Understanding Net Positive Suction Head

Similar documents
TUTORIAL. NPSHA for those who hate that stuffy word. by Jacques Chaurette p. eng. copyright 2006

THE INNER WORKINGS OF A SIPHON Jacques Chaurette p. eng. January 2003

PROCESS ROTATING EQUIPMENT (CENTRIFUGAL PUMPS )

PUMP CONSULTING & TRAINING LLC Joseph R. Askew 1811 Stonecrest Ct. Lakeland, Fl

The Discussion of this exercise covers the following points: Pumps Basic operation of a liquid pump Types of liquid pumps The centrifugal pump.

UNUSUAL ASPECTS OF PUMP SYSTEMS. Jacques Chaurette p. eng. ww.lightmypump.com July 2003

Pump Selection and Sizing (ENGINEERING DESIGN GUIDELINE)

FACHGESPRÄCH 3 NPSH NPSH3. Let us call it: CAVITATION A LOOK UNDER THE HOOD

A centrifugal pump consists of an impeller attached to and rotating with the shaft and a casing that encloses the impeller.

Exercise 4-2. Centrifugal Pumps EXERCISE OBJECTIVE DISCUSSION OUTLINE DISCUSSION. Pumps

Operating Instructions

Exercises The Atmosphere (page 383) 20.2 Atmospheric Pressure (pages )

Dean Pump Self-Priming Chemical Process Pumps

PREVIEW COPY. Table of Contents. Basic Pumping Concepts...3. Maintaining Packing and Seals Lesson Three Maintaining Centrifugal Pumps...

THERMODYNAMICS, HEAT AND MASS TRANSFER TUTORIAL NO: 1 (SPECIFIC VOLUME, PRESSURE AND TEMPERATURE)

Air Eliminators and Combination Air Eliminators Strainers

Pump Primer 1 CEU Training Course $ Plus Tax 48 HOUR RUSH ORDER PROCESSING FEE ADDITIONAL $50.00

PHYS 101 Previous Exam Problems

Gases. Edward Wen, PhD

L 13 Fluid Statics [2] More on fluids. How can a steel boat float. A ship can float in a cup of water! Today s weather

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

N2 Blanketing Valve DST100 / DST200 TYPE INSTRUCTION MANUAL CONTENTS K.S.P.C. General Description Operation. Installation Maintenance

(Refer Slide Time: 2:16)

FLUID DYNAMICS Ch.E-204 Umair Aslam Lecturer Department of Chemical Engineering

Introduction to Pumps

PRESSURE. 7. Fluids 2

Chapter 10 Fluid Power Pneumatics (gas) & Hydraulics (liquid)

Centrifugal Pump Intro

More About Solids, Liquids and Gases ASSIGNMENT

PHYSICS - CLUTCH CH 17: FLUID MECHANICS.

Moving Fluids Concept and Theory

Practical Guide. By Steven T. Taylor, P.E., Member ASHRAE

General Training Pty Ltd

Slide 5 / What is the difference between the pressure on the bottom of a pool and the pressure on the water surface? A ρgh B ρg/h C ρ/gh D gh/ρ

Gases and Pressure. Main Ideas

The following article was authored by Jacques Chaurette of Fluide Design, Inc. ( All rights reserved. - HOW DOES A SIPHON WORK?

AP B Fluids Practice Problems. Multiple Choice. Slide 2 / 43. Slide 1 / 43. Slide 4 / 43. Slide 3 / 43. Slide 6 / 43. Slide 5 / 43

Sizing Pulsation Dampeners Is Critical to Effectiveness

. In an elevator accelerating upward (A) both the elevator accelerating upward (B) the first is equations are valid

Chapter 9 Fluids and Buoyant Force

Pressure is defined as force per unit area. Any fluid can exert a force

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

Phys101 Lectures Fluids I. Key points: Pressure and Pascal s Principle Buoyancy and Archimedes Principle. Ref: 10-1,2,3,4,5,6,7.

Another convenient term is gauge pressure, which is a pressure measured above barometric pressure.

then the work done is, if the force and the displacement are in opposite directions, then the work done is.

Comments on Homework. Quiz. Class 3 - Pressure. Atmospheric Pressure. 2. Gauge vs. Absolute Pressure. 1. Definitions. Temperature conversion

Matter is made up of particles which are in continual random motion Misconception: Only when a substance is in its liquid or gas state do its

Comments on Homework. Class 4 - Pressure. Atmospheric Pressure. Gauge vs. Absolute Pressure. 2. Gauge vs. Absolute Pressure. 1.

