8-99 M,Y and O. E:\public_html\8-99 elevated tank problem.mcd 1 / 11 9/4/99 / 8:03 AM elevated tank problem.mcd last save 9/4/99 / 8:03 AM

Size: px
Start display at page:

Download "8-99 M,Y and O. E:\public_html\8-99 elevated tank problem.mcd 1 / 11 9/4/99 / 8:03 AM elevated tank problem.mcd last save 9/4/99 / 8:03 AM"

Transcription

1 8-99 M,Y and O The pressure at section shown in the Fi. below is not to fall below 50 lb / in when the flowrate in the tank varies from 0 to cfs and the branch line is shut off. Determine the minimum heiht h of the water tank under the assumption that (a) minor losses are neliible; (b) minor losses not neliible last save E:\public_html\ /

2 known data: psia :=.7 psi k density of water r := 999 vapor pressure of water p m 3 v :=.5 psia viscosity of water m :=.00 newton sec ft of water =.33 psi m unit weiht of water 6. lbf := ft 3 p d pipe diameter d := 6 in area of pipe A 6 := ft 3 ft 3 ft 3 :=.,.5.. rane of flows used sec sec sec Use the "Blasius equation" for smooth pipes, that is pipes with a Reynolds number of less than 00,000. In such a situation the friction factor, f, is function of the Reynolds number, f = f(re). flow velocity as a function of : ( ) := A 6 Reynolds number as a function of : Re( ) := r d ( ) m velocity at water surface in elevated tank : V s := 0 ft sec last save E:\public_html\ /

3 f( ).36 := : Blasius Equation for "smooth pipes", Re < 0 Re( ) elevation at the dischare tap z ( 0 ft + h ft + 6 ft) 5 elevation at the water surface in the tank z s := 0 ft pressure at the water surface in the tank := 0 psi p := 50 psi - residual pressure at the "tap" lenth of pipe in the system L h ft ft ft + 6 ft h ft V s + z s + f L d p + z + + z s + V s f ( h ft) d p 6 ft h + Has solution(s) which are the heads required for a variety of flow rates in order to maintain a dischare pressure of 50 psi. last save E:\public_html\ 3 /

4 h, p := V s + z s f( ) d f( ) d ( ) ( ) + p ft + 6 ft ( ) 00 Head required for flow at 50 psi heiht of tank (ft) h[, 50( psi ) ] ft h[, 60( psi ) ] ft ft 3 sec flowrate residual pressure = 50 psi residual pressure = 60 psi Note the tradeoff, for a specified flow a hiher residual pressure desired at the tap requires a hiher tank last save E:\public_html\ /

5 Now consider what happens if the amount of head available is fixed, as in the case of an existin elevated tank. The curves indicate that hiher demands require hiher pressures. For a specific system with a fixed amount of head an increase in demand means a drop in pressure. Now Include Minor Losses minor loss coefficient K L :=.3 pressure at the tap: p = 50psi Bernoulli's Equation + z s + V s f ( h ft) D 5 K L p 6 ft h + solve it for the heiht of the elevated tank h t ( ) := V s + z s f( ) d ( ) 5 ft f( ) d K L ( ) + ( ) p + 6 ft ( ) last save E:\public_html\ 5 /

6 00 heiht vs flowrate, includes minor loss heiht of tank, ft. h t ( ) h[, 50( psi ) ] ft Flowrate (cfs) heiht with minor losses included, 50 psi heiht w/o minor losses, 50 psi Minor losses make more difference at hiher flowrates last save E:\public_html\ 6 /

7 Now consider the case of a specific elevated tank with a fixed heiht. Solvin Bernoulli's equation for the pressure at the dischare for a fixed tank heiht we et: h := 00 ft : fixed tank heiht al al := 50, min min al min + z s + V s f ( h ft) d A 6 p 6 ft h + A 6 p ( ) := d A 6 z s d A 6 V s d A 6 + f( ) h 506 f( ) + ft 3 ft d A 6 h d A 6 p ( ) psi Pressure at tap vs Demand pressure at the tap, psi al min last save E:\public_html\ 7 /

