1. General and basic pump knowledge
Pump theory
General and basic pump knowledge
Håkan Ekstrand/Tapflo AB/2012

2. Håkan Ekstrand/Tapflo AB/2012
Pump theory
Pump classification
Pump selection
Pump theory
Affinity laws
System curves
Cavitation
NPSH
Håkan Ekstrand/Tapflo AB/2012

3. Håkan Ekstrand/Tapflo AB/2012
Pump classification
Centrifugal pumps
The centrifugal pump produce a head and a flow by increasing the velocity of the liquid through the machine with the help of a rotating vane impeller. 
Positive displacement pumps
The positive displacement pump operates by alternating of filling a cavity and then displacing a given volume of liquid. The positive displacement pump delivers a constant volume of liquid against varying discharge pressure or head.
Håkan Ekstrand/Tapflo AB/2012

4. Håkan Ekstrand/Tapflo AB/2012
Pump classification
Centrifugal pumps
End suction pump
In-line pump
Double suction pump
Vertical multistage pump
Horizontal multistage pump
Submersible pumps
Self-priming pumps
Axial-flow pumps
Positive displacement pumps
Reciprocating pumps
Piston pumps
Diaphragm pump
Rotating pumps
Gear pump
Lobe pump
Screw pump
Håkan Ekstrand/Tapflo AB/2012

5. Selecting between C or PD Pumps
Flow rate and pressure head
The Centrifugal Pump has varying flow depending on the system pressure or head
The Positive Displacement Pump has more or less a constant flow regardless of the system pressure or head. Positive Displacement pumps generally gives more pressure than Centrifugal Pump's.
Capacity and Viscosity
In the Centrifugal Pump the flow is reduced when the viscosity is increased
A Centrifugal Pump becomes very inefficient at even modest viscosity.
In the Positive Displacement Pump the flow is increased when viscosity is increased
Liquids with high viscosity fills the clearances of a Positive Displacement Pump causing a higher volumetric efficiency and a Positive Displacement Pump is better suited for high viscosity applications.
Mechanical Efficiency
Changing the system pressure or head has little or no effect on the flow rate in the Positive Displacement Pump
Changing the system pressure or head has a dramatic effect on the flow rate in the Centrifugal Pump
Net Positive Suction Head - NPSH
In a Centrifugal Pump, NPSH varies as a function of flow determined by pressure
In a Positive Displacement Pump, NPSH varies as a function of flow determined by speed. Reducing the speed of the Positive Displacement Pump pump, reduces the NPSH
Håkan Ekstrand/Tapflo AB/2012

6. Håkan Ekstrand/Tapflo AB/2012
Centrifugal pumps
A centrifugal pump converts the input power to kinetic energy in the liquid by accelerating the liquid by a revolving device - an impeller.
The energy created by the pump is kinetic energy according the Bernoulli Equation. The energy transferred to the liquid corresponds to the velocity at the edge or vane tip of the impeller. The faster the impeller revolves or the bigger the impeller is, the higher will the velocity of the liquid energy transferred to the liquid be. This is described by the Affinity Laws.
Pressure and Head
If the discharge of a centrifugal pump is pointed straight up into the air the fluid will pumped to a certain height -  or head - called the shut off head.
A pump does not create pressure, it only creates flow. Pressure is a measurement of the resistance to flow.
In Newtonian fluids (non-viscous liquids like water or gasoline) the term head is used to measure the kinetic energy which a pump creates.
Head is a measurement of the height of the liquid column the pump creates from the kinetic energy the pump gives to the liquid. 
The main reason for using head instead of pressure to measure a centrifugal pump's energy is that the pressure from a pump will change if the specific gravity (weight) of the liquid changes, but the head will not.
The pump's performance on any Newtonian fluid can always be described by using the term head. 
Håkan Ekstrand/Tapflo AB/2012

7. Håkan Ekstrand/Tapflo AB/2012
Centrifugal pumps
Different Types of Pump Head
Total Static Head -  Total head when the pump is not running
Total Dynamic Head (Total System Head) - Total head when the pump is running
Static Suction Head - Head on the suction side, with pump off, if the head is higher than the pump impeller
Static Suction Lift - Head on the suction side, with pump off, if the head is lower than the pump impeller
Static Discharge Head - Head on discharge side of pump with the pump off
Dynamic Suction Head/Lift - Head on suction side of pump with pump on
Dynamic Discharge Head - Head on discharge side of pump with pump on
The head is measured in either feet or meters and can be converted to common units for pressure as psi or bar.
It is important to understand that the pump will pump all fluids to the same height if the shaft is turning at the same rpm. 
The only difference between the fluids is the amount of power it takes to get the shaft to the proper rpm. The higher the specific gravity of the fluid the more power is required.
Håkan Ekstrand/Tapflo AB/2012