Basic Concepts of Chemistry Notes for Students [Chapter 10, page 1] D J Weinkauff - Nerinx Hall High School. Chapter 10 Gases

Valve Sizing Considerations. Steven Hocurscak Metso Automation

2. Materials and Methods

Name Chemistry Pre-AP

Pumping Systems for Landscaping Pumps, Controls and Accessories. Mark Snyder, PE

Bulletin TCR-104 & 109 Filling and adding to the Glycol pressure system

Registration form PUMPS AND MOTORS $ plus tax 48 HOUR RUSH ORDER PROCESSING FEE ADDITIONAL $ Address. City State Zip.


Vacutrans Instructions

1.2 Example 1: A simple hydraulic system

1/4/18. Density. Density. Density

Pressure Measurement

Phys101 Lectures Fluids I. Key points: Pressure and Pascal s Principle Buoyancy and Archimedes Principle. Ref: 10-1,2,3,4,5,6,7.

Chapter 10 Fluids. Which has a greater density? Ch 10: Problem 5. Ch 10: Problem Phases of Matter Density and Specific Gravity

Liquids and Gases. 2/26/2012 Physics 214 Fall

1. All fluids are: A. gases B. liquids C. gases or liquids D. non-metallic E. transparent ans: C

Quick Reference Technical Data

Third measurement MEASUREMENT OF PRESSURE

PERFORMANCE OF GORMAN-RUPP BACKPACK PUMP WITH RESPECT TO SUCTION LIFT. LENGTH OF HOSE AND DISCHARGE HEAD

PHYS:1200 LECTURE 13 FLUIDS (2)

Operating Instructions

Slide 1 / What is the density of an aluminum block with a mass of 4050 kg and volume of 1.5 m 3?

Proper Pump Installation Practices

From and

Fluid Mechanics. Liquids and gases have the ability to flow They are called fluids There are a variety of LAWS that fluids obey

Pump ED 101. Intro to Centrifugal Pumps. Joe Evans, Ph.D. Script for Power Point Presentation. Part 1 Elementary Mechanics & Hydraulics

8.1 Properties of Gases. Goal: Describe the Kinetic Molecular Theory of Gases and the units of measurement used for gases.

Gases Chapter 8. Chapter 8

Gases. Chapter 8. Chapter 8. Gases Properties of Gases. We are surrounded by gases, but we are often

CHAPTER 11: THE GASEOUS STATE

Density and Specific Gravity

Blue River Technologies Port-A-Poly Mixer w/2.5 GPH LMI Pump And Secondary Water Dilution Line INSTALLATION AND OPERATION

Concept of Fluid. Density. Pressure: Pressure in a Fluid. Pascal s principle. Buoyancy. Archimede s Principle. Forces on submerged surfaces

1 Fluids and Pressure

Water Products. Technical Data and Pump Fundamentals TECHNICAL MANUAL TTECHWP R3

Please pick up your midterm if you haven t already. Today: Finish Chapter 13 (Liquids) from last time. Start Chapter 14 (Gases and Plasmas)

ANNEX AMENDMENTS TO THE INTERNATIONAL CODE FOR FIRE SAFETY SYSTEMS (FSS CODE) CHAPTER 15 INERT GAS SYSTEMS

Engineering / Technical Section

Gas Physics Pressure and Flow Topics Covered:

Homework #14, due Wednesday, Nov. 28 before class. Quiz #14, Wednesday November 28 at the beginning of class

Chapter 15 Fluids. Copyright 2010 Pearson Education, Inc.

Copyright, 2005 GPM Hydraulic Consulting, Inc.

SPH 4C Unit 4 Hydraulics and Pneumatic Systems

Unit A-2: List of Subjects

Today: Finish Chapter 13 (Liquids) Start Chapter 14 (Gases and Plasmas)

PULSATION DAMPENER / SUPPRESSOR SERIES PDS PROVIDES MULTIPLE SYSTEM SAFEGUARDS

Old-Exam.Questions-Ch-14 T072 T071

Gases and Pressure SECTION 11.1

Pressure Measurement

ESCONDIDO FIRE DEPT TRAINING MANUAL Section DRIVER OPERATOR Page 1 of 14 Hydraulics Revised

The Kinetic-Molecular Theory of Gases based on the idea that particles are always in motion

The Discussion of this exercise covers the following points: Range with an elevated or suppressed zero Suppressed-zero range Elevated-zero range

Transcription:

