Selection of a piezoelectric transducer for a given application is done on the basis of size (active area) of the
piezoelectric element, characteristic frequency, frequency bandwidth, and type (construction) of search unit. Descriptions
of various types of search units with piezoelectric elements are given in the section "Search Units" in this article.
Different piezoelectric materials exhibit different electrical-impedance characteristics. In many cases, tuning coils or
impedance-matching transformers are installed in the search-unit housing to render a better impedance match to certain
types of electronic instrumentation. It is important to match impedances when selecting a search unit for a particular
instrument.
Both the amount of sound energy transmitted into the material being inspected (radiated power) and beam divergence are
directly related to the size (active area) of the transducer element. Thus, it is sometimes advisable to use a larger search
unit to obtain greater depth of penetration or greater sound beam area.
Each transducer has a characteristic resonant frequency at which ultrasonic waves are most effectively generated and
received. This resonant frequency is determined mainly by the material and thickness of the active element. Any
transducer responds efficiently at frequencies in a band centered on the resonant frequency. The extent of this band,
known as bandwidth, is determined chiefly by the damping characteristics of the backing material that is in contact with
the rear face of the piezoelectric element.
Narrow-bandwidth transducers exhibit good penetrating capability and sensitivity, but relatively poor resolution.
(Sensitivity is the ability to detect small flaws; resolution is the ability to separate echoes from two or more reflectors that
are close together in depth.) Broad-bandwidth transducers exhibit greater resolution, but lower sensitivity and penetrating
capability, than narrow-bandwidth transducers.
Operating frequency, bandwidth, and active-element size must all be selected on the basis of inspection objectives. For
example, high penetrating power may be most important in the axial examination of long shafts. It may be best to select a
large-diameter, narrow-bandwidth, low-frequency transducer for this application, even though such a transducer will have
both low sensitivity (because of low frequency and large size) and low resolution (because of narrow bandwidth).
When resolution is important, such as in the inspection for near-surface discontinuities, use of a broad-bandwidth
transducer is essential. Penetrating capability probably would not be very important, so the relatively low penetrating
power accompanying the broad bandwidth would not be a disadvantage. If necessary, high sensitivity could be achieved
by using a small, high-frequency, broad-bandwidth transducer; an increase in both sensitivity and penetrating power
would require the use of a large, high-frequency transducer, which would emit a more directive ultrasonic beam.
Resolution can also be improved by using a very short pulse length, an immersion technique, or delay-tip or dual-element
contact-type search units.
Array Transducers. In recent years, there has been a growing need to increase the speed of ultrasonic inspections. The
fastest means of scanning is the use of an array of transducers that are scanned electronically by triggering each of the
transducers sequentially. Such transducers consist of several crystals placed in a certain pattern and triggered one at a
time, either manually or by a multiplexer. Array transducers can either transmit normal to their axis or can have an angle
beam. To perform beam steering, sound is generated from the various crystals with a predetermined phase difference. The
degree of difference determines the beam angle.
EMA Transducers
Electromagnetic-acoustic (EMA) phenomena can be used to generate ultrasonic waves directly into the surface of an
electrically conductive specimen without the need for an external vibrating transducer and coupling. Similar probes can
also be used for detection, so that a complete non-contact transducer can be constructed. The method is therefore
particularly suitable for use on high-temperature specimens, rough surfaces, and moving specimens. The received
ultrasonic signal strength in EMA systems is 40 to 50 dB lower than a conventional barium titanate probe, but input
powers can be increased.
The principle of EMA transducers is illustrated in Fig. 33. A permanent magnet or an electromagnet produces a steady
magnetic field, while a coil of wire carries an RF current. The radio frequency induces eddy currents in the surface of the
specimen, which interact with the magnetic field to produce Lorentz forces that cause the specimen surface to vibrate in
sympathy with the applied radio frequency. When receiving ultrasonic energy, the vibrating specimen can be regarded as
a moving conductor or a magnetic field, which generates currents in the coil. The clearance between the transducer and
the metal surface affects the magnetic field strength and the strength of the eddy currents generated, and the ultrasonic