Abstract:Abstract-A new method for measuring the pressure reflection coefficient in a buffer rod configuration is presented, together with experimental results for acoustic measurements of the liquid density, based on the measurement of the liquid's acoustic impedance. The method consists of using 2 buffers enclosing the liquid in a symmetrical arrangement with a transducer fixed to each buffer. One of the transducers is used in a pulse-echo mode while the other transducer operates as a receiver. The echo amplitudes le… Show more
“…Therefore, a plane-wave approach with diffraction correction is taken. These aspects, along with an experimental realization using this measuring principle, are further described in [30].…”
Section: A Description and Theory Of The Proposed Measuring Principlementioning
confidence: 99%
“…A particular component of the systematic noise is the interference effect from the conversion of shear wave to compressional wave at the buffer-sample interface [32]. Using echo signals that do not interfere with such systematic noise components will be beneficial as the measurement of the echo signal's amplitudes leading to the reflection coefficient otherwise will be in error [30]. Also scattering both from within the buffers and the liquid is ignored.…”
Section: B Nonideal Behaviormentioning
confidence: 99%
“…Some of these new methods seem particularly suited for the measurement of high attenuation liquids, and they benefit from being able to obtain a reduced sensitivity of interference effects arising from mode conversion at the buffer-liquid interface, because these methods use a reduced time trace, compared with the ABC method. Experimental verification of some of these new methods in comparison with the ABC method will be given in an accompanying paper regarding acoustic measurement of liquid density [30], with more extensive results given in [35].…”
Abstract-The known acoustic methods for obtaining the pressure reflection coefficient from a buffer rod based measurement cell are presented, along with 2 new generic approaches for measuring the pressure reflection coefficient using 2 buffer rods enclosing the liquid to be characterized in a symmetrical arrangement. An acoustic transducer is connected to each of the buffer rods. The generic approaches are divided into a relative amplitude approach and a mixed amplitude approach. For the relative amplitude approach, families of 4, 5, or 6 echo signals can be used to obtain the pressure reflection coefficient. The mixed amplitude approach uses specific information about the transducers and/or the electronics sensitivities in receive mode to obtain the pressure reflection coefficient using families of 3, 4, 5, or 6 echo signals. Some of the new methods from the relative amplitude approach imply a reduced uncertainty relative to the previously known ABC method. The effect of the liquid attenuation, digitizer bit resolution, and the signal-to-noise ratio on the uncertainty characteristics of the pressure reflection coefficient are discussed, along with a discussion of the suitability of the various methods for different buffer materials.
“…Therefore, a plane-wave approach with diffraction correction is taken. These aspects, along with an experimental realization using this measuring principle, are further described in [30].…”
Section: A Description and Theory Of The Proposed Measuring Principlementioning
confidence: 99%
“…A particular component of the systematic noise is the interference effect from the conversion of shear wave to compressional wave at the buffer-sample interface [32]. Using echo signals that do not interfere with such systematic noise components will be beneficial as the measurement of the echo signal's amplitudes leading to the reflection coefficient otherwise will be in error [30]. Also scattering both from within the buffers and the liquid is ignored.…”
Section: B Nonideal Behaviormentioning
confidence: 99%
“…Some of these new methods seem particularly suited for the measurement of high attenuation liquids, and they benefit from being able to obtain a reduced sensitivity of interference effects arising from mode conversion at the buffer-liquid interface, because these methods use a reduced time trace, compared with the ABC method. Experimental verification of some of these new methods in comparison with the ABC method will be given in an accompanying paper regarding acoustic measurement of liquid density [30], with more extensive results given in [35].…”
Abstract-The known acoustic methods for obtaining the pressure reflection coefficient from a buffer rod based measurement cell are presented, along with 2 new generic approaches for measuring the pressure reflection coefficient using 2 buffer rods enclosing the liquid to be characterized in a symmetrical arrangement. An acoustic transducer is connected to each of the buffer rods. The generic approaches are divided into a relative amplitude approach and a mixed amplitude approach. For the relative amplitude approach, families of 4, 5, or 6 echo signals can be used to obtain the pressure reflection coefficient. The mixed amplitude approach uses specific information about the transducers and/or the electronics sensitivities in receive mode to obtain the pressure reflection coefficient using families of 3, 4, 5, or 6 echo signals. Some of the new methods from the relative amplitude approach imply a reduced uncertainty relative to the previously known ABC method. The effect of the liquid attenuation, digitizer bit resolution, and the signal-to-noise ratio on the uncertainty characteristics of the pressure reflection coefficient are discussed, along with a discussion of the suitability of the various methods for different buffer materials.
“…In cases where the equilibrium density cannot be employed, such as polymerization or structural formation processes, the simultaneous measurement could provide useful insight. The MERUS technique is different from previous literature but is similar to an ultrasound densitometer using a buffer rod . However, MERUS utilizes a disposable plastic cell (free from contamination attached to the buffer rod), and the error could be minimized by employing a reference to correct the small phase shift during measurements.…”
Ultrasonic waves are widely employed in medical diagnosis and non-destructive testing to observe the condition of fetuses and to study non-transparent materials, respectively. Although ultrasonic waves are mostly applied to relatively large-scale structures, megahertz ultrasound has been utilized to investigate the microstructure of particulate matter and the local dynamics of soft matter. More recently, due to the development of high-speed recording technology with large memory storage and sophisticated techniques employing scattered amplitude and phase, analyses of the dynamics as well as the structures of highly turbid suspensions are possible for a wide range of concentrations and particle sizes (several tens of nanometers to several tens of micrometers) using new routes. The technology could simultaneously allow the investigation of complex dynamics involving the Brownian motion of nanoparticles and sedimentation due to the formation of large aggregates. The advantages of using ultrasound are not only the applicability to optically turbid systems but also the wave characteristics related to mechanical (viscoelastic) information, allowing one to evaluate the elastic moduli of particular components, e.g. the elastic shell of a microcapsule immersed in liquid without dilution or drying of the sample. In this paper, the recent developments of novel ultrasound techniques for soft matter characterization are reviewed.
“…Later, several authors have used the same kind of technique to determine the mass density of liquids. [4][5][6] Recently, a line-slab-line system was implemented to accurately determine the acoustic attenuation in a liquid layer from the analysis of the reflection of L pulses. 7 This technique has been used later to monitor the polymerization of an epoxy layer from the determination of L velocity and attenuation in epoxy.…”
We present a technique for determining the rheology of visco-elastic materials in the ultrasonic frequency range based on the measurement of the longitudinal and shear waves reflected and transmitted by a slab of material with a controlled thickness sandwiched between two delay lines. The high sensitivity of this Fabry-Pérot resonator-based technique allows one to access characteristic relaxation times associated with visco-elasticity. As a useful application of the technique, we characterize the Olympus SWC-2 shear-wave couplant in the 0.7–5 MHz frequency range.
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