Understanding Net Positive Suction Head Atmospheric Pressure Until the early 17 th century air was largely misunderstood. Evangelista Torricelli, an Italian scientist, was one of the first to discover that air, like water, has weight. He once said, We live submerged at the bottom of an ocean of the element air. The weight of this ocean of air exerts a force on the Earth s surface called atmospheric pressure. Torricelli went on to develop the mercury barometer which now allowed for quantifiable measurement of this pressure. A mercury barometer (figure 1) uses a complete vacuum at the top of a glass tube to draw mercury up the tube. The weight of the column of mercury is equal to the weight of the air outside the tube Figure 1 Operation of a mercury barometer (the atmospheric pressure). For this reason, atmospheric pressure is often measured in mmhg or inhg, corresponding to the height of the mercury column. This atmospheric pressure controls the weather, enables you to breathe, and is the cornerstone of pump operation. Pump Operation When asked how a pump operates, most reply that it sucks. While not a false statement, it s easy to see why so many pump operators still struggle with pump problems. Fluid flows from areas of high pressure to areas of low pressure. Pumps operate by creating low pressure at the inlet which allows the liquid to be pushed into the pump by atmospheric or head pressure (pressure due to the liquid s surface being above the centerline of the pump). Consider placing a pump at the top of the mercury barometer above: Even with a perfect vacuum at the pump inlet, atmospheric pressure limits how high the pump can lift the liquid. With liquids lighter than mercury, this lift height can increase, but there s still a physical limit to pump operation based on pressure external to the pump. This limit is the key consideration for Net Positive Suction Head. Net Positive Suction Head (NPSH) NPSH can be defined as two parts: NPSH Available (NPSH A ): The absolute pressure at the suction port of the pump. AND NPSH Required (NPSH R ): The minimum pressure required at the suction port of the pump to keep the pump from cavitating. NPSH A is a function of your system and must be calculated, whereas NPSH R is a function of the pump and must be provided by the pump manufacturer. NPSH A MUST be greater than NPSH R for the pump system to operate without cavitating. Put another way, you must have more suction side pressure available than the pump requires.

Vapor Pressure and Cavitation To understand Cavitation, you must first understand vapor pressure. Vapor pressure is the pressure required to boil a liquid at a given temperature. Soda water is a good example of a high vapor pressure liquid. Even at room temperature the carbon dioxide entrained in the soda is released. In a closed container, the soda is pressurized, keeping Vapor Pressure the vapor entrained. 25 Temperature affects vapor pressure as well 20 (figure 2). A chilled bottle of soda has a lower vapor 15 pressure than a warm bottle (as anyone who s 10 opened a warm bottle of root beer has probably 5 0 already figured out). Water, as another example, 40 60 80 100 120 140 160 will not boil at room temperature since its vapor Temperature ( F) 180 200 212 pressure is lower than the surrounding atmospheric Water Soda pressure. But, raise the water s temperature t 212 F and the vapors are released because at that increased temperature the vapor pressure is greater than the atmospheric pressure. Vapor Pressure (psia) o Figure 2 Vapor Pressure versus Temperature Pump cavitation occurs when the pressure in the pump inlet drops below the vapor pressure of the liquid. Vapor bubbles form at the inlet of the pump and are moved to the discharge of the pump where they collapse, often taking small pieces of the pump with them. Cavitation is often characterized by: Loud noise often described as a grinding or marbles in the pump Loss of capacity (bubbles are now taking up space where liquid should be) Pitting damage to parts as material is removed by the collapsing bubbles Noise is a nuisance and lower flows will slow your process, but pitting damage will ultimately decrease the life of the pump. Figure 3 shows an idler gear from an internal gear pump that has suffered cavitation (note the pitting along the roots and the tips of the gear). Often this is mistaken for corrosion, but unlike corrosion, the pitting is isolated within the pump (corrosion attacks the pump material throughout). Figure 3 An idler gear which has pitting due to caviation Calculating NPSH A No engineer wants to be responsible for installing a noisy, slow, damaged pump. It s critical to get the NPSH R value from the pump manufacturer AND to insure that your NPSH A pressure will be adequate to cover that requirement.

