PumpTech Customer Education

Similar documents
Pressure and Flow Characteristics

Chapter Four Hydraulic Machines

Chapter Four Hydraulic Machines

CHAPTER EIGHT P U M P I N G O F L I Q U I D S

Pumping Stations Design For Infrastructure Master Program Engineering Faculty-IUG

COURSE CODE : 3072 COURSE CATEGORY : B PERIODS/ WEEK : 5 PERIODS/ SEMESTER : 75 CREDIT : 5 TIME SCHEDULE

Department of Energy Fundamentals Handbook. THERMODYNAMICS, HEAT TRANSFER, AND FLUID FLOW, Module 3 Fluid Flow

Applied Fluid Mechanics

Lecture 3 The energy equation

EXPERIMENT No.1 FLOW MEASUREMENT BY ORIFICEMETER

Chapter (6) Energy Equation and Its Applications

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

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

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

Fluid Mechanics II 3 credit hour. Fluid flow through pipes-minor losses

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

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 3 BASIC EQUATIONS IN FLUID MECHANICS NOOR ALIZA AHMAD

vector H. If O is the point about which moments are desired, the angular moment about O is given:

Chemical Engineering 3P04 Process Control Tutorial # 1 Learning goals

Mechanical Engineering Programme of Study

Hydraulic (Piezometric) Grade Lines (HGL) and

WATER DISTRIBUTION NETWORKS

Introduction to Fluid Machines, and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

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

New Website: M P E il Add. Mr. Peterson s Address:

Fluid Mechanics. du dy

Basic Fluid Mechanics

Chapter 4 DYNAMICS OF FLUID FLOW

For example an empty bucket weighs 2.0kg. After 7 seconds of collecting water the bucket weighs 8.0kg, then:

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

Properties and Definitions Useful constants, properties, and conversions

1-Reynold s Experiment

THE APPLICATION OF THERMODYNAMICS TO PUMP SYSTEMS

PUMP PERFORMANCE MEASUREMENTS Jacques Chaurette p. eng. April 2003

CONCEPTS AND DEFINITIONS. Prepared by Engr. John Paul Timola

Exam #2: Fluid Kinematics and Conservation Laws April 13, 2016, 7:00 p.m. 8:40 p.m. in CE 118

FLOW MEASUREMENT IN PIPES EXPERIMENT

Thermal & Fluids PE Exam Technical Study Guide Errata

5 ENERGY EQUATION OF FLUID MOTION

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

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

PART II. Fluid Mechanics Pressure. Fluid Mechanics Pressure. Fluid Mechanics Specific Gravity. Some applications of fluid mechanics

Nicholas J. Giordano. Chapter 10 Fluids

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

PROPERTIES OF FLUIDS

Pipe Flow. Lecture 17

Therefore, the control volume in this case can be treated as a solid body, with a net force or thrust of. bm # V

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

Theory of turbo machine Effect of Blade Configuration on Characteristics of Centrifugal machines. Unit 2 (Potters & Wiggert Sec

CHAPTER THREE FLUID MECHANICS

Homework 6. Solution 1. r ( V jet sin( θ) + ω r) ( ρ Q r) Vjet

FLOW FRICTION CHARACTERISTICS OF CONCRETE PRESSURE PIPE

Pressure Head: Pressure head is the height of a column of water that would exert a unit pressure equal to the pressure of the water.

Piping Systems and Flow Analysis (Chapter 3)

Guidelines for the Installation of SYGEF Pipes, Fittings and Valves

Experiment (4): Flow measurement

June 9, Phosphate Conference Clearwater Convention June Abstract:

Experimental and Numerical Investigations of the Effect of Net Positive Suction Head on Water Hammer In Pipeline Systems

BASIC EQUATION. Rotational speed. u = linear velocity in m/s r = radius in m ω = angular velocity in rad/s D = diameter in m N = rotation per minute

Lesson 6 Review of fundamentals: Fluid flow

Introduction to Fluid Machines and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

S.E. (Mech.) (First Sem.) EXAMINATION, (Common to Mech/Sandwich) FLUID MECHANICS (2008 PATTERN) Time : Three Hours Maximum Marks : 100

LEAKLESS COOLING SYSTEM V.2 PRESSURE DROP CALCULATIONS AND ASSUMPTIONS

Pipe Flow Design 1. Results Data

CEE 3310 Control Volume Analysis, Oct. 7, D Steady State Head Form of the Energy Equation P. P 2g + z h f + h p h s.

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

Chapter (3) Water Flow in Pipes

Useful concepts associated with the Bernoulli equation. Dynamic

ACCOUNTING FOR FRICTION IN THE BERNOULLI EQUATION FOR FLOW THROUGH PIPES

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

Hydraulics and hydrology

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

Mass of fluid leaving per unit time

MAKING MEASUREMENTS. I walk at a rate of paces per...or...my pace =

Introduction to Fluid Machines and Compressible Flow Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

IJREAS Volume 2, Issue 2 (February 2012) ISSN:

Angular momentum equation

Lecture on Francis Turbine. by Dr. Shibayan Sarkar Department of Mechanical Engg Indian Institute of Technology (ISM), Dhanbad

Introduction to Fluid Machines (Lectures 49 to 53)

mywbut.com Hydraulic Turbines

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

Chapter 9. Solids and Fluids. 1. Introduction. 2. Fluids at Rest. 3. Fluid Motion

Design optimization of a centrifugal pump impeller and volute using computational fluid dynamics

EXPERIMENT NO: F5. Losses in Piping Systems

Theory of turbo machinery / Turbomaskinernas teori. Dixon, chapter 7. Centrifugal Pumps, Fans and Compressors

