ArticlePDF Available

Design of a High Frequency Driving Circuit of Surface Acoustic Wave Transducer

Authors:
Open Access Library Journal
2018, Volume 5, e4737
ISSN Online: 2333-9721
ISSN Print: 2333-9705
DOI:
10.4236/oalib.1104737 Jul. 25, 2018 1 Open Access Library Journal
Design of a High Frequency Driving Circuit of
Surface Acoustic Wave Transducer
Guan Zhao
Automotive Engineering College, Shanghai University of Engineering Science, Shanghai, China
Abstract
In this paper, a high frequency driving circuit of surface acoustic wave tran
s-
ducer has been designed to separate oil from oil/water mixed droplet. The
transmission frequency of the surface acoustic wave transducer driving circuit
can be up to 1 MHz. The transmit frequency of conventional ultrasonic dri
v-
ing circuit is mostly 40 kHz.
However, the high transmit frequency driving
circuit presents a good stability and accuracy. By establishing the
surface
acoustic wave driving circuit model, the actual circuit and debugging verific
a-
tion, the driving circuit can excite the frequency signal required for the exp
e-
riment. Thus, the surface acoustic wave driving circuit could provide nece
s-
sary technical support for application in other fields.
Subject Areas
Applied Physics, Electric Engineering
Keywords
Surface Acoustic Wave, Driving Circuit, High Frequency, Transducer
1. Introduction
With the development of industry and the advancement of science and technol-
ogy, ultrasonic technology has been widely developed and used. Ultrasonic
technology has long been gradually integrated into people’s daily lives to become
an inseparable part. Ultrasonic technology has been applied in various fields,
which is usually divided into two major categories of ultrasonic testing and
power ultrasound [1]. For example, hospitals use B-ultrasound to diagnose dis-
eases [2], which is simple, convenient, high diagnostic accuracy. Above all, it can
prevent patients from suffering unnecessary pain. M Yamamoto
et al.
[3] used
How to cite this paper:
Zhao, G. (2018)
Design of a High Frequency Driving Circuit
of Surface Acoustic Wave Transducer
.
Open
Access
Library Journal
,
5
: e4737.
https://doi.org/10.4236/oalib.1104737
Received:
June 24, 2018
Accepted:
July 22, 2018
Published:
July 25, 2018
Copyright
© 2018 by author and Open
Access
Library Inc.
This
work is licensed under the Creative
Commons
Attribution International
License
(CC BY 4.0).
http://creativecommons.org/licenses/by/4.0/
Open Access
G. Zhao
DOI:
10.4236/oalib.1104737 2 Open Access Library Journal
ultrasonic technology to design a sewage flow measurement system and suc-
cessfully achieved accurate measurement of sewage flow. Zhang
et al. [4]
suc-
cessfully designed a car anti-collision system using ultrasonic wireless transmis-
sion and ultrasonic ranging technology. J Tsujino [5] studied the latest technol-
ogy of ultrasonic welding, and Qiu
et al.
[6] conducted numerical simulation
and analysis of ultrasonic traveling wave driving droplet motion on the glass
surface.
However, for practical applications in these fields of ultrasonic technology,
the driving frequency of the drive circuit is mostly 40 kHz, and it is rare for the
high frequency of 1 MHz for the transmission frequency. Therefore, in order
to improve the accuracy, stability, and reliability of related ultrasound experi-
ments. In this paper, a surface acoustic wave transducer driving circuit with a
transmission frequency of up to 1 MHz is designed. Through appropriate de-
bugging, this circuit can stimulate the waveforms required for the experiment
and achieve the functions required to separate oil from an oil/water mixed
droplet.
2. Theory of Surface Acoustic Wave Driving Circuit
In recent years, surface acoustic wave (SAW) technologies have received signifi-
cant attention to be applied in various fields. And the (SAWs) have been used to
drive and manipulate microfluidic flow, such as Rayleigh [7] [8] and Lamb
waves [9] [10]. Some researchers have applied the SAW technologies to make
SAW transducers, which the device can convert electrical energy into sound
energy and convert sound energy into electrical energy. And these technical
characteristics are usually applied in microfluidics community, such as acoustic
microreactors [11], and microseparattors [12].
On the basis of the several potential applications of droplet propulsion and
emulsion separation by using the ultrasonic waves, the SAW driving circuit
could be applied to separate two immiscible liquids. In this study, the surface
acoustic wave driving circuit has functions of operate at high frequency, good
install, low cost, and high efficiency. Flow chart of the SAW driving circuit de-
sign shows in Figure 1.
