

9. Pumps (compressors & turbines) Partly based on Chapter 10 of the De Nevers textbook. Lecture Notes CHE 31 Fluid Mechanics (Fall 010) 9. Pumps (compressors & turbines) Partly based on Chapter 10 of the De Nevers textbook. Basics (pressure head, efficiency, working point, stability) Pumps

More information

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

Lecture 30 (Walker: ) Fluid Dynamics April 15, 2009 Physics 111 Lecture 30 (Walker: 15.6-7) Fluid Dynamics April 15, 2009 Midterm #2 - Monday April 20 Chap. 7,Chap. 8 (not 8.5) Chap. 9 (not 9.6, 9.8) Chap. 10, Chap. 11 (not 11.8-9) Chap. 13 (not 13.6-8)

More information

Signature: (Note that unsigned exams will be given a score of zero.)

Signature: (Note that unsigned exams will be given a score of zero.) Neatly print your name: Signature: (Note that unsigned exams will be given a score of zero.) Circle your lecture section (-1 point if not circled, or circled incorrectly): Prof. Dabiri Prof. Wassgren Prof.

More information

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

Petroleum Engineering Department Fluid Mechanics Second Stage Assist Prof. Dr. Ahmed K. Alshara Continents Petroleum Engineering Department Fluid Mechanics Second Stage Assist Prof. Dr. Ahmed K. Alshara Chapter 1. Fluid Mechanics -Properties of fluids -Density, specific gravity, specific volume and

More information

ME 4232: FLUID POWER CONTROLS LAB. Class #5 Valve Modeling

ME 4232: FLUID POWER CONTROLS LAB. Class #5 Valve Modeling ME 4232: FLUID POWER CONTROLS LAB Class #5 Valve Modeling Notes No Office Hours Today Upcoming Labs: Lab 9: Flow Divider Lab 10: Sequencing Circuits 2 Agenda Wrap-up: Leakage Calculations Fluid Compressibility

More information

MODULE CODE: ENGG08021 INTRODUCTION TO THERMOFLUIDS. Date: 15 January 2016 Time: 10:00 12:00

MODULE CODE: ENGG08021 INTRODUCTION TO THERMOFLUIDS. Date: 15 January 2016 Time: 10:00 12:00 School of Engineering & Computing Session 2015-16 Paisley Campus Trimester 1 MODULE CODE: ENGG08021 INTRODUCTION TO THERMOFLUIDS Date: 15 January 2016 Time: 10:00 12:00 Attempt FOUR QUESTIONS IN TOTAL

More information

Introduction to Micro/Nanofluidics. Date: 2015/03/13. Dr. Yi-Chung Tung. Outline

Introduction to Micro/Nanofluidics. Date: 2015/03/13. Dr. Yi-Chung Tung. Outline Introduction to Micro/Nanofluidics Date: 2015/03/13 Dr. Yi-Chung Tung Outline Introduction to Microfluidics Basic Fluid Mechanics Concepts Equivalent Fluidic Circuit Model Conclusion What is Microfluidics

More information

Viscous Flow in Ducts

Viscous Flow in Ducts Dr. M. Siavashi Iran University of Science and Technology Spring 2014 Objectives 1. Have a deeper understanding of laminar and turbulent flow in pipes and the analysis of fully developed flow 2. Calculate

More information

Applied Fluid Mechanics

Applied Fluid Mechanics Applied Fluid Mechanics 1. The Nature of Fluid and the Study of Fluid Mechanics 2. Viscosity of Fluid 3. Pressure Measurement 4. Forces Due to Static Fluid 5. Buoyancy and Stability 6. Flow of Fluid and

More information

FLOW IN CONDUITS. Shear stress distribution across a pipe section. Chapter 10

FLOW IN CONDUITS. Shear stress distribution across a pipe section. Chapter 10 Chapter 10 Shear stress distribution across a pipe section FLOW IN CONDUITS For steady, uniform flow, the momentum balance in s for the fluid cylinder yields Fluid Mechanics, Spring Term 2010 Velocity

More information

Only if handing in. Name: Student No.: Page 2 of 7

Only if handing in. Name: Student No.: Page 2 of 7 UNIVERSITY OF TORONTO FACULTY OF APPLIED SCIENCE AND ENGINEERING FINAL EXAMINATION, DECEMBER 10, 2014 2:00 PM 2.5 HOURS CHE 211F FLUID MECHANICS EXAMINER: PROFESSOR D.G. ALLEN ANSWER ALL SEVEN (7) QUESTIONS

More information

Laminar and turbulent flows

Laminar and turbulent flows Ventilation 0 Duct Design Vladimír Zmrhal (room no. 84) http://users.fs.cvut.cz/~zmrhavla/index.htm Dpt. Of Environmental Engineering Laminar and turbulent flos Reynolds number d Re = ν laminar flo Re

More information

INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad AERONAUTICAL ENGINEERING QUESTION BANK : AERONAUTICAL ENGINEERING.

INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad AERONAUTICAL ENGINEERING QUESTION BANK : AERONAUTICAL ENGINEERING. Course Name Course Code Class Branch INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad - 00 0 AERONAUTICAL ENGINEERING : Mechanics of Fluids : A00 : II-I- B. Tech Year : 0 0 Course Coordinator

More information

Fluids and their Properties

Fluids and their Properties Chapter (1) Fluids and their Properties Dr. KHALIL MAHMOUD ALASTAL Eng.Mohammed AbuRahma Eng.Reem Sbaih 2017 Newton s Law of Viscosity: - / Non-Newtonian Fluids: - Mass Density: - / Specific weight: -

More information

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

FE Fluids Review March 23, 2012 Steve Burian (Civil & Environmental Engineering) Topic: Fluid Properties 1. If 6 m 3 of oil weighs 47 kn, calculate its specific weight, density, and specific gravity. 2. 10.0 L of an incompressible liquid exert a force of 20 N at the earth s surface.

More information

Fluid Mechanics II Viscosity and shear stresses

Fluid Mechanics II Viscosity and shear stresses Fluid Mechanics II Viscosity and shear stresses Shear stresses in a Newtonian fluid A fluid at rest can not resist shearing forces. Under the action of such forces it deforms continuously, however small

More information

Universität Duisburg-Essen Fakultät für Ingenieurwissenschaften WS 2012 Maschinenbau, IVG, Thermodynamik Dr. M. A. Siddiqi

Universität Duisburg-Essen Fakultät für Ingenieurwissenschaften WS 2012 Maschinenbau, IVG, Thermodynamik Dr. M. A. Siddiqi 1 Universität Duisburg-Essen 3. Semester Fakultät für Ingenieurwissenschaften WS 2012 Maschinenbau, IVG, Thermodynamik Dr. M. A. Siddiqi THERMODYNAMICS LAB (ISE) Pressure Measurement 2 2 Pressure Measurement

More information

Theory and Fundamental of Fluid Mechanics

Theory and Fundamental of Fluid Mechanics 1 2 Lecture (1) on Fayoum University Theory and Fundamental of Fluid Mechanics By Dr. Emad M. Saad Mechanical Engineering Dept. Faculty of Engineering Fayoum University Faculty of Engineering Mechanical

More information

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

COURSE NUMBER: ME 321 Fluid Mechanics I. Fluid: Concept and Properties COURSE NUMBER: ME 321 Fluid Mechanics I Fluid: Concept and Properties Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET 1 What is Fluid Mechanics? Fluid mechanics

More information

Universal Viscosity Curve Theory

Universal Viscosity Curve Theory TM Universal Viscosity Curve Theory Turbine Flow Meters and Flow Viscosity Introduction Like any transducer, a turbine flow meter is sensitive to physical parameters other than the one which is of interest.

More information

HEAT TRANSFER BY CONVECTION. Dr. Şaziye Balku 1

HEAT TRANSFER BY CONVECTION. Dr. Şaziye Balku 1 HEAT TRANSFER BY CONVECTION Dr. Şaziye Balku 1 CONDUCTION Mechanism of heat transfer through a solid or fluid in the absence any fluid motion. CONVECTION Mechanism of heat transfer through a fluid in the

More information

FACULTY OF CHEMICAL & ENERGY ENGINEERING FLUID MECHANICS LABORATORY TITLE OF EXPERIMENT: MINOR LOSSES IN PIPE (E4)

FACULTY OF CHEMICAL & ENERGY ENGINEERING FLUID MECHANICS LABORATORY TITLE OF EXPERIMENT: MINOR LOSSES IN PIPE (E4) FACULTY OF CHEMICAL & ENERGY ENGINEERING FLUID MECHANICS LABORATORY TITLE OF EXPERIMENT: MINOR LOSSES IN PIPE (E4) 1 1.0 Objectives The objective of this experiment is to calculate loss coefficient (K

More information

PHYSICAL MECHANISM OF CONVECTION

PHYSICAL MECHANISM OF CONVECTION Tue 8:54:24 AM Slide Nr. 0 of 33 Slides PHYSICAL MECHANISM OF CONVECTION Heat transfer through a fluid is by convection in the presence of bulk fluid motion and by conduction in the absence of it. Chapter

More information

Exercise sheet 5 (Pipe flow)

Exercise sheet 5 (Pipe flow) Exercise sheet 5 (Pipe flow) last edited June 4, 2018 These lecture notes are based on textbooks by White [13], Çengel & al.[16], and Munson & al.[18]. Except otherwise indicated, we assume that fluids

More information

PIPING SYSTEMS FOR INDUSTRIAL PLANTS, Part I: Fluid Mechanics, Materials, Piping Systems, Piping Layout

PIPING SYSTEMS FOR INDUSTRIAL PLANTS, Part I: Fluid Mechanics, Materials, Piping Systems, Piping Layout Proyectos Consultoría Formación PIPING SYSTEMS FOR INDUSTRIAL PLANTS, Part I: Fluid Mechanics, Materials, Piping Systems, Piping Layout STUDY NOTES Instructor: Javier Tirenti training@arvengconsulting.com

More information

FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER

FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER ANKARA UNIVERSITY FACULTY OF AGRICULTURE DEPARTMENT OF AGRICULTURAL MACHINERY AND TECHNOLOGIES ENGINEERING 1 5. FLOW IN PIPES Liquid or gas flow through pipes

More information