An educational resource
for students, industrial technicians and buyers
This short course has been designed to help those people
who are either new to flowmeters or who have some general
background knowledge about them but wish to have a broader
understanding of flowmeters.
There seems to be some general confusion and misconception
regarding the definition of what a flow meter is. Basically
a flowmeter is a device that meters movement of fluid
in a conduit or an open space. This fluid could be water,
chemicals, air, gas , steam or solids. Several flowmeter
definitions confine the term to a particular application
but in reality the term can be applied to much wider
usages
Here is an example of some current definitions to prove
this point –
Definitions of flow meter on the web:
- A gauge indicating the velocity of wastewater moving
through a treatment plant or of any liquid moving
through various industrial processes.
- A device for measuring the rate of fluid flow,
usually in pipes.
- A device for monitoring and measuring the flow
of a substance (typically fluid or gas).
- An instrument for measuring the flow of liquids.
- Any device that measures the flow of a specific
gas or gas mixture passing through.
The above definitions are too application specific,
so we shall use the more general definition of flowmeters.
A flowmeter is a device that
meters movement of fluid in a conduit or an open space.
This fluid could be water,chemicals, air, gas , steam
or solids
Selection of flowmeters:
Selecting a flowmeter can be an easy or a difficult
task depending on the requirements. It is important
to remember that there is no universal flowmeter that
will be appropriate for every application. The selection
process can be driven by many factors. Here we will
list some of them
- Accuracy requirements in the particular application
- Repeatabililty requirements in the particular application
- Price /economic constraints
- Personal or company preference
- Brand preference
- Robustness or ability to work in harsh or hazardous
type conditions
- Size
- Ease of installation
- Longevity
- Response time
- Special requirements
Since currently there is exists no single type of flowmeter
that meets everyone’s requirements, it is possible
for several companies around the world to manufacture
and develop many types of flow measurement devices which
are sold/supplied into various industries. This short
training course has not been designed to serve as a
recommendation tool since this task must be left to
the manufacturers, consultants and engineers and technical
sales personnel. Instead, we will take a look at some
of the more prominent designs and measurement techniques
of flowmeters to broaden the understanding of the reader.
Variable Area flow meters (also referred
to as Rotameters)
Despite the growing popularity of other flowmeter types,
the variable area flowmeter continues to command a major
portion of the industrial market. Although it has not
enjoyed the same degree of publicity granted more exotic
meter forms in technical literature, continuing innovations
and developments in variable-area metering have greatly
enhanced the capabilities of this popular flow monitor.
Their basic advantages--relatively low cost, accurate
and reliable performance, simplicity, and inherent versatility--remain
valid today. Available in a wide variety of metals and
plastics, and with current alarm and control options,
variable area meters can be used with a wide variety
of liquid, gas, and steam applications.
Perhaps the best known of the variable area meter family
is the "rotameter," first patented in the
United States in 1868. In its basic form, the rotameter
consists of a vertically oriented tapered glass tube
with the large end at the top, and a metering float
which is free to move within the tube. Fluid flow causes
the float to begin to rise in the tube as the upward
pressure differential and buoyancy of the fluid overcome
the effect of gravity.
The float will rise until the annular area between
the float and tube increases sufficiently to allow a
state of dynamic equilibrium between the (upward) pressure
differential and buoyancy factors, and (downward) gravity
factors. The height of the float is an indication of
flow rate, and the tube can be graduated in appropriate
flow units.
These meters typically can have up to a 12 to 1 turndown
(ratio of maximum to minimum measures flow), and industrial
accuracies of +/- 2% or even 1% of the full scale rating.
To meet the demands of a variety of industrial requirements,
a variety of constructions has become common. Glass
is often replaced with various plastic or metal components,
with some form of magnetic position sensing being used
in the latter case. The use of magnetic float sensing
is also used for alarm and signal transmission functions,
in many cases.
SLOTTED TUBE FLOWMETERS
Another variation of industrial variable area meters
uses a slotted cylinder and piston rather than a tapered
tube (see figure). This piston portion of the meter
float travels within a precision-honed cylinder, with
the piston acting as the fourth side of the slot. As
with tapered tube meters, fluid flow raises the piston
until sufficient slot area is exposed to bring all forces
into dynamic equilibrium. To assure constant buoyancy,
a "snorkel" device allows the top of the unit
to fill with fluid in liquid applications.
