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At least 343 records · Page 19Linked to original sources
PubMed1988

In vivo and in vitro ultrasound beam distortion measurements of a large aperture and a conventional aperture focussed transducer.

Ultrasound focussing through human tissue of thicknesses varying from 10 mm to 35 mm has been measured for two transducers with diameters 50 mm and 19 mm both focussed at 50 mm (f/1 and f/2.6, respectively). Comparisons are made between the two-way focal depth beam patterns obtained in water and those obtained after passage through tissue to study the degrading effects of frequency-dependent attenuation and inhomogeneities, and their dependence on aperture size. The effects of frequency-dependent attenuation is to broaden the beam and shorten the focal distance. Inhomogeneities mainly increase the sidelobe levels and cause deviations from the central beam axis. A direct comparison of the beam patterns of the two transducers after passage through the same tissue samples shows that the resolution is improved by using the larger aperture. The use of the larger transducer in the in vitro measurements on three human liver specimens demonstrated an average improvement in the -6 dB beamwidth, over the smaller transducer, of 42% (standard deviation +/- 3%). The average improvement in the in vivo measurements on ten female breasts was 34% (standard deviation +/- 5%). The measured improvement in water was 52%. Therefore, the measured resolution improvement in tissue is approximately 2/3 of that obtained in water. The results indicate that for an f/1 transducer with a focal depth of 50 mm the upper limit of maximum useful aperture size has not been reached.

Animals↗
PubMed1996

The effect of variations in transducer position and sound speed in intravascular ultrasound: a theoretical study.

The intravascular insonation of a blood vessel in the presence of an impedance interface between blood and the inner vessel wall is studied theoretically. The model, which uses a ray approximation, is three dimensional and allows consideration of arbitrary noncircular lumen shapes. Model results are presented for the image geometry, and the insonating intensity over the vessel wall. It is shown that the inner lumen can be imaged accurately with the transducer at any position within the lumen, and at any forward viewing angle, provided the point of origin of the beam is stationary. If it is not stationary but rotating with the same angular velocity as the beam itself, the inner vessel wall is not mapped accurately. A particular geometric distortion which has been observed in practice is predicted if the transducer is near vessel wall. Acoustic impedance interfaces will be encountered in vascular disease because the speed of sound in fatty plaque is less than in blood, whereas the speed of sound in fibrous and calcified plaque is greater than in blood. A simplified model representation of an atherosclerotic lumen in developed using a cardioid-like curve and a single impedance interface. Model results show that refraction at this interface leads to an intensity distribution which is not uniform around the lumen, and which depends on lumen shape and transducer position. The exception is the special case of a circular lumen with a centrally positioned transducer. Noncircular impedance interfaces encountered in vivo in vascular disease may cause considerable intensity distortion, particularly if the transducer is close to the wall in an irregularly shaped lumen.

Arteriosclerosis↗
PubMed2006

Comparison of low and high frequency transducers in the detection of liver metastases.

BACKGROUND AND AIMS: To evaluate the benefit of the additional use of a high frequency ultrasound probe (7.5 MHz) in finding suspicious liver lesions compared to the examination using a 3.5-MHz transducer only. PATIENTS AND METHODS: One hundred and fifty-seven patients with underlying malignant disease were examined with both transducers using one of three ultrasound machines (Siemens Sonoline Elegra, GE Healthcare Logic 9, or Hitachi EUB-8500). Findings on hepatic lesions were collected on a standardised documentation sheet and evaluated by descriptive statistics. RESULTS: Ninety-three patients (59.2% of all patients) showed no evident liver lesion on conventional ultrasound with the 3.5 MHz probe. In 29 patients (18.5%) new suspicious liver lesions were found by using the high frequency transducer. Thirteen of these 29 patients (44.8%) were suspected to suffer from diffuse infiltration of the liver with malignant lesions or at least 10 additional visible lesions. In 14 patients, no liver lesion had been known before high frequency ultrasound examination. The size of newly described liver lesions ranged from 2 mm to 1.5 cm. Time needed for the additional examination with the high frequency transducer ranged between 1 and 15 min with an average of 4.0 min. CONCLUSION: The additional use of a high frequency transducer in patients with underlying malignant disease slightly extends the examination time, but reveals new, potentially malignant hepatic lesions in almost every fifth patient.

