Clamp on Ultrasonic Instruments in Subsea Applications
Authors: Haugen Svein , Hodgson Suzanne , Upchurch John , McMahan Jim , Hazelrigg Keith , MundorFf Jan 
Published: October 2008

SAND MONITOR OVERVIEW
The subsea ultrasonic sand monitor described usesa clamp-on transducer that measures the acoustic energy generated by sand grain impacts on the inner side of a pipe wall (See Figure 1).
A preamplifier is connected to the acoustic transducer by a miniature coaxial cable. The preamplifier is connected to a signalprocessing board that outputs a 4-20 mA current signal in logarithmic proportion to themeasured acoustic energy.
The components are packaged in a sub sea housing (Figure 3) that is attached by means ofmounting adapters clamped to the outside of the pipeline.
The detector signal output is carried to the sub sea electronics module via a 2-pair oil filled cable before telemetry to surface via the umbilical. The topside master control station combines the acoustic energy signal with flow velocity information an outputs the mass of produced sand.

SANDMONITOR MEASUREMENT PRINCIPLE
Although the transducer is especially sensitive to acoustic emissions due to particle impact, it also reacts to flow induced noise (background noise) as shown in Figure 11. Since noise related to flow velocity is an unwanted component of the signal, the sandmonitor filters out this noise with an interference canceling function, subtracting it from themeasured signal. The remaining signal represents that generated by sand. So far, ithas proven difficult to reconcile theory with measurement for the multitude of different flow conditions encountered. Consequently, a background noise canceling function must be empirically derived by fitting a polynomial curve to observed detector output signal levels recorded at approximately 5 different flow rates (Shown in Figure 14). The flow velocity is calculated in the topside master control stationusing a model that relates choke position, well head temperature and pressure to flow rate. The detector signal output generated per unitof sand production, mA per gram/see. has been determined to be unique within reasonableaccuracy. The signal corresponding to a particular sand production rate is affected by the flow velocity. For this reason the system uses a normalized sand signal vs. flow velocity function to convert sand generated noise to sand production rate given that flow velocity is known.
The normalized sand signal vs. velocity function is determined by subtracting the background noise from the total output signal observed while a known amount of sand hasbeen injected into a test flow loop. The total detector signal while circulating 5 grams of sand in the flow loop is shown as a function of velocity in Figure 12. The resulting normalized sand noise function is shown in Figure 15.
To give an example of the described operation, lets imagine that the detector outputs a value of 8 mA to the topside master control station, while flow velocity is 3 mtrs./sec. At this velocity the master control station will subtract4.25 mA (read out from Figure 14) from the detector signal. The remaining 3.75 mA is divided by the normalized sand signal at 3 mtrs./sec. which is 0.25 mA per. gram/see(read off from Figure 15).