READING
CENTRIFUGAL PUMP CURVES
(Refer to Fig.2 below and its notes)
Centrifugal
pump performance is represented by multiple curves indicating
either:
The curve
consists of a line starting at "shut head" (zero flow on bottom
scale / maximum head on left scale). The line continues to the
right, with head reducing and flow increasing until the "end
of curve" is reached, (this is often outside the recommended
operating range of the pump). Flow
and head are linked, one can not be changed without varying
the other. The relationship between them is locked until wear
or blockages change the pump characteristics.
The pump
can not develop pressure unless the system creates back pressure
(ie: Static (vertical height), and /or friction loss). Therefore
the performance of a pump can not be estimated without knowing
full details of the system in which it will be operating.
Following
is fig.2 and its notes (NOTE: text
colours relate
to colours used
in fig.2):
Best
efficiency point
Various
performance curves, may indicate various impeller diameters,
or speeds.
Curves
showing power absorbed by pump (may be a separate line),
read power at operating point, see note 1.
Recommended operating
range.
Nett positive suction head
required by the pump (lines may be shown intersecting
pump curve)- should be 1m less than NPSH(a)
The points referred to as "shut
head: and "end of curve" which are outside pump operating
range.
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The
circled numbers indicate the following for bottom
curve (ie: smallest diameter impeller
or slowest speed curve shown):
1. Maximum recommended head.
2. Minimum recommended head.
3. Minimum recommended flow.
4. Maximum recommended flow.
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Note 1: SELECTING MOTOR SIZE: Power
absorbed by pump is read at point where power curve crosses
pump curve at operating point, (or curve separate to pump
curve). However this does not indicate motor / engine size
required. Various methods are used to determine driver size.
-
Select
motor or engine to suit specific engine speed or operating
range - most cost effective method where operating conditions
will not vary greatly. (very risky - as a pump is often
not used for the purpose it was originally intended)
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Read
power at end of curve - most common way that ensures
adequate power at most operating conditions.
-
Read
power at operating point plus 10% - usually only used
in refinery or other applications where there is no
variation in system characteristics.
-
By
using system curves all operating conditions can be
considered - best method where filling of long pipelines,
large variations in static head, or siphon effect exist.
-use orifice plates or valves to control power usage.
CENTRIFUGAL
PUMP OPERATING RANGE
All
types of pumps have operational limitations. This is a consideration
with any pump whether it is positive displacement or centrifugal.
The single volute centrifugal pump (the most common pump
used worldwide) has additional limitations in operating
range which, if not considered, can drastically reduce the
service life of pump components.
"BEP"
- Best Efficiency Point (refer to fig.3 below) is not only
the operating point of highest efficiency but also the point
where velocity and therefore pressure is equal around the
impeller and volute. As the operating point moves away from
the Best Efficiency Point, the velocity changes, which changes
the pressure acting on one side of the impeller. This uneven
pressure on the impeller results in radial thrust which
deflects the shaft causing:
The
resulting damage can include shortened bearing / seal
life or a damaged shaft . The radial load is greatest
at shut head.
Outside
the recommended operating range damage to pump is also
sustained due to excess velocity and turbulence. The resulting
vortexes can create cavitation damage capable of destroying
the pump casing, back plate, and impeller in a short period
of operation. Refer to fig.3 which indicates range of
operation (between approximately 50% and 120% of Best
Efficiency Point)
When
selecting or specifying a pump, it is important
not to add safety margins or base selection on inaccurate
information. The actual system curve may cross the
pump curve outside the recommended operating range.
In extreme cases the operating point may not allow
sufficient cooling of pump, with serious ramifications!
The
best practice is to confirm the actual operating
point of the pump during operation (using flow measurement
and / or a pressure gauge) to allow adjustment (throttling
of discharge or fitting of bypass line) to ensure
correct operation and long service life. |

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SYSTEM
CURVES
| System
curves allow correct selection of pumps and pipes,
and are invaluable in troubleshooting pump and system
problems. To draw a system curve, follow these steps
& refer to fig.4:
-
Find details of duty. ie, in this example: Water,
2m suction lift, 15m static discharge (17m total
static head), 360 metres of 150mm schedule 40 steel
pipe.
- Draw
a chart with flow on bottom scale and head on left
scale. (estimate scale required based on size of
existing pump, or guess maximum flow expected -
example shows max flow as 100 L/S and max head as75m
- sometimes you just have to guess to get started)
- Mark
static head. ie: 17m at zero flow.