8 As the demand ets reater the pressure at the tap drops. What, if anythin, does it mean when the pressure becomes neative Now Look at the Branch Line Look at the drawin aain. See the branch line comin off the main dischare? So far the ate valve to that line has been closed. Inorin elevation differences the branch line runs to a lare tank on a farm, as shown below: vent (screened) storae tank branch line off main line lenth of pipe from main line to water surface = 00' depth in tank (variable) last save E:\public_html\ 8 /

9 Suppose that durin a period of hih demand the ate valve is opened to add water to an insecticide solution already in the tank. This solution will then be withdrawn by a tractor with a sprayin attachment for crop application. What are the possibilities. How many of them are ood? lenth of pipe up to the ate valve L h ft ft + 6 ft h ft where h = 00' al al := 50, min min al min p ate ( ) := d A 6 z s d A 6 V s d A 6 + f( ) h 706 f( ) + ft 3 ft d A 6 h d A 6 d A 6 + d p ate ( ) psi Pressure at ate valve to branch line The Bi uestion - What happens to the liquid in the tank when the valve is opened al min last save E:\public_html\ 9 /

10 ft_ho :=.33 psi.7 psi = 57.0ft_HO last save E:\public_html\ 0 /

11 d A 6 + d last save E:\public_html\ /

Fluid Properties: := 1.35 cp liquid viscosoty. m 3 density of the flowing liquid. sg:= specific gravity of the flowing liquid. Pipe System Conditions:

Fluid Properties: := 1.35 cp liquid viscosoty. m 3 density of the flowing liquid. sg:= specific gravity of the flowing liquid. Pipe System Conditions: Control Valve Selection August 17 th 1997 Andrés Felipe Ortega Montoya Chemical Engineer - Universidad Pontificia Bolivariana - Medellín, Colombia. E - Mail: aortega@janua.upb.edu.co I originally obtained

More information

Cunningham, Drew Homework 32 Due: Apr , 4:00 am Inst: Florin 1

Cunningham, Drew Homework 32 Due: Apr , 4:00 am Inst: Florin 1 Cunninham, Drew Homework 3 Due: Apr 1 006, 4:00 am Inst: Florin 1 This print-out should have 10 questions. Multiple-choice questions may continue on the next column or pae find all choices before answerin.

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

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

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

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

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

Mechanical Engineering Programme of Study

Mechanical Engineering Programme of Study Mechanical Engineering Programme of Study Fluid Mechanics Instructor: Marios M. Fyrillas Email: eng.fm@fit.ac.cy SOLVED EXAMPLES ON VISCOUS FLOW 1. Consider steady, laminar flow between two fixed parallel

More information

Chapter 5 Flow in Pipelines

Chapter 5 Flow in Pipelines For updated ersion, please click on http://kalam.ump.edu.my Chapter 5 Flow in ipelines by Dr. Nor Azlina binti Alias Faculty of Ciil and Earth Resources Enineerin azlina@ump.edu.my 5.4 Flowrate and Velocity

More information

TOTAL HEAD, N.P.S.H. AND OTHER CALCULATION EXAMPLES Jacques Chaurette p. eng., June 2003

TOTAL HEAD, N.P.S.H. AND OTHER CALCULATION EXAMPLES Jacques Chaurette p. eng.,   June 2003 TOTAL HEAD, N.P.S.H. AND OTHER CALCULATION EXAMPLES Jacques Chaurette p. eng., www.lightmypump.com June 2003 Figure 1 Calculation example flow schematic. Situation Water at 150 F is to be pumped from a

More information

Chapter Four fluid flow mass, energy, Bernoulli and momentum

Chapter Four fluid flow mass, energy, Bernoulli and momentum 4-1Conservation of Mass Principle Consider a control volume of arbitrary shape, as shown in Fig (4-1). Figure (4-1): the differential control volume and differential control volume (Total mass entering

More information

SOLUTIONS TO PRACTICE PROBLEMS FOR MIDTERM I

SOLUTIONS TO PRACTICE PROBLEMS FOR MIDTERM I University of California, Berkeley Physics 7A Sprin 009 (Yury Kolomensky) SOLUTIONS TO PRACTICE PROBLEMS FOR MIDTERM I Maximum score: 100 points 1. (15 points) Race Stratey Two swimmers need to et from

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

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

Pressure and Flow Characteristics

Pressure and Flow Characteristics Pressure and Flow Characteristics Continuing Education from the American Society of Plumbing Engineers August 2015 ASPE.ORG/ReadLearnEarn CEU 226 READ, LEARN, EARN Note: In determining your answers to