Chapter 11. Fluids. continued

Lecture 22. Mechanical Energy Balance

Department of Civil and Environmental Engineering CVNG 1001: Mechanics of Fluids

SKM DRILLING ENGINEERING. Chapter 3 - Drilling Hydraulics

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

Basics of fluid flow. Types of flow. Fluid Ideal/Real Compressible/Incompressible

CHAPTER TWO CENTRIFUGAL PUMPS 2.1 Energy Transfer In Turbo Machines

A Model Answer for. Problem Set #7

40 N 40 N. Direction of travel

Design of Monoblock Centrifugal Pump Impeller

Physics 220: Classical Mechanics

Centrifugal Machines Table of Contents

Hydraulic Considerations for Citrus Microirrigation Systems 1

Reference : McCabe, W.L. Smith J.C. & Harriett P., Unit Operations of Chemical

Transcription:

PumpTech Customer Education http://www.pumptechnw.com Bellevue Moses Lake Canby

PumpTech Product Lines UL Listed Packaged Systems

Two full time Mechanical Engineers Licensed in OR, WA & ID SolidWorks & E-Drawings Viewer AutoCad Compatible Drawings All Systems UL QCZJ Listed Designed to HI Standards

Manufacturing Facility Canby, OR

Installation, Maintenance & Repair 9 Full Time Service Technicians 3 Full Service Shops 6 Service Trucks 23 Ton Crane Truck 8 Ton Crane Truck 3 Ton Crane Truck 2 Ton Flatbed & Trailer 1 Ton Flatbed & Trailer

Pipeline newsletter@pumptechnw.com

Pump Ed 101 Joe Evans, Ph.D http://www.pumped101.com http://www.pump-zone.com Velocity Head

Hint * Centrifugal Pump Impeller Discharge Suction Cutwater Volute What Type of Energy is Added by the Impeller?

* Centrifugal Force It is defined as center fleeing

* Centrifugal Force Instead it actually moves in the same direction it was traveling at the exact instant it is released. When an object is traveling in a circle, it is actually moving in a straight line at any single point in time.

So, How Does It Work? * 1 Rotation of the impeller forces water from its entry point, at the eye, into its vanes. 2 Water moving through the vanes creates a partial vacuum at the eye allowing atmospheric, or some other outside pressure, to force more water into the eye. 3 As water travels through the vanes, it gains rotational velocity (kinetic energy) and reaches its maximum velocity just as it exits the vanes. 4 Upon exiting the vanes, water enters the volute where its kinetic energy of motion is transformed into pressure energy.

Linear versus Rotational Motion * Speed = d / t Rotational Speed (w) = rotations / t Linear Speed (v) radius (r) x w

* Linear Velocity in a Rotational Frame of Reference On the disc to the right there are two points, one at 6 from its center and one at 12. The circle described at 6 has a circumference of 37.7 and the one at 12 a circumference of 75.4. 6 12 At a speed of one rotation per second a point 12 from the center will travel twice the distance of a point that is 6 from the center. Therefore its velocity is twice as great. v = C x w

Water Energy * Water Can Possess Three Forms of Hydraulic Energy Potential Energy Due to Elevation Kinetic Energy Due to Velocity Pressure Energy Due to Weight (force) These Three Forms of Energy Must Live In Harmony Conservation of Energy

* Conservation of Energy Bernoulli s theorem states that, during steady flow, the energy at any point in a conduit is the sum of the velocity head, pressure head, and elevation head. It also states that this sum will remain constant if there are no losses. Daniel Bernoulli 1700-1782 H = v + p + z = Constant 50 PSI 50 PSI 48 PSI 100 GPM

Daniel Bernoulli Hydrodynamica - 1738 * Energy = v + P + z = Constant

Energy = v + P + z = Constant * Piezometer Measurement

Energy = v + P + z = Constant * Piezometer & Pitot Tube Measurement

Energy = v + P + z = Constant *

Total Dynamic Head What is the Total Head produced by a centrifugal pump? Total Head

Total Dynamic Head Total Dynamic Head H = h d - h s Where: h d = discharge head h s = suction head Total Suction Head h s = ± h gs + h vs ± Z s Total Discharge Head h d = h gd + h vd ± Z d Where: h g = gauge head h v = velocity head Z = gauge distance above or below datum Total Head

Velocity Head What is the effect of velocity? KE = 1/2mv 2 Falling Body Equation Velocity Head Equation V 2 = 2gh h = V 2 / 2g At a Velocity of 8 ft/sec h = 1 Total Head

The Performance Curve BEBOP BEP

Pump Testing 247.2 258.3 TDH Error 4.7% TDH Error 0.6% 3X4 End Suction - 650 GPM Velocity 3 = 28.2 ft/sec Velocity 5 = 10.4 ft/sec h v = V 2 / 2g 3 Section h v = 12.4 ft 5 Section h v = 1.7 ft Total Head Actual 3 Pressure = 112.4 PSI (259.6 ft). Actual 5 Pressure = 112.5 PSI (260 ft)

* Pump Testing Lift Station Pump 650 GPM @ 25 (10.8 PSI) 4 Discharge Piping 10 ft Gauge Reading at Valve Box = 6.6 (2.8 PSI) Corrected for Friction = 10.8 (4.7 PSI) Corrected for Elevation = 20.8 (9 PSI) Corrected for Velocity Head (v = 16.4 ft/sec) = 25 (10.8 PSI) TDH Error Ignoring Velocity Head = 19%

*

*

*

*

*

Pump Ed 101 Joe Evans, Ph.D http://www.pumptechnw.com http://www.pumped101.com http://www.pump-zone.com Velocity Head