Flow Measurement

Chapter 16 - Target Flowmeters

Versatility and low installation cost make the target flowmeter a viable candidate
for many difficult flow measurement applications. Full bore, in-line meters are
available in sizes from 1/2 to 6 inches. Insertion versions for larger line sizes are
also available. Target flowmeters are used on liquids, gases, vapors, dirty fluids,
light slurries, and high viscosity fluids, particularly where fluid characteristics
preclude the use of flowmeters with pressure taps or moving parts. Process temperatures
vary from cryogenic to low temperature steam.

Operating Principle

Whenever there is flow past an obstacle in a pipe, a force, commonly referred
to as drag, is generated to push or drag the obstacle in the direction of flow. Such
an obstacle left unsupported would be carried away with the fluid. If, on the other
hand, the obstacle was constrained by a force equal and opposite to the drag, the
magnitude of that force could be used to determine the rate of flow. This is the
underlying principle behind the target flowmeter.

There are two primary contributors to drag. One results from the force generated
by the fluid viscosity as it slides by the obstacle. This is referred to as friction
drag and has its major influence when the flowmeter is operated in the laminar
flow regime. The second contributor is the so-called pressure drag. Pressure drag
is the force resulting from the difference between the pressures immediately
upstream and immediately downstream of the obstacle. For turbulent flows, the
pressure drag is the prime contributor to the total drag on the obstacle.

Advantages:

  • Low cost
  • Ease of installation,
    service
  • Simple construction,
    high reliability
  • No pressure ports to plug
  • Can be used on most fluids, clean or dirty

The obstacle or target typically used in practice is a circular disc mounted concentrically
in a pipe. The idealized flow past such a target is shown in Figure 16-1.
The upstream face sees a relatively high pressure since the forward motion of a
large percentage of the fluid is abruptly stopped before turning and traveling
around the target. As the fluid passes through the annulus around the target, it sees
an increase in velocity and, as a result, a decrease in pressure. At the downstream
edge of the plate, this high velocity, low pressure flow separates from the target
surface, setting up turbulence downstream of the target. This results in a relatively
low pressure region near the downstream face.

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