The metering cylinder and piston are contained within
a T-shaped body, and flow is read by means of a knife-edged
disk supported by an extension from the piston. This
disk moves up and down in response to flow within a
transparent sight tube containing an externally mounted
scale. As the tube is cylindrical and the disk always
close to its walls, flow can be read in dirty fluids.
If a transparent sight tube cannot be used, a magnet
is added to the float and an external indicator used.
Use of a magnet on or encapsulated in the float also
provides alarm and control functions with appropriate
accessories.
Advantages of this meter style include more compact
and less costly construction, high rangeabilities of
25 to 1, and easy access to flow internals for cleaning
or changing meter capacity without removing the unit
from the pipeline. Standard accuracy is +/-2% full scale,
with +/-1% calibrations as an option, and repeatability
+/-0.3% of rate. Pressure drops are reasonably low,
and similar to tapered tube models.
VANE AND PISTON FLOWMETERS
Yet another style
of variable area meter incorporates a spring-loaded
orifice and tapered plug or a vane within a "bowl."
Fluid flow moves the vane or orifice, exposing
a greater area around the tapered plug or within
the bowl until equilibrium is achieved. Flow is
read by means of a pointer mechanically positioned
by the vane, or by a magnetic indicator. Although
use of a spring does have drawbacks in terms of
pressure drop and repeatability, the principal
flow element does not rely on gravity and, therefore,
these meters can be mounted in any position.
Accuracies vary from +/-2% to +/-5%, depending
on the model, and average repeatability is +/-1%.
Rangeability is usually 6 or 10 to 1. Because
of the incorporation of the spring, pressure drops
are high (often expressed in pounds rather than
inches W. C. as with other variable area meters),
and generally go up from 2 psig. |
 |
Differential Pressure Meters
The use of differential pressure as an inferred measurement
of a liquid's rate of flow is well known. Differential
pressure flowmeters are, by far, the most common units
in use today. Estimates are that over 50 percent of
all liquid flow measurement applications use this type
of technology.
The basic operating principle of differential pressure
flowmeters is based on the knowledge that the pressure
drop across the meter is proportional to the square
of the flow rate. The flow rate is obtained by measuring
the pressure differential and extracting the square
root.
Differential pressure flowmeters, like most flowmeters,
have a primary and secondary element. The primary element
causes a change in kinetic energy, which creates the
differential pressure in the pipe. The unit must be
properly matched to the pipe size, flow conditions,
and the liquid's properties. And, the measurement accuracy
of the element must be good over a reasonable range.
The secondary element measures the differential pressure
and provides the signal or read-out that is converted
to the actual flow value.
Orifices are the most widely liquid flowmeters in use
today. An orifice is simply a flat piece of metal with
a specific-sized hole bored in it. Most orifices are
of the concentric type, but eccentric, conical (quadrant),
and segmental designs are also available.
An orifice plate is a very simple device installed
in a straight run of pipe. The orifice plate contains
a hole smaller than the pipe diameter. The flow constricts,
experiences a pressure drop, and then the differential
pressure can be related to a flow.

Figure 1: Orifice Plate Arrangement
In practice, the orifice plate is installed in the
pipe between two flanges. Acting as the primary device,
the orifice constricts the flow of liquid to produce
a differential pressure across the plate. Pressure taps
on either side of the plate are used to detect the difference.
Major advantages of orifices are that they have no moving
parts and their cost does not increase significantly
with pipe size.
The segmental wedge is a variation of the segmental
orifice. It is a restriction orifice primarily designed
to measure the flow of liquids containing solids. The
unit has the ability to measure flows at low Reynolds
numbers and still maintain the desired square-root relationship.
Its design is simple, and there is only one critical
dimension the wedge gap. Pressure drop through the unit
is only about half that of conventional orifices. Integral
wedge assemblies combine the wedge element and pressure
taps into a one-piece pipe coupling bolted to a conventional
pressure transmitter. No special piping or fittings
are needed to install the device in a pipeline. Metering
accuracy of all orifice flowmeters depends on the installation
conditions, the orifice area ratio, and the physical
properties of the liquid being measured.
Venturi tubes have the advantage of being able to handle
large flow volumes at low pressure drops. A venturi
tube is essentially a section of pipe with a tapered
entrance and a straight throat. As liquid passes through
the throat, its velocity increases, causing a pressure
differential between the inlet and outlet regions.