More information

Hydraulics and hydrology

Hydraulics and hydrology Hydraulics and hydrology - project exercises - Class 4 and 5 Pipe flow Discharge (Q) (called also as the volume flow rate) is the volume of fluid that passes through an area per unit time. The discharge

More information

CIVE HYDRAULIC ENGINEERING PART I Pierre Julien Colorado State University

CIVE HYDRAULIC ENGINEERING PART I Pierre Julien Colorado State University CIVE 401 - HYDRAULIC ENGINEERING PART I Pierre Julien Colorado State University Problems with and are considered moderate and those with are the longest and most difficult. In 2018 solve the problems with

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

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

CHAPTER THREE FLUID MECHANICS

CHAPTER THREE FLUID MECHANICS CHAPTER THREE FLUID MECHANICS 3.1. Measurement of Pressure Drop for Flow through Different Geometries 3.. Determination of Operating Characteristics of a Centrifugal Pump 3.3. Energy Losses in Pipes under

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

Engineers Edge, LLC PDH & Professional Training

Engineers Edge, LLC PDH & Professional Training 510 N. Crosslane Rd. Monroe, Georgia 30656 (770) 266-6915 fax (678) 643-1758 Engineers Edge, LLC PDH & Professional Training Copyright, All Rights Reserved Engineers Edge, LLC Pipe Flow-Friction Factor

More information

Exam 2A Solution. 1. A baseball is thrown vertically upward and feels no air resistance. As it is rising

Exam 2A Solution. 1. A baseball is thrown vertically upward and feels no air resistance. As it is rising Exam 2A Solution 1. A baseball is thrown vertically upward and feels no air resistance. As it is risin Solution: Possible answers: A) both its momentum and its mechanical enery are conserved - incorrect.

More information

AEROSPACE ENGINEERING DEPARTMENT. Second Year - Second Term ( ) Fluid Mechanics & Gas Dynamics

AEROSPACE ENGINEERING DEPARTMENT. Second Year - Second Term ( ) Fluid Mechanics & Gas Dynamics AEROSPACE ENGINEERING DEPARTMENT Second Year - Second Term (2008-2009) Fluid Mechanics & Gas Dynamics Similitude,Dimensional Analysis &Modeling (1) [7.2R*] Some common variables in fluid mechanics include:

More information

Chemical Engineering 374

Chemical Engineering 374 Chemical Engineering 374 Fluid Mechanics Single Pipelines 1 Fluids Roadmap Where are we going? 3 Imagine you just started a new job You are a process engineer at a plant Your boss comes to you and says:

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

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

CHAPTER 3 BASIC EQUATIONS IN FLUID MECHANICS NOOR ALIZA AHMAD

CHAPTER 3 BASIC EQUATIONS IN FLUID MECHANICS NOOR ALIZA AHMAD CHAPTER 3 BASIC EQUATIONS IN FLUID MECHANICS 1 INTRODUCTION Flow often referred as an ideal fluid. We presume that such a fluid has no viscosity. However, this is an idealized situation that does not exist.

More information

Physics 111 P 2 A = P 1. A + mg = P 1. A + ρ( AΔh)g. Wednesday, 8-9 pm in NSC 118/119 Sunday, 6:30-8 pm in CCLIR 468.

Physics 111 P 2 A = P 1. A + mg = P 1. A + ρ( AΔh)g. Wednesday, 8-9 pm in NSC 118/119 Sunday, 6:30-8 pm in CCLIR 468. ics Announcements day, ember 11, 011 C5: Fluids Pascal s Principle Archimede s Principle Fluid Flows Continuity Equation Bernoulli s Equation Toricelli s Theorem Wednesday, 8-9 pm in NSC 118/119 Sunday,

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

Chapter (3) Water Flow in Pipes

Chapter (3) Water Flow in Pipes Chapter (3) Water Flow in Pipes Water Flow in Pipes Bernoulli Equation Recall fluid mechanics course, the Bernoulli equation is: P 1 ρg + v 1 g + z 1 = P ρg + v g + z h P + h T + h L Here, we want to study

More information

Fluid Flow Analysis Penn State Chemical Engineering

Fluid Flow Analysis Penn State Chemical Engineering Fluid Flow Analysis Penn State Chemical Engineering Revised Spring 2015 Table of Contents LEARNING OBJECTIVES... 1 EXPERIMENTAL OBJECTIVES AND OVERVIEW... 1 PRE-LAB STUDY... 2 EXPERIMENTS IN THE LAB...