3. Driving Circuit Design
There are some conventional ultrasonic driving circuits that are used in various
fields [13] (shown in Figures 2-5). However, one of the biggest drawbacks of
these driving circuits is that the frequencies are all 40 kHz, which is not suffi-
cient for the unique field and experiment requirements.
In this design, the function of driving circuit is to amplify the input voltage
through corresponding electronic components and generate SAW with a specific
power, a specific pulse width, and a regular frequency to excite the transducer.
And the driving circuit can obtain the requirements for experiment. The sche-
matic of SAW driving circuit as shown in Figure 6.
G. Zhao
DOI:
10.4236/oalib.1104737 3 Open Access Library Journal
Figure 1. Flow chart of the SAW driving circuit design.
Figure 2. Self-excited driving circuit.
Figure 3. SCR drive circuit.
Figure 4. Dedicated integration of driving circuit.
The schematic of SAW driving circuit is to input DC voltage, which output
interface attained 1 MHz attenuation sine wave pulse. Thus, function of this
driving circuit can be seen as an inverter circuit, which can convert DC power
supply into AC pulse with a frequency of 1 MHz. The switching diode (1SS360)
is applied to control the function of inverter circuit. The voltage stabilizing cir-
cuit consists of zener diode (IN4007) and rectifier diode (1N4003). There are
some field effect transistors has been applied in this driving circuit to be
G. Zhao
DOI:
10.4236/oalib.1104737 4 Open Access Library Journal
Figure 5. Ultrasound transducer driving circuit com-
posed of 55.
Figure 6. Schematic of SAW driving circuit.
integrated easily. And the integration circuit is used to replace triodes, resis-
tances, and diodes that are needed in this designed. Thus, driving circuit of SAW
is high-precision integration.
The important feature of the SAW driving circuit is different from traditional
circuit, which the frequency can up to 1 MHz. It can present good stability, and
high accuracy to be applied to separate oil from an oil/water mixed droplet. In
this experiment, water droplet and oil droplet are mixed to produce an oil/water
mixed droplet as Figure 7(a). The oil/water mixed droplet will be promoted
under the effect of the SAW streaming forces as Figure 7(b). With the time goes
on, the oil/water mixed droplet will get critical separation position as Figure
7(c). At last, the oil droplet will be separated from an oil/water mixed drop as
Figure 7(d). The experiment phenomenon of oil/water mixed droplet separation
process can be seen in Figure 7. And the output interface can be attain 1 MHz
attenuation sine wave pulse of SAW driving circuit as shown in Figure 8.
4. Conclusion
In this design, the SAW driving circuit output interface attains 1 MHz attenua-
tion sine wave pulse. It presents a good stability, and high accuracy by testing.
And the SAW driving circuit that is designed can separate oil from oil/water
mixed droplet. It could provide a good approach to separate oil/water droplet.
The SAW driving circuit could be applied to other ultrasonic technology field of
G. Zhao
DOI:
10.4236/oalib.1104737 5 Open Access Library Journal
Figure 7. Separation process of oil/water mixed droplet.
Figure 8. Attenuation sine wave pulse of SAW driving circuit.
higher precision requirements in the future. And the SAW driving circuit could
be used to separate two kinds of immiscible liquids.
References
[1] Kinoshita, M.M. (2001) Ultrasonic Testing Improves Power Plant Efficiency.
Tur-
bomachinery International
, 5, 39-40.
[2] Su, L.Y., Sun, C.K. and Zhang, Z. (2013) Comparative Study of the B-Ultrasound
and Molybdenum X-Ray in the Diagnosis of Breast Disease.
Journal of Bengbu
Medical College
,
38, 1471-1472.
[3] Yamamoto. M., Tamura, K., Yanagisita, S. and Inagaki, S. (2009) An Ultrasonic
Flow Measurement System for Sewage and Waste Water.
Transactions of the Socie-
ty of Instrument & Control Engineers
, 14, 564-571.
https://doi.org/10.9746/sicetr1965.14.564
[4] Zhong, Y. and Yu, H. (2016) Design of Car Reversing Anti-Collision Warning De-
vice Based on Ultrasonic Ranging Principle.
Electronic Design Engineering
, 24,
158-161.
[5] Tsujino, J. (1995) Recent Developments of Ultrasonic Welding.
Ultrasonics Sympo-
sium
, 2, 1051-1060. https://doi.org/10.1109/ULTSYM.1995.495743
[6] Qiu, H.C. and Jiang, L.B. (2017) Numerical Simulation of Droplet Motion on Glass
G. Zhao
DOI:
10.4236/oalib.1104737 6 Open Access Library Journal
Surface Driven by Ultrasonic Travelling Wave.
Journal of Beijing University of
Aeronautics & Astronautics
, 43, 908-917.
