Kinnick, Randall R.

The ultrasound radiation force can be used as a noncontact method for exciting vibrational modes. In one implementation, an audio-range modulation signal is combined with a 40-kHz carrier to form a double-sideband suppressed-carrier (DSSC) waveform that is emitted from an ultrasound transducer. The frequency of the ultrasound radiation force is the difference between the frequencies of the sidebands, therefore at twice the modulation frequency. We describe a method for selective mode excitation using a transducer pair, each emitting a DSSC signal. The modulation signal for one transducer was phase shifted relative to the other transducer. When the two modulation signals were in phase, the radiation stress field was uniform. For devices studied, this excited transverse modes while suppressing torsional modes. Similarly, if the modulation signals were out of phase, torsional modes were excited while suppressing transverse modes. This technique has been demonstrated for devices including an MEMS mirror, hard-drive suspension, and brass cantilever. For a cantilever, the ratio of the amplitudes of 180-Hz transverse over 1.3-kHz torsional modes was varied by over two orders of magnitude by shifting the phase difference between the two beams over a range of 90 deg. This noncontact technique allows control over the types of vibration excited.

We have proposed generating a bending wave in the arterial wall using ultrasound radiation force and measuring the wave velocity along the arterial wall [Zhang et al., IEEE Trans. Ultrason. Ferroelectr. Freq. Control 52, 642–652 (2005)]. Here, we report the results of in vivo studies on pigs. The pig was anesthetized, and a micromanometer tip catheter was inserted into the femoral artery to measure luminal pressure. A water bath was created on the animal’s groin to allow unimpeded access of the ultrasound beams to the femoral artery. The femoral artery was first located using a 13-MHz linear-array transducer. Then, a vibro-acoustography image was obtained to ensure precise positioning of the excitation force relative to the artery. The artery was excited by the force transducer and the resulting vibration of the arterial wall was measured by a sensing Doppler transceiver. Measured wave velocity was 3.1 m/s at 300 Hz. With this new method wave velocity over a distance of 5 mm, and therefore stiffness of arteries, can be measured locally and non-invasively. Measurement time is short in a few tens of milliseconds, which allows pressure dependence and pharmacological effect on the wall properties to be measured at different cardiac times.

The head-gimbal assembly suspension is a cantilever-like structure that holds the heads on a hard drive. We will discuss a noncontact method for modal testing, of suspensions in air, that utilizes the radiation force at the difference frequency generated by two intersecting ultrasound beams. The resulting low-frequency excitations were measured using a scanning vibrometer. This excitation technique has been demonstrated for MEMS and other small devices. There are several unique advantages of the ultrasound radiation force relative to mechanical shakers. Since the ultrasound radiation force is noncontact, a specialized test fixture was not needed; the technique was relatively insensitive to distracting resonances of fixtures and support structures. Another advantage is broadband excitation; a 550-kHz confocal ultrasound transducer excited suspension resonance frequencies from under 1 kHz to over 50 kHz. Other advantages include the ability to selectively excite different modes. For example, the amplitude of the suspension’s 2.28-kHz transverse mode was suppressed by an order of magnitude by shifting the modulation phase between the two ultrasound beams by 90. In another test, the amplitude of the 6.01-kHz torsional mode was doubled by moving the ultrasound focus point from near the center to near the edge of the suspension.

In vitro studies have shown that treatment with 1.5 MHz ultrasound signal (160 mW/cm2) at a 200 μs tone burst repeating at 1 kHz increases proteoglycan synthesis in chondrocytes [J. Parvisi et al., J. Orthop. Res. 17, 488–494 (1999)]. It was hypothesized that a continuous 1 kHz signal would be similar to the pulsed 1.5 MHz signal in stimulating chondrocytes to produce proteoglycan, which may cause accelerated fracture healing. In vitro experiments were performed with ATDC5 cells, a chondrogenic clonal cell line, plated in 6-well plates for 3 to 7 days before receiving ultrasound treatments. Cells were treated with either 1.5 MHz pulsed signal or 1 kHz signal for 20 minutes per day for 9 to 11 days. The signals were calibrated so that the bottom of the 6-well plate moved 10 nm for each condition. After the final treatment, cell layers were stained with Alcian blue, which stains cartilage nodules providing a measure of chondrogenesis. Both 1.5 MHz and 1 kHz led to a highly significant increase in chondrogenesis compared to control. Quantitative image analysis of stained wells showed that treatments with either signal increased number of nodules 2.3-fold (p<0.02) and total area of nodules 3-fold (p<0.02) compared to controls.

With the advent of MEMS, modal analysis of small structures is increasingly important. However, conventional excitation techniques normally require contact, which may not be feasible for small objects. We present a non-contact method that uses interference of ultrasound frequencies in air to produce low-frequency excitation of structures. Objects studied included hard-drive HGA suspensions and MEMS devices. The vibration induced by the ultrasound radiation force was varied in a wide range from 0 Hz to 50 kHz. Object motion was detected using a laser vibrometer; measured frequencies agreed with expected values. Also demonstrated was the unique capability to selectively enhance or suppress modes independently. For example, the ratio of the vibrational amplitudes of the 175 Hz first-bending and 1.33 kHz torsional modes of a small cantilever could be changed from in excess of 10:1 to less than 1:10 by shifting the ultrasound modulation phase 90 degrees. Similar changes were obtained for a 3 mm square MEMS mirror in the ratios of vibration amplitude around its two separate axes. Torsional modes of a hard-drive suspension could be selectively enhanced by over a factor of two by moving the ultrasound focus point from near the center to near the edge of the suspension.