More information

Orifice and Venturi Pipe Flow Meters

Orifice and Venturi Pipe Flow Meters Orifice and Venturi Pipe Flow Meters by Harlan H. Bengtson, PhD, P.E. 1. Introduction Your Course Title Here The flow rate of a fluid flowing in a pipe under pressure is measured for a variety of applications,

More information

Newton's laws of motion

Newton's laws of motion Episode No - 5 Date: 03-04-2017 Faculty: Sunil Deshpande Newton's laws of motion * A plank with a box on it at one end is slowly raised about the other end. As the anle with the horizontal slowly reaches

More information

EXPERIMENT NO: F5. Losses in Piping Systems

EXPERIMENT NO: F5. Losses in Piping Systems SJSU ME115 - THERMAL ENGINEERING LAB EXPERIMENT NO: F5 Losses in Piping Systems Objective One of the most common problems in fluid mechanics is the estimation of pressure loss. It is the objective of this

More information

ME3560 Tentative Schedule Spring 2019

ME3560 Tentative Schedule Spring 2019 ME3560 Tentative Schedule Spring 2019 Week Number Date Lecture Topics Covered Prior to Lecture Read Section Assignment Prep Problems for Prep Probs. Must be Solved by 1 Monday 1/7/2019 1 Introduction to

More information

WATER DISTRIBUTION NETWORKS

WATER DISTRIBUTION NETWORKS WATER DISTRIBUTION NETWORKS CE 370 1 Components of Water Supply System 2 1 Water Distribution System Water distribution systems are designed to adequately satisfy the water requirements for a combinations

More information

LOSSES DUE TO PIPE FITTINGS

LOSSES DUE TO PIPE FITTINGS LOSSES DUE TO PIPE FITTINGS Aim: To determine the losses across the fittings in a pipe network Theory: The resistance to flow in a pipe network causes loss in the pressure head along the flow. The overall

More information

ME3560 Tentative Schedule Fall 2018

ME3560 Tentative Schedule Fall 2018 ME3560 Tentative Schedule Fall 2018 Week Number 1 Wednesday 8/29/2018 1 Date Lecture Topics Covered Introduction to course, syllabus and class policies. Math Review. Differentiation. Prior to Lecture Read

More information

2.2 Differentiation and Integration of Vector-Valued Functions

2.2 Differentiation and Integration of Vector-Valued Functions .. DIFFERENTIATION AND INTEGRATION OF VECTOR-VALUED FUNCTIONS133. Differentiation and Interation of Vector-Valued Functions Simply put, we differentiate and interate vector functions by differentiatin

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

Determining Liquid Capacity 4 th Annual Pipeline Knowledge Retention Chris Sonneborn November 7, 2013

Determining Liquid Capacity 4 th Annual Pipeline Knowledge Retention Chris Sonneborn November 7, 2013 Determining Liquid Capacity 4 th Annual Pipeline Knowledge Retention Chris Sonneborn November 7, 2013 Outline What is important? Liquid Properties Thermal Conditions Hydraulic Gradient Flow Regime in Liquids

More information

Unit C-1: List of Subjects

Unit C-1: List of Subjects Unit C-: List of Subjects The elocity Field The Acceleration Field The Material or Substantial Derivative Steady Flow and Streamlines Fluid Particle in a Flow Field F=ma along a Streamline Bernoulli s

More information

2.The lines that are tangent to the velocity vectors throughout the flow field are called steady flow lines. True or False A. True B.

2.The lines that are tangent to the velocity vectors throughout the flow field are called steady flow lines. True or False A. True B. CHAPTER 03 1. Write Newton's second law of motion. YOUR ANSWER: F = ma 2.The lines that are tangent to the velocity vectors throughout the flow field are called steady flow lines. True or False 3.Streamwise

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

Flow Measurement in Pipes and Ducts COURSE CONTENT

Flow Measurement in Pipes and Ducts COURSE CONTENT Flow Measurement in Pipes and Ducts Dr. Harlan H. Bengtson, P.E. COURSE CONTENT 1. Introduction This course is about measurement of the flow rate of a fluid flowing under pressure in a closed conduit.

