Flow Measurement

Chapter 11 - Magnetic Flowmeters

Magnetic flowmeters (magmeters) are designed to measure the flow of electrically
conductive liquids in a closed pipe. They are volumetric flow-measuring
devices and have been commercially available since the mid-1950s. Sizes range
from 1/25 inch to about 120 inches from most manufacturers. This covers a flow
range of about 0.003 gallon per minute to about 1,100,000 gallons per minute.
Early units were flanged devices that bolted to adjacent pipe flanges in much the
same way as an ordinary section of flanged pipe. They were large, heavy, and
expensive, but they offered several advantages over other flowmeters available at
that time.

Advantages:

  • Obstructionless design
  • Linear output
  • Corrosion-resistant
    wetted parts
  • High accuracy

With the obstructionless design, there are no moving parts to wear and no pressure
drop other than that offered by a section of pipe with equal length and inside
diameter. The only wetted parts are the electrodes and an insulating liner. These
can be selected for compatibility with the most corrosive of chemicals as well as
to meet sanitary requirements for food applications such as milk and other liquid
dairy products. The output signal is linear and directly proportional to the flow
velocity. Accuracy over a wide range (typically 30 to 1) has evolved from 1% of
full scale reading to 0.5% of rate as typical. Higher accuracies are available for
special applications. The basic fundamentals of operation, selection, installation,
and maintenance will be discussed in this chapter. The discussion will be basic
and generic. Specifics on availability of features and options can be obtained from
the various magmeter manufacturers.

Operating Principle

Magnetic flowmeters operate on the principle of Michael Faraday's law of electromagnetic
induction. Without getting into the mathematics of this theory, it can
be simply stated as follows:

 E = constant × B × L × v(11-1)

where:   
 E=magnitude of the voltage
 B=magnetic field density
 L=path length
 =average velocity of the medium

Equation (11-1) implies that a voltage is developed when a conductor is passed
through a magnetic field. It further states that the voltage developed is proportional
to the density of the magnetic field, the length of the conductor, and the
velocity of the conductor moving through the field. There is nothing in the equation
about temperature, pressure, density, or viscosity because the magmeter
develops its signal independent of these parameters.

 

 

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