Adult↗
PubMed2005

Relationship between transducer type and low-frequency hearing loss for patients with ventilation tubes.

OBJECTIVE: To determine the relationship between the type of transducer used to perform pure-tone audiometry and the appearance of low-frequency hearing loss at 250Hz and 500Hz for patients with ventilation tubes. METHODS: Air conduction thresholds at 250Hz and 500Hz were measured using Telephonics TDH-49 supra-aural headphones and EARTONE 3-A insert earphones for patients with normal ears (N=16) and patients with ventilation tubes (N=114). Tympanometry was performed on each patient prior to audiometric testing. Audiometric test results obtained in normal ears were compared to results for patients with ventilation tubes. For analysis, the ventilation tube patients were separated into two groups, representative of ventilation tube type. RESULTS: Audiometric results obtained using the two transducer types at 250Hz and 500Hz revealed significant differences in threshold for patients with ventilation tubes. Thresholds obtained using insert earphones were generally worse than thresholds obtained using supra-aural headphones for this group. On average, difference in threshold was 14.15dB worse with insert earphones at 250Hz and 9.75dB worse with insert earphones at 500Hz for patients with Sheehy tubes. Average difference in threshold for patients with Donaldson tubes was 13.93dB worse with insert earphones at 250Hz and 8.93dB worse with insert earphones at 500Hz. In addition, thresholds were more variable for patients with ventilation tubes than normal ears at 500Hz. There were no significant differences in threshold for normal ears using both transducers. CONCLUSIONS: When performing pure-tone audiometry, choice of transducer can influence the accurate identification of a low-frequency hearing loss in patients with ventilation tubes. Low-frequency thresholds were generally worse using insert-style earphones to test subjects with tubes, resulting in the apparent identification of a hearing loss. However, with supra-aural headphones, no low-frequency hearing loss existed. There were no significant differences in threshold values using either transducer in normal ears.

Acoustic Impedance Tests↗
PubMed2004

First experience in human beings with a permanently implantable intrasac pressure transducer for monitoring endovascular repair of abdominal aortic aneurysms.

OBJECTIVES: Endovascular stent graft repair of abdominal aortic aneurysms (AAAs) prevents rupture by excluding the aneurysm sac from systemic arterial pressure. Current surveillance protocols after endovascular aneurysm repair (EVAR) follow secondary markers of sac pressurization, namely, endoleak and sac enlargement. We report the first clinical experience with the use of a permanently implantable, ultrasound-activated remote pressure transducer to measure intrasac pressure after EVAR. METHODS: Over 7 months, 14 patients underwent EVAR of an infrarenal abdominal aortic aneurysm with implantation of an ultrasound-activated remote pressure transducer fixed to the outside of the stent graft and exposed to the excluded aortic sac. Twelve patients received modular bifurcated stent grafts, and 2 patients received aortouniiliac devices. Intrasac pressures were measured directly with an intravascular catheter and by the remote sensor at stent-graft deployment. Follow-up sac pressures were measured with a remote sensor and correlated with systemic arterial pressure at every follow-up visit. Mean follow-up was 2.6 +/-1.9 months. RESULTS: Excellent concordance was found between catheter-derived and transducer-derived intrasac pressssure intraoperatively. Pulsatile waveforms were seen in all functioning transducers at each evaluation interval. One implant ceased to function at 2 months of follow-up. In 1 patient a type I endoleak was diagnosed on 1-month computed tomography (CT) scans; 3 type II endoleaks were observed. Those patients with complete exclusion of the aneurysm on CT scans had a significant difference in systemic and sac systolic pressures initially (P <.001) and at 1 month (P <.001). Initial sac diastolic pressures were higher than systemic diastolic pressures (P <.001). The ratio of systemic to sac systolic pressure increased over time in those patients with complete aneurysm exclusion ( P <.001). Four of 6 patients with no endoleak and greater than 1-month follow-up had diminution of sac systolic pressure to 40 mm Hg or less by 3 months. CONCLUSION: This is the first report of a totally implantable chronic pressure transducer to monitor the results of EVAR in human beings. Aneurysm exclusion leads to gradual diminution of sac pressure over several months. Additional clinical follow-up will be necessary to determine whether aneurysm sac pressure monitoring can replace CT in the long-term surveillance of patients after EVAR.