Fig, 19 Venturi Tube
The flowmeters have no moving parts. They can be installed
in large diameter pipes using flanged, welded or threaded-end
fittings. Four or more pressure taps are usually installed
with the unit to average the measured pressure. Venturi
tubes can be used with most liquids, including those
having a high solids content.
Fig 20 Flow Nozzle
Flow Nozzles, at high velocities, can handle approximately
60 percent greater liquid flow than orifice plates having
the same pressure drop. Liquids with suspended solids
can also be metered. However, use of the units is not
recommended for highly viscous liquids or those containing
large amounts of sticky solids.
Fig. 21 Pitot tube
Pitot tubes sense two pressures simultaneously, impact
and static. The impact unit consists of a tube with
one end bent at right angles toward the flow direction.
The static tube's end is closed, but a small slot is
located in the side of the unit. The tubes can be mounted
separately in a pipe or combined in a single casing.
Pitot tubes are generally installed by welding a coupling
on a pipe and inserting the probe through the coupling.
Use of most pitot tubes is limited to single point measurements.
The units are susceptible to plugging by foreign material
in the liquid. Advantages of pitot tubes are low cost,
absence of moving parts, easy installation, and minimum
pressure drop.
Fig 22 Elbow Flow meter
Elbow meters operate on the principle that when liquid
travels in a circular path, centrifugal force is exerted
along the outer edges. Thus, when liquid flows through
a pipe elbow, the force on the elbow's interior surface
is proportional to the density of the liquid times the
square of its velocity. In addition, the force is inversely
proportional to the elbow's radius. Any 90 deg. pipe
elbow can serve as a liquid flowmeter. All that is required
is the placement of two small holes in the elbow's midpoint
(45 deg. point) for piezometer taps. Pressure-sensing
lines can be attached to the taps by using any convenient
method.
Target meters sense and measure forces caused by liquid
impacting on a target or drag-disk suspended in the
liquid stream. A direct indication of the liquid flow
rate is achieved by measuring the force exerted on the
target. In its simplest form, the meter consists only
of a hinged, swinging plate that moves outward, along
with the liquid stream. In such cases, the device serves
as a flow indicator. A more sophisticated version uses
a precision, low-level force transducer sensing element.
The force of the target caused by the liquid flow is
sensed by a strain gage. The output signal from the
gage is indicative of the flow rate. Target meters are
useful for measuring flows of dirty or corrosive liquids.
Some manufacturers also apply them to certain steam
applications.
Electromagnetic Flowmeters (Magmeters)
The operating principle of magnetic flowmeters is based
upon Faraday's Law of electromagnetic induction,
" It states that a voltage will be induced in a
conductor moving through a magnetic field."
 |
Faraday's Law :
E=kBDV Where
E = Induced Voltage,
B = Strength of the magentic field,
D = Conductor Width,
V = Velocity of the conductor |
The magnitude of the induced voltage E is directly
proportional to the velocity of the conductor V, conductor
width D, and the strength of the magnetic field B. Magnetic
field coils placed on opposite sides of the pipe generate
a magnetic field. As the conductive process liquid moves
through the field with average velocity V, electrodes
sense the induced voltage. The width of the conductor
is represented by the distance between electrodes. An
insulating liner prevents the signal from shorting to
the pipe wall. The only variable in this application
of Faraday's law is the velocity of the conductive liquid
V because field strength is controlled constant and
electrode spacing is fixed. Therefore, the output voltage
E is directly proportional to liquid velocity, resulting
in the linear output of a magnetic resulting in the
linear output of a magnetic flowmeter
Magnetic flowmeters are based on Faraday's Law of Magnetic
Induction. In a magnetic flowmeter, the liquid acts
as a conductor as it flows through the pipe. This induces
a voltage which is proportional to the average flow
velocity - the faster the flow rate, the higher the
voltage. This voltage is picked up by sensing electrodes
mounted in the meter tube and sent to the transmitter
which takes the voltage and calculates the flow rate
based on the cross sectional area of the meter tube.
Where to use
- High percentage of solids
- Sludges, slurries, minerals, paper, sewage - flows
with high levels of solids which cannot be measured
other types of meters.
- Obstructionless measurement
- Nothing projects into the flow stream, no head
loss, no parts to maintain.
- Very corrosive liquids
- Acids, caustics and corrosive chemical additives
are isolated from the meter by inert linings and electrodes.