The formula for calculating NPSH A : NPSH A = H A ± H Z - H F + H V - H VP Term Definition Notes The absolute pressure on the surface of the Typically atmospheric pressure (vented supply tank), but can be different for closed tanks. liquid in the supply tank Don t forget that altitude affects atmospheric pressure H A (H A in Denver, CO will be lower than in Miami, FL). Always positive (may be low, but even vacuum H Z H F H V H VP The vertical distance between the surface of the liquid in the supply tank and the centerline of the pump Friction losses in the suction piping Velocity head at the pump suction port Absolute vapor pressure of the liquid at the pumping temperature vessels are at a positive absolute pressure) Can be positive when liquid level is above the centerline of the pump (called static head) Can be negative when liquid level is below the centerline of the pump (called suction lift) Always be sure to use the lowest liquid level allowed in the tank. Piping and fittings act as a restriction, working against liquid as it flows towards the pump inlet. Often not included as it s normally quite small. Must be subtracted in the end to make sure that the inlet pressure stays above the vapor pressure. Remember, as temperature goes up, so does the vapor pressure. All too often, these calculations are faulted by a simple unit discrepancy. Most often, it s easiest to work with feet of liquid. Adding the liquid name helps to be clear as well (feet of water, feet of gasoline, feet of ammonia, etc.). Also, make sure to include the specific gravity of the liquid. As discussed above, a 10 column of mercury and a 10 column of water exert very different pressures at their base. Solving NPSH Problems Let s be honest, many of us don t begin reading documents like this until after there s a problem. It would be wonderful if proper NPSH calculations had been run for every pump installation, but for thousands of cavitating pumps out there it s not too late. The first step is to diagnose the pump. As discussed above, noise, capacity loss, and pitting are three major indicators, but direct measurement not only helps to confirm your suspicions, but also let s you know what your true NPSH A is. Install a compound gauge (one that measures both vacuum pressures as well as light positive gauge pressures) (figure 4) into the suction port of the pump (or as close as you can in the suction piping). When the pump is running, the reading from this gauge will be equal to your NPSH A, less vapor pressure. If after subtracting vapor pressure this value is less than the pump s NPSH R, you have confirmed that this is a cavitation problem. Figure 4 A Compound Pressure Gauge

Diagnosing the problem is the easy part. Fixing the problem is usually much more difficult. Step by step, look at which of the NPSH A factors can be improved: Term H A H Z H F H VP Improvements Though you may use external pressure to feed the pump, this is usually atmospheric pressure and outside of your control. If the pump only starts to cavitate near the end of emptying the supply tank, you may consider allowing for a higher level of liquid to remain. Raising the tank, or lowering the pump helps, but may not be feasible. This factor is often the easiest to change. You can cut your frictional losses by: - Increasing the size of the suction piping or decreasing the length - Reducing obstructions such as valves, strainers, and other fittings. - For thicker liquids, heat tracing the lines will help to reduce the viscous losses - Hoses and corroded pipes have high losses. Consider replacing with new pipe Control the temperature to make sure the vapor pressure doesn t get too high. Often tanks and pipes holding high vapor pressure liquids are painted light colors to avoid the sun heating them and raising the vapor pressure. If system changes aren t feasible or aren t adequate to increase the NPSH A, consult with the pump manufacturer about reducing the NPSH R. In the case of a positive displacement pump, this will likely mean going with a larger model and slowing it down. For example, a gear pump generating 100 GPM at 780 RPM has an NPSH R of 9.1 feet of water. By switching to a larger pump running at 350 RPM to generate the same 100 GPM, the NPSH R drops to 3.8 feet of water. Slowing the pump allows more time for the tooth cavities to fill, allowing the pump to operate without cavitating even at low suction pressures (figure 5). Figure 5 Internal Gear Pump Just the Beginning Hopefully you now feel more knowledgeable regarding NPSH and its importance when selecting a pump. A basic understanding can go a long way in identifying potential problems before they occur. Lifting liquids from underground tanks or rail cars, pulling thick liquids long distances or through hoses, handling high vapor pressure liquids such as LP gas or alcohol these are just a few example cases of applications which pose the maximum risk of failure for the engineer who does not understand or account for NPSH.

The UK s leading pump specialist OFFICIAL DISTRIBUTORS FOR: Viking Gear Pumps Liquiflo Gear Pumps Finish Thompson Drum & Centrifugal Pumps Codip Air Operated PTFE Diaphragm Pumps Micropump Gear Pumps HNP Gear Pumps Hydra-Cell High Pressure Diaphragm Pumps M Pumps, Centrifugal, Turbine and Vane Pumps Ismatec Peristaltic Pumps Fluid Metering Piston Pumps Michael Smith Engineers Tel: 0800 316 7891 www.michael-smith-engineers.co.uk Info@michael-smith-engineers.co.uk