Angioplasty↗
PubMed2004

A cam-displacement transducer device for measuring small two-degree of freedom inter-component motion in a prosthesis.

An electromechanical system is described that comprises a cam and two linear displacement transducers for measuring two-degree of freedom. This is aimed at quantifying the extent and pattern of both transverse rotation and longitudinal translation that takes place during amputee gait at what is sometimes termed a "torque-shock absorbing adapter" located between the prosthetic socket and foot. Both types of motion are measured independently by mounting the cam around the adapter and the two transducers orthogonal to one another with their spring loaded plungers moving separately against the cam's perimeter and distal, flat face. The cam geometry should be an arc of a spiral and not a circle for the angular displacement measurement to be linear in response to rotation. Over a range of +/-18 degrees for transverse rotation the maximum deviation of the ideal cam geometry away from an arc of a circle is less than +/-0.5% of the transducers' 10 mm stroke. The transducer's linearity is +/-2% and it could therefore be assumed that this would be the dominant source of error. The theoretical predictions are supported by the calibration results, in which the pattern of errors that are found in the transducers' calibration can also be seen in the calibration of the cam.

Artificial Limbs↗
PubMed2006

Resonance frequency analysis of implants in the guinea pig model: influence of boundary conditions and orientation of the transducer.

The goal of this study was to identify the parameters that must be controlled during in vivo resonance frequency measurements with a custom Osstell transducer for custom implants in the guinea pig animal model. A numerical study and in vitro measurements were performed to determine the influence of the boundary conditions as well as the transducer orientation on the resonance frequency measured by the custom Osstell transducer. In the reported guinea pig model, the type of boundary condition, the orientation of the transducer (parallel or perpendicular to the long axis of the bone) and the length of the modelled bone have a large influence on the resonance frequency values. This implies that a follow-up in time of the stability of an implant requires the boundary conditions applied to the bone in which the implant is installed as well as the orientation of the transducer to be highly repeatable. Applying controlled boundary conditions during in vivo measurements had a highly positive influence on the repeatability of the Osstell measurements. This improves the possibility of the technique to measure changes in the implant-bone interface during healing of the implant.

Animals↗
PubMed2006

Design and modeling of inversion layer ultrasonic transducers using LiNbO3 single crystal.

Using inversion domain engineering controlled by heating temperature, the LiNbO(3) (LNO) piezoelectric plate with both odd and even-order thickness-extensional modes can be excited simultaneously. Therefore, the inversion layer ultrasound transducer is expected to be capable of operating over a wider frequency range. In this paper, the electrical impedance and the acoustic characteristics of LiNbO(3) (LNO) inversion layer transducer have been studied by finite element modeling (FEM). The transducer designed for this study uses a 36 degrees rotated Y-cut LiNbO(3) thin plate with an active element thickness of approximately 100 microm. First the electrical and elastic properties of the 36 degrees rotated Y-cut LNO were obtained by transforming a basic piezoelectric matrix for Z-cut LNO. In order to validate the FEM using the transformed properties several pieces of pure and 50% inversion layer LNO were tested on the electrical impedance analyzer. The modeled impedance characteristics were consistent with the measured data. Next the model was used to design 50-60 MHz transducers using pure and 30% inversion LNO. Two lambda/4 matching layers and a Tungsten loaded epoxy backing were used in these designs. The modeled results show that an over 90% bandwidth transducer can be made with proper matching and 30% inversion layer.