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

Answer Key 8 th Grade Geometry Honors Summer 2018 Mathematics Packet

Answer Key 8 th Grade Geometry Honors Summer 2018 Mathematics Packet Answer Ke 8 th Grade Geometr Honors Summer 08 Mathematics Packet [] [B] [] You will never reach point B. [] a. raph 4. raph c. raph d. raph [4] $7.78 [] 4% [6] 6 4 % decrease [7] A population is a roup

More information

Final 1. (25) 2. (10) 3. (10) 4. (10) 5. (10) 6. (10) TOTAL = HW = % MIDTERM = % FINAL = % COURSE GRADE =

Final 1. (25) 2. (10) 3. (10) 4. (10) 5. (10) 6. (10) TOTAL = HW = % MIDTERM = % FINAL = % COURSE GRADE = MAE101B: Advanced Fluid Mechanics Winter Quarter 2017 http://web.eng.ucsd.edu/~sgls/mae101b_2017/ Name: Final This is a three hour open-book exam. Please put your name on the top sheet of the exam. Answer

More information

PIRATE SHIP EXAMPLE REPORT WRITE UP

PIRATE SHIP EXAMPLE REPORT WRITE UP PIRATE SHIP EXAMPE REPORT WRITE UP Title Aim period Pirate Ship investiation To find the relationship between the lenth of a pendulum and its Independent variable the lenth of the pendulum. I will use

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

1/54 Circulation pump, safety valve, expansion vessel

1/54 Circulation pump, safety valve, expansion vessel 1/54 Circulation pump, safety valve, expansion vessel pressure loss efficiency of pump secured heat output safety valve sizing expansion vessel sizing Circulation pump 2/54 similar principle as for heating

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

Pipe Flow Design 1. Results Data

Pipe Flow Design 1. Results Data Pipe Flow Design 1 Results Data Color of Pipe: Velocity in m/sec 1.9 2.2 2.4 2.7 2.9 3.2 Pipe Flow Expert Results Key f = flow in Modelling a 'Tee' fitting: The flow rate through the 'Tee' w ill be different

More information

Ch 14: Feedback Control systems

Ch 14: Feedback Control systems Ch 4: Feedback Control systems Part IV A is concerned with sinle loop control The followin topics are covered in chapter 4: The concept of feedback control Block diaram development Classical feedback controllers

More information

Rate of Flow Quantity of fluid passing through any section (area) per unit time

Rate of Flow Quantity of fluid passing through any section (area) per unit time Kinematics of Fluid Flow Kinematics is the science which deals with study of motion of liquids without considering the forces causing the motion. Rate of Flow Quantity of fluid passing through any section

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

V DD. M 1 M 2 V i2. V o2 R 1 R 2 C C

V DD. M 1 M 2 V i2. V o2 R 1 R 2 C C UNVERSTY OF CALFORNA Collee of Enineerin Department of Electrical Enineerin and Computer Sciences E. Alon Homework #3 Solutions EECS 40 P. Nuzzo Use the EECS40 90nm CMOS process in all home works and projects

More information

Pressure Measurement. Transmitters for basic requirements SITRANS P MPS (submersible sensor) Transmitter for hydrostatic level 2/27

Pressure Measurement. Transmitters for basic requirements SITRANS P MPS (submersible sensor) Transmitter for hydrostatic level 2/27 Overview Siemens AG 011 Function s are for measuring the liquid levels in wells, tanks, channels and dams. Diaphragm p Sensor U const. U + (brown) I EM I -1 (blue) 0, U B s are submersible sensors for

More information

Properties and Definitions Useful constants, properties, and conversions

Properties and Definitions Useful constants, properties, and conversions Properties and Definitions Useful constants, properties, and conversions gc = 32.2 ft/sec 2 [lbm-ft/lbf-sec 2 ] ρwater = 1.96 slugs/ft 3 γwater = 62.4 lb/ft 3 1 ft 3 /sec = 449 gpm 1 mgd = 1.547 ft 3 /sec

More information

APPENDICES. Consider a cylinder of a fluid that is travelling a velocity (v) as shown in Figure 10. Distance S

APPENDICES. Consider a cylinder of a fluid that is travelling a velocity (v) as shown in Figure 10. Distance S 1 PPENDICES 1. Kinetic Energy of a Fluid Consider a cylinder of a fluid that is travelling a velocity (v) as shown in Figure 10. v Distance S Figure 10. This body contains kinetic energy (energy of movement).