- Conductive Liquids
- Liquids where conductivity is at sufficient levels
to induce measurable voltage
Turbine Flow meters
Turbine type flowmetering devices are applied worldwide
to the measurement and control of liquid products in
the industrial, chemical and petroleum marketplaces.
Significant advantages associated with the use of turbine
flowmeters, in lieu of other metering principles, make
increased future use inevitable. Newcomers to the field
of flow measurement should become familiar with fundamental
characteristics and conditions surrounding the turbine
flowmeter in order to better understand its usage. Consequently,
this article is provided as a brief guide to the operation
and application of turbine flowmeters for liquid product
measurement.
The basic construction of the turbine flowmeter incorporates
a bladed turbine rotor installed in a flow tube. The
rotor is suspended axially in the direction of flow
through the tube. The turbine flowmeter is a transducer,
which senses the momentum of the flowing stream. The
bladed rotor rotates on its axis in proportion to the
rate of the liquid flow through the tube.
TURBINE ROTATION
As the liquid product strikes the front edge of the
rotor blades, a low-pressure area is produced between
the upstream cone and the rotor hub.
The blades of the turbine rotor will tend to travel
toward this low-pressure area as a result of this pressure
differential across the blades. The pressure differential
(or pressure drop) constitutes the energy expended to
produce movement of the rotor. The initial tendency
of the rotor is to travel downstream in the form of
axial thrust. But since the rotor is restrained from
excessive downstream movement, the only resulting movement
is rotation.
Fluid flowing through the meter impacts an angular velocity
to the turbine rotor blades, which is directly proportional
to the linear velocity of the liquid. The degree of
the angular velocity or number of revolutions per minute
of the turbine rotor is determined by the angle of the
rotor blades to the flowing stream of the approach velocity.
ROTOR BALANCE
With axial thrust forcing the turbine rotor downstream,
the friction resulting from contact between the turbine
rotor and the downstream cone would cause excessive
wear if there were not some means of balancing the turbine
rotor on its axis between the upstream and the downstream
cone.
Bernoulli's Principle states that when flow velocity
decreases, the static pressure increases. Therefore,
a high-pressure area exists at the downstream side of
the turbine rotor exerting an upstream force on the
rotor. As a result, the turbine rotor is hydraulically
balanced on its axis.
SIGNAL OUTPUT
Electrical output is generated using the principle of
reluctance. A pickup coil, wrapped around a permanent
magnet, is installed on the exterior of the flow tube
or the meter body immediately adjacent to the perimeter
of the rotor (Figure 1). The magnet is the source of
the magnetic flux field that cuts through the coil.
Each blade of the turbine rotor passing in close proximity
to the pickup coil causes a deflection in the existing
magnetic field. This change in the reluctance of the
magnetic circuit generates a voltage pulse within the
pickup coil.
Each pulse generated represents a discrete amount of
volumetric throughput. Dividing the total number of
pulses generated by the specific amount of liquid product
that passed through the turbine flowmeter determines
the K-Factor. The K-Factor, expressed in pulses per
unit volume, may be used with a factoring totalizer
to provide an indication of volumetric throughput directly
in engineering units. The totalizer continuously divides
the incoming pulses by the K-Factor (or multiplies them
with the inverse of the K-Factor) to provide factored
totalization. The frequency of the pulse output, or
number of pulses per unit time, is directly proportional
to the rotational rate of the turbine rotor. Therefore,
this frequency of the pulse output is proportional to
the rate of the flow.
By dividing the pulse rate by the K-Factor, the volumetric
throughput per unit time of the rate of flow can be
determined. Frequency counters or converters are commonly
used to provide instantaneous flow rate indication.
Plotting the electrical signal output versus flow rate
provides the characteristics profile or calibration
curves for the turbine flowmeter.
Electrical output is also generated using the principle
of inductance. A pickup coil is installed on the exterior
of the flow tube immediately adjacent to the perimeter
of the turbine rotor. The magnetic source of the flux
field in this type of output is either the rotor itself
or small magnets installed in the rotor. In the case
of the rotor, the material of construction would be
nickel or some other easily magnetized flux field. The
results are identical to that of the reluctance principal.
Figure 1
ACCURACY
The accuracy of a turbine flowmeter is derived from
its output (electrical or mechanical) and is the measure
of the deviation of an indicated measurement from the
referenced standard. Turbine meter accuracy is dependent
upon several items.