Computer Simulation↗
PubMed2006

Study on the radial composite piezoelectric ceramic transducer in radial vibration.

A new type of radial composite piezoelectric transducer in radial vibration is developed and analyzed. The radial composite transducer consists of a piezoelectric ceramic thin ring polarized in the thickness direction and a metal thin circular ring. They are connected together and excited to vibrate in the radial direction. The radial vibrations of a piezoelectric ceramic thin ring and a metal thin circular ring are analyzed, respectively. Their radial electro-mechanical equivalent circuits are obtained. Based on the electro-mechanical equivalent circuits and using the boundary conditions between the piezoelectric ceramic thin ring and the metal thin circular ring in the radial direction, the electro-mechanical equivalent circuit of the radial composite piezoelectric transducer is derived out and the resonance frequency equation is obtained. The relationship between the resonance frequency and the geometrical dimensions of the transducer is analyzed. Some radial composite piezoelectric transducers are designed and manufactured. The resonance frequencies and the anti-resonance frequencies, the electro-mechanical equivalent circuit parameters are measured. The effective electro-mechanical coupling coefficient and the mechanical quality factor are calculated. It is illustrated that the measured radial resonance frequencies are in good agreement with the theoretical results from the resonance frequency equation.

Ceramics↗
PubMed2005

Model-based optimization of ultrasonic transducers.

Numerical simulation and automated optimization of Langevin-type ultrasonic transducers are investigated. These kind of transducers are standard components in various applications of high-power ultrasonics such as ultrasonic cleaning and chemical processing. Vibration of the transducer is simulated numerically by standard finite element method and the dimensions and shape parameters of a transducer are optimized with respect to different criteria. The novelty value of this work is the combination of the simulation model and the optimization problem by efficient automatic differentiation techniques. The capabilities of this approach are demonstrated with practical test cases in which various aspects of the operation of a transducer are improved.

Computer Simulation↗
PubMed2000

Factors influencing the output of an implantable force transducer.

The objective of this study was to evaluate the performance of the Arthroscopically Implantable Force Probe (AIFP; MicroStrain, Burlington VT) for measuring force in a patellar tendon graft. Transducer drift, reproducibility of output due to the number of loading cycles and device location, and sensitivity to the tendon cross-sectional area were investigated. The AIFP was initialized, and then implanted into five human patellar tendon grafts three times; twice within the same location and once in a different location. The tendons were cyclically loaded in uniaxial tension for 500 cycles in each insertion site. The AIFP was then removed from the tendon and the baseline output was remeasured. It was determined that transducer drift was negligible. The relationship between the tensile load applied to the graft and AIFP output was quadratic and specimen dependent. The cyclic load response of the tendon-AIFP interface demonstrated a 24.9% decrease over the first 20 loading cycles, and subsequent cycling yielded relatively reproducible output. The output of the transducer varied when it was removed from the tendon and then reimplanted in the same location (range 3.7-109. 4% error), as well as in the second location (range 1.5-202.8% error). No correlation was observed between the cross-sectional area of the tendon and transducer output. This study concludes that implantable force probes should be used with caution and calibrated without removing the transducer from the graft.

Aged↗
PubMed2000

Application of different spatial sampling patterns for sparse array transducer design.

In the last few years, the efforts of many researchers have been focused on developing 3D real-time scanners. The use of 2D phased-array transducers makes it possible to steer the ultrasonic beam in all directions in the scanned volume. An unacceptably large amount of transducer channels (more than 4,000) must be used, if the conventional phased array transducers are extrapolated to the 2D case. To decrease the number of channels, sparse arrays with different aperture apodization functions in transmit and receive apertures have to be designed. The design is usually carried out in 1D, and then transferred to a 2D rectangular grid. In this paper, five different 2D array transducers have been considered and their performance was compared with respect to spatial and contrast resolution. An optimization of the element placement along the diagonals using vernier arrays is suggested. The simulation results of the ultrasound fields show a decrease in the grating-lobe level of 10 dB for the diagonally optimized 2D array transducers compared to the previously designed 2D arrays which did not consider the diagonals.