More information

Fluids Engineering. Pipeline Systems 2. Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET

Fluids Engineering. Pipeline Systems 2. Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET COURSE NUMBER: ME 423 Fluids Engineering Pipeline Systems 2 Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET 1 SERIES PIPE FLOW WITH PUMP(S) 2 3 4 Colebrook-

More information

5 Shallow water Q-G theory.

5 Shallow water Q-G theory. 5 Shallow water Q-G theory. So far we have discussed the fact that lare scale motions in the extra-tropical atmosphere are close to eostrophic balance i.e. the Rossby number is small. We have examined

More information

PHYS 1443 Section 002 Lecture #24

PHYS 1443 Section 002 Lecture #24 PHYS 443 Section 00 Lecture #4 Monday, Dec. 3, 007 Dr. Jae Yu uoyant Force and Archimedes Principle Flow Rate and Continuity Equation ernoulli s Equation Simple Harmonic Motion Equation of the SHM Simple

More information

CIVE HYDRAULIC ENGINEERING PART II Pierre Julien Colorado State University

CIVE HYDRAULIC ENGINEERING PART II Pierre Julien Colorado State University 1 CIVE 401 - HYDRAULIC ENGINEERING PART II Pierre Julien Colorado State University Problems with and are considered moderate and those with are the longest and most difficult. In 2018 solve the problems

More information

ANALYZE In all three cases (a) (c), the reading on the scale is. w = mg = (11.0 kg) (9.8 m/s 2 ) = 108 N.

ANALYZE In all three cases (a) (c), the reading on the scale is. w = mg = (11.0 kg) (9.8 m/s 2 ) = 108 N. Chapter 5 1. We are only concerned with horizontal forces in this problem (ravity plays no direct role). We take East as the +x direction and North as +y. This calculation is efficiently implemented on

More information

A Multigrid-like Technique for Power Grid Analysis

A Multigrid-like Technique for Power Grid Analysis A Multirid-like Technique for Power Grid Analysis Joseph N. Kozhaya, Sani R. Nassif, and Farid N. Najm 1 Abstract Modern sub-micron VLSI desins include hue power rids that are required to distribute lare

More information

Disclaimer: This lab write-up is not

Disclaimer: This lab write-up is not Disclaimer: This lab write-up is not to be copied, in whole or in part, unless a proper reference is made as to the source. (It is stronly recommended that you use this document only to enerate ideas,

More information

Chapter (6) Energy Equation and Its Applications

Chapter (6) Energy Equation and Its Applications Chapter (6) Energy Equation and Its Applications Bernoulli Equation Bernoulli equation is one of the most useful equations in fluid mechanics and hydraulics. And it s a statement of the principle of conservation

More information

Thermal & Fluids PE Exam Technical Study Guide Errata

Thermal & Fluids PE Exam Technical Study Guide Errata Thermal & Fluids PE Exam Technical Study Guide Errata This product has been updated to incorporate all changes shown in the comments on the webpage and email comments as of October, 30 2017. If you have

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

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics. Physics 8.01x Fall Term 2001 EXAM 1 SOLUTIONS

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics. Physics 8.01x Fall Term 2001 EXAM 1 SOLUTIONS MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.01x Fall Term 2001 EXAM 1 SOLUTIONS Problem 1: We define a vertical coordinate system with positive upwards. The only forces actin

More information

Turbulent Compressible Flow in a Slender Tube

Turbulent Compressible Flow in a Slender Tube Turbulent Compressible Flow in a Slender Tube Kurt O. Lund* 1, and Christine M. Lord 2 1 COMSOL Consultant, 2 Lord Engineering Corp. *Corresponding author: 135 Sixth Street, Del Mar, CA 92014, kurtlund@roadrunner.com

More information

Experiment- To determine the coefficient of impact for vanes. Experiment To determine the coefficient of discharge of an orifice meter.