[7] Kang, K., Lim, H., Lee, H. and Lee, S. (2013) Evaporation-Induced Saline Rayleigh
Convection inside a Colloidal Droplet.
Physics of Fluids
, 25, Article ID: 042001.
https://doi.org/10.1063/1.4797497
[8] Agostini, M., Grecoa, G. and Cecchini, M. (2018) A Rayleigh Surface Acoustic Wave
(R-SAW) Resonator Biosensor Based on Positive and Negative Reflectors with
Sub-Nanomolar Limit of Detection.
Sensors and Actuators B
:
Chemical
, 254, 1-7.
https://doi.org/10.1016/j.snb.2017.07.014
[9] Schmitt, M., Stich, S., Fromm, S., Fischer, F. and Lindner, G. (2010) Detection and
Removal of Droplets on Non-Piezoelectric Substrates via Mode Conversion of
Lamb Waves.
British Journal for the Philosophy of Science
, 143, 304-308.
https://doi.org/10.1109/ICSENS.2010.5689878
[10] Savva, N. and Kalliadasis, S. (2013) Droplet Motion on Inclined Heterogeneous
Substrates.
Journal of Fluid Mechanics
, 725, 462-491.
https://doi.org/10.1017/jfm.2013.201
[11] Dong, Z., Yao, C. and Zhang, Y. (2016) Hydrodynamics and Mass Transfer of Os-
cillating Gas-Liquid Flow in Ultrasonic Microreactors.
AIChE Journal
, 62, 1294-1307.
[12] Watanabe, S., Matsumoto, S. and Higurashi, T. (2015) Almost Complete Separation
of a Fluid Component from a Mixture Using Burgers Networks of Microseparators.
Journal of the Physical Society of Japan
, 84, Article ID: 043401 (1-4).
https://doi.org/10.1002/aic.15091
[13] Tu, X.K., Wu, Y., Li, G.F. and Li, Z.J. (2009) Design of a High Frequency Driving
Circuit of Ultrasonic Wave Transducer.
Electronic Measurement Technology
,
32,
23-25.
ResearchGate has not been able to resolve any citations for this publication.
Article
Full-text available
Two ways of networking microseparators to almost completely separate, for example, hydrogen from a mixture are proposed. Each separator has two outlets for slightly higher and lower concentrations, whose difference is modeled by a quadratic map of the average concentration at its inlet. In the continuum, the networks are governed by the Burgers equation or its variant with no-flux boundary conditions. The initial boundary value problem is exactly solvable. A family of equilibria are global attractors. The target component is shown to be extracted from one side of a stationary shock. Microdevices for testing the idea are also proposed.
Article
Full-text available
Inside evaporating two-component sessile droplets, a family of the Rayleigh convection exists, driven by salinity gradient formed by evaporation of solvent and solute. In this work, the characteristic of the flow inside an axisymmetric droplet is investigated. A stretched coordinate system is employed to account for the effect of boundary movement. A scaling analysis shows that the flow velocity is proportional to the (salinity) Rayleigh number (Ras) at the small-Rayleigh-number limit. A numerical analysis for a hemispherical droplet exhibits the flow velocity is proportional to the non-dimensional number Ras1/2, at high Rayleigh numbers. A self-similar condition is established for the concentration field irrespective of the Rayleigh numbers after a moderate time, and the flow field is invariant with time at this stage. The scaling relation for the high Rayleigh numbers is verified experimentally by using aqueous NaCl droplets.
Article
A label-free sub-nanomolar Rayleigh surface acoustic wave (R-SAW)-based resonator biosensor is demonstrated for biomolecular detection in liquid after drying. The biosensor comprises two interdigital transducers for R-SAW generation and two positive and negative reflectors to confine the acoustic energy in the sensitive area. We benchmark this biosensor against biotin-streptavidin binding, which is a standard, well-known model for a variety of biosensing processes. The experiments demonstrate a limit of detection of 104 pM and a normalized sensitivity of −296 m² kg⁻¹. As a comparison with similar acoustic-wave based systems, both sensitivity and limit of detection are better than that of standard commercial gravimetric sensors (i.e., quartz-crystal-microbalances) and generally better than that of more common Love-SAW biosensors. Our biosensor has a dynamic range potentially compatible with several health- and safety-related assays, among all cancer biomarker detection.
Article
The Hawaiian Electricity Company (HECO) has used a predictive maintenance (PdM) programme using ultrasound, vibration analysis, tribology and infrared thermography to improve efficiency. The PdM programme has included using an Ultraprobe 9000TM ultrasonic system to inspect rolling element bearings and to detect leakage from boiler feed recirculation. Ultrasonic inspection is routinely used to inspect bearings, valves and circuit breakers.