The accuracy must include the error associated with
the calibration standard. In the USA, the National Institute
of Standards and Technology represents the flow standard.
Linearity is the variation of the flowmeter K-factor
from a nominal value of a point on a curve. Normally
during calibration, a value is chosen which makes linearity
fall in line with accuracy. Linearity may remain constant
during meter life although the absolute accuracy level
has changed.
Repeatability is the ability of a turbine flowmeter
to reproduce its output indefinitely under constant
operating conditions at any point over its specified
operating range.
Figure 2 (click on the image to enlarge picture)
SPECIFIC GRAVITY
The specific gravity of a liquid is the ratio of its
density to that of water at 4BC (39.2BF) and is dimensionless.
While changes in specific gravity do not affect the
average turbine meter K-factor value, the overall linear
range of the flowmeter is changed (Figure 2). The linear
range represents the minimum to the maximum flow rate
within which the linearity of the flowmeter is specified.
As stated previously, the rotor rotates due to pressure
differential across the rotor blades. Specific gravity
is one of the factors affecting this pressure differential.
As the specific gravity decreases, the pressure differential
decreases. On a fluid with a low specific gravity and
a low flow rate, the pressure differential across the
blades is very low. This leaves almost no energy for
turning the rotor. Consequently, the rotor cannot turn
in proportion to the liquid throughput and the K-factor
drops off.
Therefore, the angle of the rotor blades is changed
to help compensate for the change to a lower specific
gravity. This allows products with lower specific gravity's
to be measured accurately by the turbine flowmeter.
VISCOSITY
Viscosity if the measure of the liquid products resistance
to flow. Kinematics viscosity is the ratio of the absolute
viscosity to the specific gravity, usually expressed
in centistokes (cs), where the resistance to flow is
measured in square millimeters per second (mm2/s).
VISCOSITY EFFECTS ON RANGEABILITY
Viscosity has two different effects on the turbine flowmeter
rotor. First of all, the profile causes boundary layer
thickness to increase as viscosity increases for a fixed
volume. This means that rotor-blade shape and length
will be important in determining the K-factor since
the flow around the blade tip region changes with respect
to viscosity. This boundary layer thickness causes the
turbine flowmeter to be non-linear. Supplying a shroud
around the turbine rotor, with the shroud outer diameter
slightly smaller than the inside diameter of the flow
tube, increases the viscosity and creates a drag (resistance
to rotation). This drag offsets the non-linear effect
of the boundary layer.
The second effect of viscosity is one of viscous shear-force
change on the rotor and increased viscous drag within
the bearing. These effects act to slow the rotor while
the profile effect acts to speed the rotor. The relative
magnitude of all these forces changes the Reynolds number.
As previously indicated, some turbine flowmeter designs
introduce a device or shroud that introduces viscous
drag, which eliminates the hump that normally, occurs
in the transition region.
While linearity is affected by viscosity, repeatability
is not.
FLOW RANGE
The minimum flow rate of a turbine flowmeter becomes
a factor of viscosity versus the degree of accuracy.
As product viscosity increases, the minimum flow rate
required to maintain a specific degree of accuracy increases.
The maximum rate of flow allowable becomes a factor
of viscosity versus the pressure drop across the flowmeter.
As the product viscosity increases, the maximum flow
rate decreases in accordance with the maximum allowable
pressure drop across the flowmeter. In order to arrive
at the minimum and maximum rate of flow limits for a
particular turbine flowmeter size and application these
factors must first be determined:
· The viscosity of the product to be metered
(or maximum value of viscosity for products with varying
viscosity's at 37.8B (100BF).
· The degree of accuracy required.
· The maximum amount of pressure drop allowed
across the flowmeter.
Using an area-of-operation diagram for a particular
turbine flowmeter size and charting the factors for
viscosity accuracy and pressure drop will determine
the minimum and maximum flow rates.
Operating the flowmeter within this flow range will
meet the operating requirements unique to that application.
Technical bulletins providing area of operation for
turbine flowmeter sizes with varying viscosity fluids
can be obtained from the various meter manufacturers.