8. Håkan Ekstrand/Tapflo AB/2012
Affinity laws
The Affinity Laws of centrifugal pumps or fans can be used to express the influence on volume capacity, head (pressure) or power consumption of a pump or fan due to
change in speed of wheel - revolutions per minute (rpm)
geometrically similarity - change in impeller diameter
Volume Capacity
The volume capacity of a fan or pump can be expressed like
q1 / q2 = (n1 / n2)(d1 / d2)3 (1)
where
q = volume flow capacity (m3/s, gpm, cfm, ..)
n = wheel velocity - revolution per minute - (rpm)
d = wheel diameter
Head or Pressure
The head or pressure of a fan or pump can be expressed like
dp1 / dp2 = (n1 / n2)2 (d1 / d2)2 (2)
dp = head or pressure  (m, ft, Pa, psi, ..)
Power
The power consumption of a fan or pump can be expressed as
P1 / P2 = (n1 / n2)3 (d1 / d2)5 (3)
P = power (W, bhp, ..)
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9. Håkan Ekstrand/Tapflo AB/2012
Cavitation
What is Cavitation?
Cavitation may occur when the local static pressure in a fluid reach a level below the vapor pressure of the liquid at the actual temperature.
According to the Bernoulli Equation this may happen when the fluid accelerates in a control valve or around a pump impeller.
The vaporization itself does not cause the damage - the damage happens when the vapor almost immediately collapses after evaporation when the velocity is decreased and pressure increased.
Avoiding Cavitation
Cavitation can in general be avoided by
increasing the distance between the actual local static pressure in the fluid - and the vapor pressure of the fluid at the actual temperature
This can be done by:
reengineering components initiating high speed velocities and low static pressures
increasing the total or local static pressure in the system
reducing the temperature of the fluid
Håkan Ekstrand/Tapflo AB/2012

10. Håkan Ekstrand/Tapflo AB/2012
Cavitation
Reengineering of Components Initiating High Speed Velocity and Low Static Pressure
Cavitation and damage can be avoided by using special components designed for the actual rough conditions.
Conditions as huge pressure drops can - with limitations - be handled by Multi Stage Control Valves
Difficult pumping conditions - with fluid temperatures close to the vaporization temperature - can be handled with a special pump - working after an other principle than the centrifugal pump.
Increasing the Total or Local Pressure in the System
By increasing the total or local pressure in the system, the distance between the static pressure and the vaporization pressure is increased and vaporization and cavitation may be avoided.
The ratio between static pressure and the vaporization pressure, an indication of the possibility of vaporization, is often expressed by the Cavitation Number.
Unfortunately it may not always be possible to increase the total static pressure due to system classifications or other limitations. Local static pressure in the component may then be increased by lowering the component in the system. Control valves and pumps should in general be positioned in the lowest part of the systems to maximize the static head.
Reducing the Temperature of the Fluid
The vaporization pressure is highly dependable of the fluid temperature
Håkan Ekstrand/Tapflo AB/2012

11. Håkan Ekstrand/Tapflo AB/2012
System curve
A fluid flow system can in general be characterized with the System Curve
Håkan Ekstrand/Tapflo AB/2012

12. Pump performance curve
The pump curve describes the relation between flowrate and head for the actual pump. Other important information for proper pump selection is also included – efficiency curves, NPSHr curve, pump curves for several impeller diameters and different speeds, and power consumption.
Håkan Ekstrand/Tapflo AB/2012

13. Håkan Ekstrand/Tapflo AB/2012
Selection of Pump
A pump can be selected by combining the System Curve and the Pump Curve:
Håkan Ekstrand/Tapflo AB/2012

14. NPSH - Net Positive Suction Head
Low pressure at the suction side of a pump can encounter the fluid to start boiling with
reduced efficiency
cavitation
damage of the pump as a result.
To characterize the potential for boiling and cavitation, the difference between the total head on the suction side of the pump - close to the impeller, and the liquid vapor pressure at the actual temperature may be used
The Net Positive Suction Head - NPSH - can be expressed as the difference between the Suction Head and the Liquids Vapor Head
Håkan Ekstrand/Tapflo AB/2012

15. Håkan Ekstrand/Tapflo AB/2012
NPSH
Required NPSH - NPSHr
The required NPSH - NPSHr - is the NPSH that must be exceeded to avoid vaporization and cavitation in the impellers eye. The NPSHr is always higher than the theoretical NPSH due to head loss in the suction pipe and the pump casing, and local velocity acceleration and pressure decrease on the impeller surface.
NPSHr is in general determined experimentally by the pump manufacturer and a part of the pump performance curves documentation.
The required NPSHr increases with the square of increased capacity.
Available NPSH - NPSHa
The available NPSH - HPSHa - is the NPSH available for a particular system
must be determined during design and construction of the system,
or determined experimentally on the actual physical system.
Håkan Ekstrand/Tapflo AB/2012