Article
Ultrasonic microreactors were used to intensify gas-liquid mass-transfer process and study the intensification mechanism. Fierce surface wave oscillation with different modes was excited on the bubble. It was found that for slug bubbles confined in smaller microchannel, surface wave oscillations require more ultrasound energy to excite due to the confinement effect. Cavitation microstreaming with two toroidal vortices was observed near the oscillating bubble by a streak photography experiment. Surface wave oscillation at the gas-liquid interface increases the specific surface area, while cavitation microstreaming accelerates the interface renewal and thus improves the individual mass-transfer coefficient. With these two reasons, the overall mass-transfer coefficient was enhanced by 3-20 times under ultrasonication. As for gas-liquid flow hydrodynamics, ultrasound oscillation disturbs the bubble formation process and changes the initial bubble length and pressure drop.
Article
A new ultrasonic flow measurement system has been developed for sewage and waste water flowing in circular conduits with or without free surface. The system is composed of three units, an ultrasonic height gauge to measure depth of water, an ultrasonic doppler velocity meter to measure velocity at a predetermined point in the water and a flow computing unit. The flow computing unit consists of a meter coefficient generator and a multiplier to calculate the product of the meter coefficient and the velocity. We derived the meter coefficient as a function of water depth and geometry of the conduit from theoretical investigation and some experimental work. The validity of the derived coefficient was confirmed by some field tests. The results obtained are summerized as follows: (1) The meter coefficient is independent of the inclination of the flow surface. (2) When a velocity measuring point is set at 0.1D from the bottom (D is the diameter of conduit), the measuring error due to the variation of roughness coefficient may be negligible. (3) The results of the tests show that the accuracy of the system is within ±3% of full scale. The above results are also applied to rectangular channel, but in this case the velocity measuring point should be set at 0.1B from the bottom (B is the width of channel).
Article
We consider the static and dynamic behaviour of two-dimensional droplets on inclined heterogeneous substrates. We utilize an evolution equation for the droplet thickness based on the long-wave approximation of the Stokes equations in the presence of slip. Through a singular perturbation procedure, evolution equations for the location of the two moving fronts are obtained under the assumption of quasi-static dynamics. The deduced equations, which are verified by direct comparisons with numerical solutions to the governing equation, are scrutinized in a variety of dynamic and equilibrium settings. For example, we demonstrate the possibility for stick–slip dynamics, substrate-induced hysteresis, the uphill motion of the droplet for sufficiently strong chemical gradients and the existence of a critical inclination angle beyond which the droplet can no longer be supported at equilibrium. Where possible, analytical expressions are obtained for various quantities of interest, which are also verified by appropriate numerical experiments.
Article
A combination of detection and propulsion of droplets on glass substrates at macroscopic dimensions has been accomplished via mode conversion of 1 MHz Lamb waves excited and detected by piezoelectric interdigital transducers (IDT) attached to the substrates forming a delay line configuration . Experimental results with respect to water, oil and glycerin droplets with liquid volumes between 8 and 160 μl on hydrophobic and hydrophilic glass surfaces are reported. In order to switch from sensing to actuating the excitation voltage of the IDT has been increased from 20 Vpp to 300 Vpp and the operation mode has been changed from burst to continuous excitation. Applications of this approach are envisaged at mirrors, windows and other optical components whose function may be affected adversely by the presence of liquid droplets.
Conference Paper
New ultrasonic welding methods of metal and plastic materials have been proposed by the author and their effectiveness shown. For welding of thick and large metal specimens: (1) ultrasonic butt welding methods joining thick metal specimens end to end are proposed. Large capacity vibration sources and solid state power amplifiers of 50, 100 kW were developed; (2) a welding method using two vibration systems crossed at a right angle is effective, and 10 mm thick aluminum plates were joined successfully. For medium size metal welding specimens; (3) complex vibration welding tips were shown to be very effective, and one-dimensional complex vibration systems are developed to simplify the systems. For welding of small metal specimens; (4) higher vibration frequency and a complex vibration wire bonding system are proposed, and it is shown that they are significantly effective. The bonding systems of 60 to 780 kHz were designed and the required vibration amplitude and velocity obtained for thin aluminum wire using the 40 to 780 kHz bonding systems. For welding of plastic materials; (5) high frequency, complex vibration and two-vibration-system welding methods are effective
Comparative Study of the B-Ultrasound and Molybdenum X-Ray in the Diagnosis of Breast Disease
  • L Y Su
  • C K Sun
  • Z Zhang
Su, L.Y., Sun, C.K. and Zhang, Z. (2013) Comparative Study of the B-Ultrasound and Molybdenum X-Ray in the Diagnosis of Breast Disease. Journal of Bengbu Medical College, 38, 1471-1472.