Arterial wall stiffness can be associated with various diseases. The stiffness of an artery can be assessed by measurement of the pulse wave velocity (PWV). PWV is directly related to the Youngs modulus by the well-known Moens–Korteweg equation. Usually, PWV is estimated using the foot-to-foot method. However, the foot of the pressure wave is not very clear due to reflected waves. Also, the pressure wave is normally at a low frequency, hence, the time resolution is low. PWV is an average indicator of artery stiffness between the two measuring points, therefore it is not easy to identify local stiffness. We propose producing a very short pulse wave in the arterial wall using ultrasound radiation force and measuring its propagation speed along the artery by laser. The temporal resolution of this method is in the range of microseconds, which allows PWV to be measured accurately over a few millimeters. Experiments were carried out on a silicone tube in gelatin. PWV was measured by two scanning methods: (1) fixed source and scanning detector, (2) scanning source and fixed detector. Results: PWV was measured at 2 mm/40 μs by both methods. The Doppler technique was also tested which is potentially suitable for clinical applications.

Vibro-acoustography is an imaging technique that maps the acoustic response of an object to a localized harmonic radiation force. This force is generated by two interfering continuous-wave ultrasound beams at slightly different frequencies f1 and f2. The system point-spread function (PSF) is related to the radiation force on a point-target. Imaging artifacts depend on the PSF sidelobes, which can be reduced by mismatching the sidelobes of each ultrasound beam. Here, we propose a beamforming approach based on an 8-element sector transducer with consecutive elements alternately driven at f1 and f2. The transducer generates two ultrasound beams skewed by 22.5° with respect to each other. The system PSF is analytically derived. The theory is validated by experiments using a small steel sphere (radius =0.2 mm) as a point-target. A laser vibrometer is used to measure the vibration of the sphere and evaluate the PSF of the system. Theoretically, the PSF sidelobes are under −15.8 dB in eight spots circularly distributed and separated by 22.5°, which agrees with the experimental results. Simulation shows that with 16 elements sidelobes are under −35.2 dB. In conclusion, sector transducers for vibro-acoustography may have lower sidelobes as the number of array elements is increased. [Work supported by Grant Nos. EB00535-01, EB2640, and IMG0100744.]

Ultrasound (US) enhancement of plasmid-based gene transfer is an emerging technique. Our hypothesis was that two contrast agents (Optison and PESDA), and two US exposure modalities (dedicated continuous wave system and diagnostic scanner) may have different effects. Luciferase plasmid with or without contrast agent was added to vascular smooth muscle cells and endothelial cells, followed by US exposure. Luciferase activity was measured 24 h later. US exposure consistently induced higher transfection rates than all controls. PESDA was superior to Optison in both cell lines. In vitro, continuous wave and diagnostic US were not significantly different. In vivo, Lux and PESDA were injected into skeletal muscles of rats (IM or intra-arterial) followed or not by US exposure. In separate animals, adenovirus encoding for luciferase was injected IM and was not followed by US exposure. Gene transfer efficacy was 8–10 fold higher with US and PESDA than with plasmid alone, but 2 fold lower than with adenovirus. However, as opposed to adenovirus, US-enhanced plasmid gene transfer was highly localized to the injected muscle, with no expression at distal sites. Our results support the hypothesis that contrast agents and exposure modalities are not equivalent with regard to gene transfer efficacy.

The goal of this experiment was to excite and measure, in a noncontact manner, the vibrational modes of the reed from a reed organ pipe. To perform ultrasound stimulated excitation, two ultrasound beams in air of different frequencies were directed at the reed; the audio-range beat frequency between these ultrasound beams induced vibrations. The resulting vibrational deflection shapes were measured with a scanning vibrometer. The modes of any relatively small object can be studied in air using this technique. For a 36 mm by 7 mm clamped brass reed cantilever, displacements and velocites of 5 μ and 4 mm/s could be imparted at the fundamental frequency of 145 Hz. Using the same ultrasound transducer, excitation across the entire range of audio frequencies was obtained, which was not possible using audio excitation with a speaker. Since the beam was focused on the reed, ultrasound stimulated excitation eliminated background effects observed during mechanical shaker excitation, such as vibrations of clamps and supports. We will discuss the results obtained using single, dual, and confocal ultrasound transducers in AM and unmodulated CW modes, along with results obtained using a mechanical shaker and audio excitation using a speaker.

Characterization of the viscoelastic mechanical properties of skin is important for improving accurate medical examination and diagnosis of disorders involving cutaneous and subcutaneous tissues; more thoroughly understanding skin biophysical and physiological properties; identifying normal and abnormal skin aging and disease processes; developing and applying improved pharmacologic and other therapeutic interventions; as well as cosmetic applications. Several noninvasive methods have been developed for measurement of mechanical properties of skin [1]. However, most methods measure a stiffness parameter but not the material properties of skin. For example, the suction method measures the displacement of skin in response to suction. The measurement is dependent on the aperture and fixation of probes and also difficult to interpret.