- Mark
2 or 3 other points.ie: at 20L/S friction loss is
0.73 m / 100m of pipe, therefore 0.73 x 3.6 + 17
= 19.6 metres. Put mark at junction of 20 L/S and
19.6 m. Repeat for other points. (remember to add
static head each time)
- Join
these points with a line. You have completed the
System Curve. (Curve may have to be extended to
suit higher flow pumps.)
- The
pump operating point is where a pump curve crosses
the system curve. Draw as many pump curves over
the system curve as you like, to see where different
pumps will operate, or draw system curve over pump
curve.
- If
pump curve does not cross system curve, the pump
is not suitable. If the pump curve crosses the system
curve twice, then the pump will be unstable and
is not suitable.
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Note:
It is tempting to add extra margins to these calculations,
but in most circumstances that can contribute to the
wrong pump selection and a big repair bill for a damaged
oversized pump operating outside it's operating range.
Extra Note: Some applications require a best guess (hopefully)
oversize pump with budgeting for pressure gauges, valves,
and / or orifice plates, to allow adjustment during
commissioning to ensure the duty is achieved with maximum
pump life. |
Note:
'demand' pressure, ie: sprinklers etc, should be added at
each flow calculated to make the system curve. If you can't
get the data for the sprinkler / nozzles at various flows,
but you know that ie: 10 sprinklers will pass 0.2 L/s each
at approx 30psi, then your required flowrate is 2 L/s and
add 21m (approx 30 psi) to the static head when you start
drawing the system curve (as an approximation).
The
'demand' pressure or "head loss through sprinkler /
nozzle at a particular flowrate" is not added for each
sprinkler. Only the flowrate of each one is added together.
If the pressure is available for the most 'disadvantaged'
sprinkler, then it will be available for all sprinklers
in that system. Note: this means that a higher pressure
will be available to less 'disadvantaged' sprinklers allowing
a higher flowrate through those sprinklers. There may be
no need to calculate each sprinkler / nozzle, but if there
are significant differences in static head / long lengths
of pipe / reduced pipe diameters, then the system may require
more investigation to allow correct pump selection.
PARALLEL
& SERIES OPERATION
| The
use of two or more pumps to increase flowrate is called
Parallel pumping. The use of two or more pumps to
increase head is called Series pumping. Operation
of pumps under these circumstances may appear simple,
but there are more complex issues to consider, ie:
In
series applications: consider the pressure rating
of pump, shaft seal, pipework and fittings. Placement
is critical to ensure both pumps are operating within
their recommended range and will have a constant supply
of water.
Drawing
a curve for 2 or more pumps is simple, draw 1st pump
curve then draw 2nd curve, adding the head each pump
produces at the same flow. More curves can be added
in the same way Fig.5.
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In parallel applications: confirm suitability of pumps
by drawing a system curve (often 2 pumps will only
deliver slightly more than one pump due to excessive
friction loss. Also you can confirm that pump operation
will be within its recommended range.). Non return
valves are required especially if one pump operates
alone at times. Dissimilar pumps or pumps placed at
different heights requires special investigation.
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Drawing
a curve for 2 or more pumps is simple, draw 1st
pump curve then draw 2nd curve, adding the flows
each pump delivers at the same head. More curves
can be added in the same way Fig.6.
Once
the curve for two pumps has been drawn, add the system
curve, the point where the system curve crosses the
curve for two pumps , indicates the total flow from
two pumps. Draw a horizontal line from this point
back to the head axis. Where this horizontal line
crosses the curves for a single pump indicates the
amount of flow contributed by that pump to the total
flow.
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Unstable
Operation
| Fig.7
shows a system curve crossing a pump curve twice.
This is an example of unstable operation. Note that
if the first pump is operating at point 'C' when the
second pump is started, the second pump will operate
at shut head, delivering no flow as it will never
be able to open the non return valve (required to
prevent one pump discharging through the other when
only one pump is operating). If this was to occur,
the pump could eventually explode!
In
some cases it may be possible to change the order
of starting the pumps, and the curves can be drawn
to check this operation, however if there is any indication
of unstable operation or possibility of one pump being
'over powered' by another, the system may need to
be changed or different pumps will have to be used.
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CAVITATION
- TWO MAIN CAUSES
| A:
NPSH (r) EXCEEDS NPSH (a)
Due
to low pressure the water vapourises (boils) and higher
pressure implodes into the vapour bubbles as they
pass through the pump causing reduced performance
and potentially major damage. For more see NPSH -
Nett Positive Suction Head |
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B:
Suction or discharge recirculation
The
pump is designed for a certain flow range, if there
is not enough or too much flow going through the pump,
the resulting turbulence and vortexes can reduce performance
and damage the pump. For more see Centrifugal pump
Operating Range |
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The damage to a pump from cavitation can be severe.
