International Journal of Power Electronics and Drive System (IJPEDS)
Vol. 10, No. 2, June 2019, pp. 1064~1071
ISSN: 2088-8694, DOI: 10.11591/ijpeds.v10.i2.pp1064-1071 1064
Journal homepage: http://iaescore.com/journals/index.php/IJPEDS
Study and simulation with VHDL-AMS of the electrical
impedance of a piezoelectric ultrasonic transducer
Toufik Merdjana, Abdelhafid Chaabi
Hyper Frequency and Semiconductor Laboratory (LHS), University Mentouri Constantine1, Algeria
Article Info ABSTRACT
Article history:
Received Sep 22, 2018
Revised Nov 19, 2018
Accepted Mar 3, 2019
Ultrasonic transducers are a key element that governs the performances of
both generating and receiving ultrasound in an ultrasonic measurement
system. Electrical impedance is a parameter sensitive to the environment of
the transducer; it contains information about the transducer but also on the
medium in which it is immersed. Several practical applications exploit this
property. For this study, the model is implemented with the VHDL-AMS
behavioral language. The simulations approaches presented in this work are
based on the electrical Redwood model and its parameters are deduced from
the transducer electroacoustic characteristics.
Keywords:
Impedance
Piezoelectic
Transducer
Ultrasonic
VHDL-AMS
Copyright © 2019 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Toufik Merdjana,
Department of Electronic, Faculty of science and Technology,
University Mentouri Constantine1, Algeria
Constantine, Algeria
Email: merdjana_toufik@umc.edu.dz
1. INTRODUCTION
Ultrasound systems are widely used. They find many applications in engineering, medicine, biology,
and other areas. The one indispensible part in these systems is the transducer. These will use the properties of
magnetostrictive or piezoelectric materials to convert electrical energy into ultrasonic mechanical energy [1].
Piezoelectric materials have the advantage over other systems of having good performance and being
available in very diverse geometries. The electromechanical interaction of piezoelectric transducer,
represented by electrical equivalent circuits, was first introduced by Mason [2]. He proposed an exact
equivalent circuit that separated the piezoelectric material into an electrical port and two acoustical ports
through the use of an ideal electromechanical transformer. The problems with the model are that it required a
negative capacitance at the electrical port. Redwood [3] improved this electromechanical model by
incorporating a transmission line, making possible to extract useful information on the temporal response of
the piezoelectric component.
The Electrical impedance is a parameter sensitive to the environment of the transducer. Several
practical applications exploit this property[4, 5]. The measurement of the impedance makes it possible, for
example, to detect the physical or structural modifications of the medium due in particular to damage. This
approach is used for non-destructive testing to monitor the condition of structures such as aging and
corrosion [6, 7]. Frequency analysis of the impedance makes it possible to precisely locate the resonance
zone of the transducer. This location can be exploited to control and stabilize the operating frequency of high
power systems such as ultrasonic welding devices [8]. Real-time knowledge of the electrical impedance also
makes it possible to determine and optimize the power emitted by a transmitter or the sensitivity in reception
of a piezoelectric sensor [9].