Experiment- To determine the coefficient of impact for vanes. Experiment To determine the coefficient of discharge of an orifice meter. SUBJECT: FLUID MECHANICS VIVA QUESTIONS (M.E 4 th SEM) Experiment- To determine the coefficient of impact for vanes. Q1. Explain impulse momentum principal. Ans1. Momentum equation is based on Newton s

More information

LECTURE 1 THE CONTENTS OF THIS LECTURE ARE AS FOLLOWS:

LECTURE 1 THE CONTENTS OF THIS LECTURE ARE AS FOLLOWS: LECTURE 1 THE CONTENTS OF THIS LECTURE ARE AS FOLLOWS: 1.0 INTRODUCTION TO FLUID AND BASIC EQUATIONS 2.0 REYNOLDS NUMBER AND CRITICAL VELOCITY 3.0 APPROACH TOWARDS REYNOLDS NUMBER REFERENCES Page 1 of

More information

Get the frictional force from the normal force. Use dynamics to get the normal force.

Get the frictional force from the normal force. Use dynamics to get the normal force. . L F n µ k L =00 t µ k = 0.60 = 0 o = 050 lb F n +y +x x = sin y = cos = µf n Is the initial elocity o the car reater than 30 mph? Approach: Use conseration o enery. System: car Initial time: beore you

More information

Chapter (3) Water Flow in Pipes

Chapter (3) Water Flow in Pipes Chapter (3) Water Flow in Pipes Water Flow in Pipes Bernoulli Equation Recall fluid mechanics course, the Bernoulli equation is: P 1 ρg + v 1 g + z 1 = P ρg + v g + z h P + h T + h L Here, we want to study

More information

Objectives. Conservation of mass principle: Mass Equation The Bernoulli equation Conservation of energy principle: Energy equation

Objectives. Conservation of mass principle: Mass Equation The Bernoulli equation Conservation of energy principle: Energy equation Objectives Conservation of mass principle: Mass Equation The Bernoulli equation Conservation of energy principle: Energy equation Conservation of Mass Conservation of Mass Mass, like energy, is a conserved

More information

FLOW MEASUREMENT IN PIPES EXPERIMENT

FLOW MEASUREMENT IN PIPES EXPERIMENT University of Leicester Engineering Department FLOW MEASUREMENT IN PIPES EXPERIMENT Page 1 FORMAL LABORATORY REPORT Name of the experiment: FLOW MEASUREMENT IN PIPES Author: Apollin nana chaazou Partner

More information

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

EXPERIMENT II - FRICTION LOSS ALONG PIPE AND LOSSES AT PIPE FITTINGS MM 30 FLUID MECHANICS II Prof. Dr. Nuri YÜCEL Yrd. Doç. Dr. Nureddin DİNLER Arş. Gör. Dr. Salih KARAASLAN Arş. Gör. Fatih AKTAŞ EXPERIMENT II - FRICTION LOSS ALONG PIPE AND LOSSES AT PIPE FITTINGS A. Objective:

More information

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. Dynamics of Viscous Fluid Flow in Closed Pipe: Darcy-Weisbach equation for flow in pipes. Major and minor losses in pipe lines. FLUID MECHANICS Dynamics of iscous Fluid Flow in Closed Pipe: Darcy-Weisbach equation for flow in pipes. Major and minor losses in pipe lines. Dr. Mohsin Siddique Assistant Professor Steady Flow Through

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

Expanded Knowledge on Orifice Meter Response to Wet Gas Flows

Expanded Knowledge on Orifice Meter Response to Wet Gas Flows 32 nd International North Sea Flow Measurement Workshop 21-24 October 2014 Expanded Knowlede on Orifice Meter Response to Wet Gas Flows Richard Steven, Colorado Enineerin Experiment Station Inc Josh Kinney,

More information

Orifice and Venturi Pipe Flow Meters

Orifice and Venturi Pipe Flow Meters Orifice and Venturi Pipe Flow Meters For Liquid and Gas Flow by Harlan H. Bengtson, PhD, P.E. 1. Introduction Orifice and Venturi Pipe Flow Meters The flow rate of a fluid flowing in a pipe under pressure

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

Experiment (4): Flow measurement

Experiment (4): Flow measurement Experiment (4): Flow measurement Introduction: The flow measuring apparatus is used to familiarize the students with typical methods of flow measurement of an incompressible fluid and, at the same time