Computer Simulation↗
PubMed2001

Transducer models of head-centred motion perception.

By adding retinal and pursuit eye-movement velocity one can determine the motion of an object with respect to the head. It would seem likely that the visual system carries out a similar computation by summing extra-retinal, eye-velocity signals with retinal motion signals. Perceived head-centred motion may therefore be determined by differences in the way these signals encode speed. For example, if extra-retinal signals provide the lower estimate of speed then moving objects will appear slower when pursued (Aubert-Fleischl phenomenon) and stationary objects will move opposite to an eye movement (Filehne illusion). Most previous work proposes that these illusions exist because retinal signals encode retinal motion accurately while extra-retinal signals under-estimate eye speed. A more general model is presented in which both signals could be in error. Two types of input/output speed relationship are examined. The first uses linear speed transducers and the second non-linear speed transducers, the latter based on power laws. It is shown that studies of the Aubert-Fleischl phenomenon and Filehne illusion reveal the gain ratio or power ratio alone. We also consider general velocity-matching and show that in theory matching functions are limited by gain ratio in the linear case. However, in the non-linear case individual transducer shapes are revealed albeit up to an unknown scaling factor. The experiments show that the Aubert-Fleischl phenomenon and Filehne illusion are adequately described by linear speed transducers with a gain ratio less than one. For some observers, this is also the case in general velocity-matching experiments. For other observers, however, behaviour is non-linear and, according to the transducer model, indicates the existence of expansive non-linearities in speed encoding. This surprising result is discussed in relation to other theories of head-centred motion perception and the possible strategies some observers might adopt when judging stimulus motion during an eye movement.

Eye Movements↗
PubMed1996

Earlens tympanic contact transducer: a new method of sound transduction to the human ear.

This article is an initial report on a new method of transducing sound to the human ear. The report describes the shortcomings of conventional acoustic amplification devices, the potential advantages afforded by the Earlens system (ReSound Corp., Redwood City, Calif.), a description of the system, and preliminary clinical results. The system is composed of two elements: a transducer that is composed of a magnet mounted on a thin, conical silicone platform and a device that generates a magnetic field which causes the Earlens to vibrate. The Earlens transducer is placed on the umbo area of the tympanic membrane and maintains its position there by floating on a droplet of mineral oil. Two configurations of the magnetic field device are described: one that is placed within the external auditory canal and another that is worn around the neck. This feasibility study was done in seven patients during a 3-month period. All patients in the study maintained the position of the transducer for the duration of the study, and the tympanic membranes showed no evidence of inflammation or other problems. The presence of the transducer caused an average 5-dB threshold depression in the speech frequencies. In the neck-worn device, maximum mean functional gain was 25 dB at 2000 Hz. Variability in the functional gain at different frequencies was noted with poorer gain above 2000 Hz.

Feasibility Studies↗
PubMed2001

Effects of transducer, velocity, Doppler angle, and instrument settings on the accuracy of color Doppler ultrasound.

The accuracy of a commercial color Doppler ultrasound (US) system was assessed in vitro using a rotating torus phantom. The phantom consisted of a thin rubber tube filled with a blood-mimicking fluid, joined at the ends to form a torus. The torus was mounted on a disk suspended in water, and rotated at constant speeds by a motor. The torus fluid was shown in a previous study to rotate as a solid body, so that the actual fluid velocity was dependent only on the motor speed and sample volume radius. The fluid velocity could, thus, be easily compared to the color Doppler-derived velocity. The effects of instrument settings, velocity and the Doppler angle was assessed in four transducers: a 2.0-MHz phased-array transducer designed for cardiac use, a 4.0-MHz curved-array transducer designed for general thoracic use, and two linear transducers designed for vascular use (one 4.0 MHz and one 6.0 MHz). The color Doppler accuracy was found to be significantly dependent on the transducer used, the pulse-repetition frequency and wall-filter frequency, the actual fluid velocity and the Doppler angle (p < 0.001 by analysis of variance). In particular, the phased array and curved array were observed to be significantly more accurate than the two linear arrays. The torus phantom was found to provide a sensitive measure of color Doppler accuracy. Clinicians need to be aware of these effects when performing color Doppler US exams.