It may shorten seal and bearing life and damage volute,
backcover, and even pipework beyond repair. The implosions
due to cavitation can sound like gravel passing through
the pump. Pumps are not able to pass vapour or air
same as an air compressor is not able to pass water.
NPSH
- Nett Positive Suction Head
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| NPSH
is a dirty word? There is enough fear of it to suggest
it is. But why? Because some people will not accept
that pumps don't suck!
If you accept that a pump creates a partial vacuum
and atmospheric pressure forces water into the suction
of the pump, then you will find NPSH a simple concept.
NPSH(a) is the Nett Positive Suction Head Available,
which is calculated as follows:
NPSH(a)= p + s - v - f
Where:
'p'= atmospheric pressure,
's'= static suction (If liquid is below pump, it is
shown as a negative value)
'v'= liquid vapour pressure
'f'= friction loss
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NPSH(a)
must exceed NPSH(r) to allow pump operation without
cavitation. (It is advisable to allow approximately
1 metre difference for most installations)
NPSH(r)
is the Nett Positive Suction Head Required by the
pump, which is read from the pump performance curve.
(Think of NPSH(r) as friction loss caused by the entry
to the pump suction.)
The other important fact to remember is that water
will boil at much less than 100 deg C if the pressure
acting on it is less than its vapour pressure, ie:
water at 95 deg C is just hot water at sea level,
but at 1500m above sea level it is boiling water and
vapour. There was enough atmospheric pressure at sea
level to contain the vapour, but once the atmospheric
pressure dropped at the higher elevation, the vapour
was able to escape. This is why vapour pressure is
always considered in NPSH calculations when temperatures
exceed 30 to 40 deg C.
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AFFINITY
LAWS - CENTRIFUGAL PUMPS
If
the speed or impeller diameter of a pump change, we
can calculate the resulting performance change (at
the same efficiency) using:
Affinity
laws:
1. The flow changes in proportion
to speed ie: double the speed = double the flow
2. The pressure changes by the square
of the difference ie: double the speed = multiply
the pressure by 4
3. The power changes by the cube
of the difference ie: double the speed = multiply
the power by 8 |
TROUBLESHOOTING
Only
one thing is a better troubleshooting tool than flowmeter
and pressure / vacuum gauges...that is:
readings from flowmeters, pressure / vacuum gauges taken
prior to the problem. ie: monitoring.
Gauge
readings will help diagnose pump and system problems quickly,
by reducing the possible causes. Flow measurement would
allow full diagnosis of pump performance but is sometimes
expensive or not possible (Cheap versions include: V notch
weir, measuring discharge from horizontal pipe, & timing
of filling / emptying). System curves can be used in evaluating
results.
Following
is troubleshooting - this list is not extensive or complete,
but covers basic symptoms and some possible causes:
1.
Pump does not prime. |
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Suction
lift too great.
Insufficient water at suction inlet.
Suction inlet or strainer blocked.
Suction line not air tight.
Suction hose collapsed.
Mechanical seal / packing drawing air into pump.
Dry-prime pumps - discharge non return valve leaking
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2.
Not enough liquid. |
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Incorrect
engine speed.
Discharge head too high.
Suction lift too great.
Suction inlet or strainer blocked.
Suction line not air tight.
Suction hose collapsed.
Mechanical seal drawing air into pump.
Obstruction in pump casing/impeller.
Impeller excessively worn.
Delivery hose punctured or blocked.
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3.
Pump ceases to deliver liquid after some time. |
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Excessive
air leak in suction line.
Mechanical seal / packing drawing air into pump.
Obstruction in pump casing/impeller.
Delivery hose punctured or blocked.
Suction
lift too great.
Insufficient water at suction inlet.
Suction inlet or strainer blocked.
Suction hose collapsed.
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4.
Pump takes excessive power. |
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Engine
speed too high.
Obstruction or contact between impeller and casing.
Viscosity and / or SG of liquid being pumped too high.
Bearing
failure or severe coupling misalignment.
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5.
Pump vibrating or overheating. |
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Engine
speed too high.
Obstruction in pump casing/impeller.
Impeller damaged.
Cavitation due to excessive suction lift / friction
loss.
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6.
Pump leaking at seal housing. |
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Mechanical
seal damaged or worn. Due to:
Dry Running during priming or loss of liquid.
Cracking of faces can occur due to thermal shock,
after pump has run dry or against shut head, and then
cool water enters the pump casing.
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