16. Håkan Ekstrand/Tapflo AB/2012
NPSH
Håkan Ekstrand/Tapflo AB/2012

17. Pumps in Parallel or Serial Connection
Pumps in Serial
Heads Added
When two (or more) pumps are arranged in serial, their resulting pump performance curve is obtained by adding heads at the same flowrate.
Pumps in Parallel
Flow Rate Added
When two or more pumps are arranged in parallel, their resulting performance curve is obtained by adding their flowrates at the same head.
Håkan Ekstrand/Tapflo AB/2012

18. Pumps in Parallel or Serial Connection
Håkan Ekstrand/Tapflo AB/2012

19. Density, Specific Weight, Specific Gravity
Density is defined as an objects mass per unit volume. Mass is a property.
The density can be expressed as
ρ = m / V (1)
Where
ρ = density (kg/m3)
m = mass (kg)
V = volume (m3)
The SI units for density are kg/m3. The imperial (BG) units are lb/ft3 (slugs/ft3).
The higher the density, the tighter the particles are packed inside the substance.
Density is a physical property constant at a given temperature and density can help to identify a substance.
Håkan Ekstrand/Tapflo AB/2012

20. Density, Specific Weight, Specific Gravity
Specific Weight is defined as weight per unit volume. Weight is a force.
Specific Weight can be expressed as
γ = ρ g (2)
where
γ = specific weight (kN/m3)
g = acceleration of gravity (m/s2)
The SI-units of specific weight are kN/m3. The imperial units are lb/ft3. The local acceleration g is under normal conditions m/s2 in SI-units and ft/s2 in imperial units.
Håkan Ekstrand/Tapflo AB/2012

21. Density, Specific Weight, Specific Gravity
The Specific Gravity - SG - is a dimensionless unit defined as the ratio of density of the material to the density of water at a specified temperature. Specific Gravity can be expressed as
SG = = ρ / ρH2O (3)
where
SG = specific gravity
ρ = density of fluid (kg/m3)
ρH2O = density of water (kg/m3)
It is common to use the density of water at 4 oC (39oF) as reference - at this point the density of water is at the highest.
Thermal Properties of Water Density, Freezing temperature, Boiling temperature, Latent heat of melting, Latent heat of evaporation, Critical temperature ...
Since Specific Weight is dimensionless it has the same value in the metric SI system as in the imperial English system (BG). At the reference point the Specific Gravity has same numerically value as density.
Håkan Ekstrand/Tapflo AB/2012

22. Dynamic, Absolute and Kinematic Viscosity
The viscosity of a fluid is an important property in the analysis of liquid behavior and fluid motion near solid boundaries.
The viscosity is the fluid resistance to shear or flow and is a measure of the adhesive/cohesive or frictional fluid property.
The resistance is caused by intermolecular friction exerted when layers of fluids attempts to slide by an other.
The knowledge of viscosity is needed for proper design of required temperatures for storage, pumping or injection of fluids.
Common used units for viscosity are
CentiPoises (cp) = CentiStokes (cSt) x Density
SSU1 = Centistokes (cSt) * 4.55
Degree Engler1 * 7.45 = Centistokes (cSt)
Seconds Redwood = Centistokes (cSt)
Håkan Ekstrand/Tapflo AB/2012

23. Dynamic, Absolute and Kinematic Viscosity
There are two related measures of fluid viscosity - known
as dynamic (or absolute) and kinematic viscosity.
Dynamic (absolute) Viscosity
is the tangential force per unit area required to move one horizontal plane with respect to the other at unit velocity when maintained a unit distance apart by the fluid.
Kinematic Viscosity
is the ratio of absolute or dynamic viscosity to density - a quantity in which no force is involved
Håkan Ekstrand/Tapflo AB/2012

24. Håkan Ekstrand/Tapflo AB/2012
Liquid behaviour
Newtonian Fluids
Fluids for which the shearing stress is linearly related to the rate of shearing strain are designated as Newtonian Fluids.
Newtonian materials are referred to as true liquids since their viscosity or consistency is not affected by shear such as agitation or pumping at a constant temperature. Fortunately most common fluids, both liquids and gases, are Newtonian. Water and oils are examples of Newtonian liquids.
Thixotropic Fluids
Shear Thinning Fluids or Thixotropic Fluids reduce their viscosity as agitation or pressure is increased at a constant temperature. Ketchup and mayonnaise are examples of thixotropic materials. They appear thick or viscous but are possible to pump quite easily.
Dilatant Fluids
Shear Thickening Fluids or Dilatant Fluids increase their viscosity with agitation. Some of these liquids can become almost solid within a pump or pipe line. With agitation, cream becomes butter and Candy compounds, clay slurries and similar heavily filled liquids do the same thing.
Bingham Plastic Fluids
Bingham Plastic Fluids have a yield value which must be exceeded before it will start to flow like a fluid. From that point the viscosity will decrease with increase of agitation. Toothpaste, mayonnaise and tomato catsup are examples of such products.
Håkan Ekstrand/Tapflo AB/2012