More information

Calibrate Rotameter and Orifice Meter and Explore Reynolds #

Calibrate Rotameter and Orifice Meter and Explore Reynolds # CM3215 Fundamentals of Chemical Engineering Laboratory Calibrate Rotameter and Orifice Meter and Explore Reynolds # Extra features! Professor Faith Department of Chemical Engineering Michigan Technological

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

FLOW MEASUREMENT IN CLOSED CONDUIT

FLOW MEASUREMENT IN CLOSED CONDUIT FLOW MEASUREMENT IN CLOSED CONDUIT Closed conduit flow: It is a flow with boundaries and runs full. As in the case of oen channel flow, the surface is not exosed to atmoshere. Since it runs full it is

More information

COURSE NUMBER: ME 321 Fluid Mechanics I 3 credit hour. Basic Equations in fluid Dynamics

COURSE NUMBER: ME 321 Fluid Mechanics I 3 credit hour. Basic Equations in fluid Dynamics COURSE NUMBER: ME 321 Fluid Mechanics I 3 credit hour Basic Equations in fluid Dynamics Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET 1 Description of Fluid

More information

2/3 Port Valves for Fluid Control Model Selection 1

2/3 Port Valves for Fluid Control Model Selection 1 / Port Valves for Control Model Selection Model Selection For product specifications such as maximum operating pressure differentials and operating temperature ranges, refer to the relevent pages of each

More information

ACCOUNTING FOR FRICTION IN THE BERNOULLI EQUATION FOR FLOW THROUGH PIPES

ACCOUNTING FOR FRICTION IN THE BERNOULLI EQUATION FOR FLOW THROUGH PIPES ACCOUNTING FOR FRICTION IN THE BERNOULLI EQUATION FOR FLOW THROUGH PIPES Some background information first: We have seen that a major limitation of the Bernoulli equation is that it does not account for

More information

Lecture 3 The energy equation

Lecture 3 The energy equation Lecture 3 The energy equation Dr Tim Gough: t.gough@bradford.ac.uk General information Lab groups now assigned Timetable up to week 6 published Is there anyone not yet on the list? Week 3 Week 4 Week 5

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

Atmospheric pressure. 9 ft. 6 ft

Atmospheric pressure. 9 ft. 6 ft Name CEE 4 Final Exam, Aut 00; Answer all questions; 145 points total. Some information that might be helpful is provided below. A Moody diagram is printed on the last page. For water at 0 o C (68 o F):

More information

Frictional Losses in Straight Pipe

Frictional Losses in Straight Pipe 2/2/206 CM325 Fundamentals of Chemical Engineering Laboratory Prelab Preparation for Frictional Losses in Straight Pipe Professor Faith Morrison Department of Chemical Engineering Michigan Technological

More information

Problems of the 9 th International Physics Olympiads (Budapest, Hungary, 1976)

Problems of the 9 th International Physics Olympiads (Budapest, Hungary, 1976) Problems of the 9 th International Physics Olympiads (Budapest, Hunary, 1976) Theoretical problems Problem 1 A hollow sphere of radius R = 0.5 m rotates about a vertical axis throuh its centre with an

More information

ONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.3 HARMONIC MOTION

ONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.3 HARMONIC MOTION ONINE: MATHEMATICS EXTENSION Topic 6 MECHANICS 6.3 HARMONIC MOTION Vibrations or oscillations are motions that repeated more or less reularly in time. The topic is very broad and diverse and covers phenomena

More information

Hydraulic Considerations for Citrus Microirrigation Systems 1

Hydraulic Considerations for Citrus Microirrigation Systems 1 Cir1425 Hydraulic Considerations for Citrus Microirrigation Systems 1 Brian Boman and Sanjay Shukla 2 Introduction Hydraulics is the study of the behavior of liquids as they move through channels or pipes.

More information

Pipe Flow/Friction Factor Calculations using Excel Spreadsheets

Pipe Flow/Friction Factor Calculations using Excel Spreadsheets Pipe Flow/Friction Factor Calculations using Excel Spreadsheets Harlan H. Bengtson, PE, PhD Emeritus Professor of Civil Engineering Southern Illinois University Edwardsville Table of Contents Introduction

More information