CAVITATION
Cavitation in a turbine flowmeter will take place when
the local pressures fall close to or below the vapor
pressure of the liquid product. The formation of bubbles
and their collapse or local vaporization of product
as it passes over the rotor blade surface can cause
erratic behavior in the turbine flowmeter and excessive
wear due to over speeding. Maintaining a system backpressure
of 2 times the flowmeter pressure drop plus 25 times
the product vapor pressure is sufficient to prevent
cavitation as shown by the following formula:
BP= ( P x 2) + (VP x 1.25)
Where,
BP= Required back pressure
P= Pressure drop at maximum flow.
VP= Absolute vapor pressure at maximum temperature.
Cavitation usually causes the rotor to speed up at
the high flow rate due to the increased flow volume
and causes the accuracy curve of the turbine flowmeter
to be adversely affected.
INSTALLATION
The term swirl is used to describe the rotational velocity
or tangential velocity component of fluid flow in a
pipe or tube. Depending on its degree and direction,
swirl will change the angle of attack between the fluid
and the turbine rotor blades, causing a different rotor
speed at a constant flow rate to non-swirling conditions
at the same flow rate. Liquid swirl and non-uniform
velocity profiles may be introduced upstream of the
turbine flowmeter by variations in piping configurations
or projections and protrusions within the piping. Swirl
may be effectively reduced or eliminated through the
use of sufficient lengths of straight pipe or a combination
of straight pipe and straightening vanes installed upstream
of the turbine flowmeter.

APPLICATIONS
Turbine flowmeters, when first introduced, were used
mainly by the aircraft industry in small sizes. Turbine
flowmeters are now used on many applications (figure
3). Reasons for this increased used are sizes up to
12", weight and size versus flow rate, extended
flow ranges, operating pressures up to 10,000 pounds
per square inch, temperature range of -450° to 1000°F
and a wide variety of construction materials including
stainless steels.
In recent years, turbine flowmeters have been competing
successfully with positive displacement flowmeters in
many applications due to the economy of installation,
low maintenance costs, weight, size and high flow rates
per comparable connection size. You must exercise caution
when making this comparison, especially on viscous products.
Following the parameters outlined previously will prevent
most misapplications of the turbine flowmeter.
When products are used in which viscosity changes with
seasonal temperature, a proving run should be done at
a time when the product temperature would be changing.
For instance, fuel oil may change 50°F in ambient
temperature between summer and winter. A change of this
magnitude would affect the flowmeter curve and directly
affect the flow range.
Increased expertise with electronics such as linearization
is permitting turbine flowmeters to be used more widely
(figure 4).
PROVING
Proving is a method of checking a measuring device against
an accepted standard to determine the accuracy and repeatability
of that measuring device. Turbine flowmeters should
be proven immediately after installation, after repair,
following removal from service (for any reason) when
changing products, when product viscosity changes, or
to chart the flow patterns of the flowmeter during a
period of time.
In general, provings should be quite frequent in the
early history of an installation. When sufficient results
have been gathered to establish meter factor versus
flow rate curves for each product, frequently proving
can taper off unless one of the aforementioned reasons
for proving occurs.

Compliments of Sponsler USA
Figure 4: The turbine flowmeter position should not
adversely affect velocity or the smooth rotation of
the rotor. The rotor should decelerate and stop in a
smooth uninterrupted fashion. An abrupt sticking motion
indicates bearing failure.
METHODS
There are several different methods of proving. Volumetric
proving consists of a measured volume of fluid being
compared to a known standard, such as a seraphin can
or piston prover.
Gravimetric proving entails measuring weight of a fluid
by scale or load cell, then converting it by a known
formula.
Master-meter proving is the comparison of a test flowmeter
to another flowmeter previously calibrated in one of
the above methods.
Turbine flowmeter manufacturers continue to respond
to industry interest with improvements.
Ultrasonic Flowmeters
The ultrasonic flowmeter is now a more common
flowmeter . It was originally looked down upon
because many of them were misapplied in the beginning.
Since that time, electronic circuits have improved
and this has meant that ultrasonic flowmeters
have been able to achieve accuracies that previously
were unreachable . Doppler flowmeters were some
of the first ultrasonic flowmeters on the market.
The Doppler meter has had success on some blood
flow indicating devices and difficult flows in
pipes with higher solids and aeration but the
transit time meter has become more popular in
general measurements because of its ability to
measure accurately in cleaner fluids.
Both types of ultrasonic flowmeters feature clamp-on
or insert designs . Many of the designs are now
becoming non-intrusive /non contact which enables
them to measure fluids without disturbing flow
profile. Since there are no mechanical parts,
there is an added plus that they are more likely
to keep working where other technologies may have
problems with sensor fouling.
