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PNNL-13501 - Pacific Northwest National Laboratory

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Therefore, in order to extract the viscosity, one also needs<br />

to measure the density.<br />

Acoustic Impedance Measurement (Density-Speed of<br />

Sound Product)<br />

The acoustic impedance of a material is defined as the<br />

product of the density and speed of sound in the material.<br />

For a perpendicular reflection, the reflection coefficient is<br />

dependent upon the acoustic impedance of the wall<br />

material and the acoustic impedance of the liquid.<br />

Speed of Sound in the Liquid<br />

Figure 1 shows 0.2 MHz transducers on opposite sides of<br />

a tank. It also might be possible to use a single transducer<br />

operating as both the sender and receiver of the ultrasonic<br />

wave, i.e., the pulse-echo mode of operation. The time of<br />

flight of the pulse can be used to determine the speed of<br />

sound.<br />

The combination of these three types of measurements<br />

can yield the density, viscosity, and speed of sound in the<br />

liquid.<br />

Approach<br />

To evaluate the feasibility of through-wall measurements,<br />

we conducted a series of experiments varying the<br />

transducer frequency and bandwidth and type of pulse for<br />

both shear and longitudinal waves to investigate the types<br />

of responses that met the criteria that the succeeding<br />

echoes do not overlap. The properties of the transducers<br />

were determined. Design parameters include the<br />

frequency of the transducer and its bandwidth, because<br />

the frequency determines the period of the pulse while the<br />

bandwidth determines the shape of the pulse. The<br />

bonding of the transducer to the wall is another important<br />

aspect, which may be accomplished using epoxy. The<br />

time length of the pulse is determined by the pulse that is<br />

sent to the transducer and the bandwidth of the transducer.<br />

For these investigations, a square-wave pulser provided a<br />

high voltage pulse of short duration to the transducer.<br />

Data were obtained using a digital oscilloscope that has<br />

the capability to obtain fast Fourier transforms and save<br />

the information to disk. Also investigated were the use of<br />

toneburst signals of approximately 6 cycles. Both<br />

methods were equivalent. An experimental apparatus was<br />

designed and constructed, and experiments were<br />

conducted to measure the acoustic impedance of a liquid.<br />

Results and Accomplishments<br />

Shear wave transducers produced vibrations that were<br />

perpendicular to the direction of the wave and that<br />

traveled easily in solids. While longitudinal waves travel<br />

easily in liquids, shear waves penetrate the liquid only<br />

very slightly. This penetration depends upon the viscosity<br />

and increases with an increasing viscosity. The acoustic<br />

impedance of stainless steel was large compared to most<br />

liquids; therefore, the change in viscosity was not<br />

significant enough to be readily observed in our<br />

experiments. However, experiments with a machinable<br />

glass allowed us to differentiate between a range of water<br />

and sugar water samples with differing viscosities. The<br />

results showed that differences in voltages can be seen for<br />

30% sugar water and 50% sugar water, compared to<br />

water.<br />

Summary and Conclusions<br />

A new approach was developed to characterize fluid<br />

density and viscosity by transmitting an ultrasonic signal<br />

through the wall of the pipe or vessel. Experiments were<br />

conducted to evaluate configurations for successful<br />

measurement. These experiments showed the potential to<br />

measure the density through the wall of pipes or vessels.<br />

Experiments showed that the measurement of viscosity<br />

using machinable glass is feasible.<br />

References<br />

Bamberger JA, and MS Greenwood. 2000. “Measuring<br />

slurry density and viscosity in-situ in real time during<br />

pipeline transport using an ultrasonic sensor.”<br />

FEDSM00-11121. Proceedings of the ASME 2000 Fluids<br />

Engineering Division Summer Meeting, June 11-15, 2000,<br />

Boston, Massachusetts. American Society of Mechanical<br />

Engineers, New York.<br />

Bamberger JA, LJ Bond, and MS Greenwood. 1999.<br />

“Ultrasonic measurements for on-line real-time food<br />

process monitoring.” In Proceedings of the Sixth<br />

Conference on Food Engineering, 1999 AIChE Annual<br />

Meeting, Dallas, Texas. <strong>PNNL</strong>-SA-32024, <strong>Pacific</strong><br />

<strong>Northwest</strong> <strong>National</strong> <strong>Laboratory</strong>, Richland, Washington.<br />

Greenwood MS, JR Skorpik, and JA Bamberger. 1999.<br />

“On-line sensor for density and viscosity measurement of<br />

a liquid or slurry for process control in the food industry.”<br />

In Proceeding of the Sixth Conference on Food<br />

Engineering, 1999 AIChE Annual Meeting, Dallas,<br />

Texas. <strong>PNNL</strong>-SA-32025, <strong>Pacific</strong> <strong>Northwest</strong> <strong>National</strong><br />

<strong>Laboratory</strong>, Richland, Washington.<br />

Sensors and Electronics 405

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