Blood Flow Velocity↗
PubMedDate not supplied

Experimental evaluation of indicators of nonlinearity for use in ultrasound transducer characterizations.

Because the number of applications for medical ultrasonic devices continue to increase and, hence, the number of diagnostic ultrasound (US) systems increase, there is a need to reliably characterize the sources in terms of their output pressures. Currently, the transducers are characterized by making pressure measurements in water for every voltage range applied to the source and, then, linearly derate the measured pressure values to estimate the derated acoustic pressure levels. The process is time-consuming and inaccuracies are introduced in the derating process due to nonlinear effects. Therefore, there is a need to find an indicator of nonlinearity that could classify the measured pressure waveform as either linear, where the derating procedure would yield an accurate derated acoustic pressure estimate, or nonlinear, where the derating process would fail. Eight different indicators of nonlinearity were evaluated experimentally using spherically focused US transducers. The transducers were selected to test the indicator sensitivity to frequency (3 to 8 MHz), f-number (1 and 2), and transducer diameter (1.905 and 5.08 cm). Sensitivity to drive voltage conditions was also tested by exciting one of the transducers with pulses of different duration and phase. None of the eight nonlinearity indicators yielded consistent results. The lack of consistency resulted from the competing effects of nonlinear absorption and asymmetrical distortion, which have yet to be combined into a unified theory.

Acoustics↗
PubMedDate not supplied

Intraoperative epicardial echocardiography with a miniature high-frequency transducer: imaging techniques and scanning planes.

Intraoperative Doppler echocardiography has the potential to provide anatomic and functional information but is hindered by the large size of standard transducers. We describe new scanning planes accessible through the application of a new 5 MHz miniature transducer with imaging, Doppler, and color-flow capability. Epicardial echocardiography was performed in 15 adults undergoing elective coronary artery bypass grafting. Standard parasternal equivalent, subcostal equivalent, aortopulmonary sulcus and aortosuperior vena caval views were obtained. Previously unobtainable apical four-chamber, five-chamber, and long-axis views were possible by positioning the transducer at the apex. The transducer has a broad bandwidth, allowing high-quality imaging at different depths and could be maneuvered laterally, posteriorly, and over the aorta and pulmonary arteries to provide off-axis views. The proximal-mid coronary arteries were imaged on the beating heart with a standoff medium. Transducer miniaturization should expand the role of epicardial ultrasonography in the surgical management of heart disorders.

Adult↗
PubMed1997

Comparison of lower oesophageal sphincter pressure measurement using circumferential vs unidirectional transducers.

UNLABELLED: Average values from unidirectional (UND) transducers have traditionally been used in standard manometric evaluation of lower oesophageal sphincter pressures (LOSPs). A single circumferential (CMF) transducer has recently become popular. Our aim was to compare LOSP measurements made using the two techniques. Ten healthy volunteers were intubated with a Konigsberg manometry catheter containing five solid-state transducers (four unidirectional at 90 degrees angles radially and 2.5-cm intervals and one circumferential, 3 cm distal). LOSP was measured using the station pull-through technique in the supine and upright positions with Synectics Polygram software for computerized analysis. Mean UND pressures were plotted against CMF pressures and a linear regression and correlation analysis was performed. A similar analysis was done for LOS length. A significant difference (P < 0.01) was found between mean (+/- SE) supine and upright LOSPs for both mean UND (20.21 +/- 1.36 vs 15.56 +/- 1.28 mmHg) and CMF (20.41 +/- 1.96 vs 16.17 +/- 1.61 mmHg); however no difference was shown between supine and upright lengths. There was a high degree of correlation between LOSP (r = 0.83) and a weaker correlation (r = 0.65) between LOS lengths when measured by CMF and UND transducers. CONCLUSION: UND and CMF transducers provide identical measurements when evaluating the LOS.

Adolescent↗