Figure 25 are typical examples of the ultrasonic
flowmeters offered by several companies. Here
are some of the capabilities of this technology.
The meter can measure pure water, wash water,
sewage, process liquids, oils, and other light
homogeneous liquids. The basic requirement is
that the fluid be capable of ultrasonic wave propagation
and have a reasonably axis-symmetrical flow.
Clamp-on types measure flow through the pipe without
any wetted parts, ensuring that corrosion and
other effects from the fluid will not deteriorate
the sensors.
An added plus to the above is that clamp-on types
simplify and speed up meter installation and minimize
maintenance.
|

Fig 25. Ultrasonic Flowmeter (Concurrent Transit
Time) – compliments of EESITEC Technologies
|
This design and others are portable, a feature particularly
advantageous for backing up an already installed flowmeter
or checking out existing meters in a number of locations.
.
Operation is linear and bidirectional.
Advances in digital signal processing have improved
performance where the flowing fluid contains air or
gas bubbles.
Some suppliers offer ultrasonic measurements of both
level and flow velocity to calculate flow quantities
in open channels with weirs or flumes. Others carry
ultrasonic meters especially adapted to measure the
flow rate of gases. This class of meter is attractive
compared to conventional flow metering methods because,
in addition to the points listed above, the meters inherently
provide linear calibration; have wide rangeability;
induce no or minimal pressure drop or disturbance in
the flow stream and recently there has been a much wider
acceptance regarding their reliability.
More about ultrasonic propagation techniques in flow
measurement.
To detect flow through a pipe, ultrasonic flowmeters
use acoustic waves or vibrations of a frequency .Depending
on the design, they use either wetted or nonwetted transducers
on the pipe perimeter to couple ultrasonic energy with
the fluid flowing in the pipe.
Doppler Flowmeters. Doppler flowmeters are named for
the Austrian physicist and mathematician Christian Johann
Doppler (18031853), who in 1842 predicted that
the frequencies of received sound waves depended on
the motion of the source or observer relative to the
propagating medium. To use the Doppler effect to measure
flow in a pipe, one transducer transmits an ultrasonic
into the flow stream .Liquid flowing through the pipe
must contain sonically reflective materials such as
solid particles or entrained air bubbles. The movement
of these materials alters the frequency of the beam
reflected onto a second, receiving transducer. The frequency
shift is measured and used to calculate flow rate.
A basic math equation defining the Doppler flowmeters
are:
(1)
and by Snell's law:
(2)
Thus, from Equations (1) and (2), we have:
(3)
where:

Equation (3) clearly shows that flow velocity is a
linear function of the Doppler frequency shift. Now,
because the inside diameter of the pipe, D, is known,
volumetric flow rate (e.g., in gallons per minute) can
be measured using the following expression:
(4)
where:
Transit-Time Flowmeters. Transit-time meters, as the
name implies, measure the difference in the time of
flight between signals transmitted alternately in the
direction of, and against, the flow. This type of meter
is commonly known as the transit time meter. Some manufacturers
send signals through each other concurrently, this is
known as Concurrent transit time.
Transit time flowmeters are becoming extremely popular
. Their usage has widened even to the point where this
technology is being used in domestic meters or submetering.
Calorimetric Flow meters
In the $3 billion dollar world market of flow metering,
a little known jewel is gradually finding its way to
acclaim…the calorimetric flow sensor. The use
of the calorimetric principle in flow is now a standard
in the industry. Significant advances over the past
decade have enabled the calorimetric sensor to assume
a very active and respected role in flow switching and
flow metering of both liquids and gaseous mediums.
The most common use of these sensors is in flow no-flow
applications for detecting the movement of air or liquids.
Popular for their solid state construction with no moving
parts, the calorimetric flow sensor is impervious to
particulate matter that spells doom for mechanical type
devices.
Historically, the calorimetric switching devices have
been costly in comparison to mechanical switches, but
with new technological breakthroughs in both electronic
and mechanical construction, there are, now available,
units that compete directly with their primitive counterparts.

Traditional Paddle Switch |

Modern Calorimetric sensor |
Flow metering has also become a substantive part of
the calorimetric sensor’s function. The sensing
technology, having no moving parts, allows measurement
of flows so low as to be below the inertia threshold
of turbine or paddlewheel sensors. This has made them
very popular for chemical dosing, leak detection, etc.
Also, extended range calorimetric sensors are now available
that can enable measurements of much higher flow rates
(up to 60 feet per second for some liquids) than previously
thought possible with calorimetric technology.
The traditional calorimetric technology utilizes two
PTC Thermistors, one of which is heated a predetermined
amount above the other, which monitors the medium temperature.
Flow of the medium conducts heat away from the sensor
probe and the corresponding change in the heated Thermistor’s
resistance value is then amplified, linearized and converted
into an output (switching or analog depending upon sensor
type) proportional to the rate of flow.


The fact that calorimetric sensors do not require the
medium to be electrically conductive (as would a mag
meter for example) makes measurements of polymers, oil,
grease, and numerous other mediums possible. The technology
also is not based upon suspended particles for measurement
accuracy (as would be the case with doppler type meters).
The addition of optional specialty metals for use in
the calorimetric construction (such as Hastelloy, Monel,
Titanium etc.) allows measurements of innumerable aggressive
medium such as chemicals and acids.
The calorimetric sensor’s minimal power requirements
have enabled the development of battery operated flow
sensors for remote locations. These can be paired with
wireless transmission devices to enable internet based
monitoring or dial up fault alarming for such applications
as loss of flow to pumps, leaking of pipes, and loss
of lubrication oil flow or coolant flow in transportation.
Inherent in the design is the continual monitoring
of the medium temperature, which enables the calorimetric
sensor to also function as a temperature monitor. This
provides the user with two sensors in one. This has
been a popular feature with chiller manufacturers, as
the same device can alarm if flow is lost, or temperature
exceeds predetermined limits.
Microflow technology in calorimetric sensors has also
enabled here-to-fore unrealizable low flow metering
of less than 2 milliliters per hour of liquid flow.
In summary, the calorimetric flow sensor is the rising
star of the flow sensing industry and offers capabilities
unmatched by other flow measurement technologies.
Coriolis Flow meters
What is the Coriolis Principle?
To some of us the Coriolis Principle is an exact science,
but to most of us it is still a black art. Well, imagine
a fluid flowing (at velocity V) in a rotating elastic
tube as shown below. The fluid will deflect the tube.

Further, consider a Mass M moving from the center to
the edge of a rotating plate.
This Mass M will take path B as shown below

If the mass M is guided by Wall A (i.e. the tube), a
Coriolis Force will be exerted on the wall as shown
below.
CORIOLIS FORCE : Fc = -2 M V W
Now, consider the interior of the RotaMASS sensor as
shown below

The tube walls guide the process fluid as it flows through
the U-Tube pathway. With no fluid inside the tubes the
Driver excites the tubes apart at a nominal 150Hz as
shown below.

No Flow:
Parallel Deflection |
Mass Flow:
Coriolis Twist |
Now imagine fluid of Mass M flowing through and out
of the RotaMASS tubes. As the fluid flows down the first
half of the U-Tubes it will tend to deflect the tubes
in towards each other. Conversely, when the fluid flows
up the second half of the U-Tubes it will tend to deflect
the tubes out away from each other. This Coriolis Twist
action is shown above.
Now consider the diagram below. The baseline deflection
of the tubes from the Driver is shown by the blue trend
and the Coriolis Twist from the Pickup Coil is designated
by the red trend.
Now the temperature of these tubes dramatically affects
their flexibility. So temperature measurement is very
critical as follows;

The Mass flow equation for the RotaMASS
can be described as follows;
Where,
M
Ac
Ae
Ac/Ae
Sk
Sk(20°C)
fv
Sk
t |
= Mass flow rate
= Amplitude of coriolis oscillation
= Amplitude of excitation oscillation
= Phase Angle
= Sensor constant (calibration constant)
= Sk(20°C) (1+Skt x (T-20°C)) temperature
correction
= Sensor constant at 20°C
= Excitation frequency
= Temperature correction coefficient (material constant)
|
The Density equation for the RotaMASS can be described
as follows;
p
fI(20)
fv(20)
KD
fv(20)
FKT |
= Density
= Exciting frequency of the empty tubes at 20°C
= Exciting frequency of the filled tubes at 20°C
= Density calibration constant
= fv / (1+FKT (T - 20 °C)) temperature correction
of the actual frequency
= Temperature correction coefficient, depending
on material and size |
|