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Inexpensive
Ultrasonic Equipment for Fingerprint Recognition
Applied to Material Testing |
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NDTnet
1998 May, Vol.3 No.5
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Introduction |
Optel, the company I represent,
was established a few years ago on the basis of the idea
that a fingertip structure (reflected in fingerprints) can
be better analyzed with the use of ultrasound than by
existing methods. It turns out that our approach was
justified; however its implementation required much more
effort than we had anticipated. Nevertheless, we have
managed to create fully-operational prototypes of an
ultrasonic camera which permit the imaging and recognition
of finger ridge patterns. We are well on our way to
developing a plan for mass production.
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| Brief
Principles of the Ultrasonic camera |
The design of the current
version of the camera and principles behind its operation
have been presented in [1]. Its operation
can be briefly summarized as follows:
| A very short
ultrasonic pulse is sent from a number of different
directions toward a finger surface and from each
direction a much longer broadband impulse response is
received. This impulse response is an effect of the
contact scattering of the ultrasonic wave on the
surface of the fingertip. Based on a set of such
impulse responses, an image of the finger surface
structure is reconstructed using computer tomography
methods.
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In order to create our camera we had to design and make
our own ultrasonic devices, for two reasons: devices
available on the market were too expensive and did not
meet a number of requirements important in our
applications. Of paramount importance was that the time
skew between different impulse responses be very small
(less than 5ns). Equally important was that the ultrasonic
transducer should be able to generate a very short pulse
(less than 100ns) and should have a sufficiently broad
bandwidth as a receiver (4-16MHz). Finally, all elements
used had to be inexpensive, since the final product should
be suitable for mass production at a reasonable price.
Now that we have created
elements that meet our needs, it has become apparent that
they are suitable for a number of other applications where
the use of ultrasonic pulses is necessary, (e.g.,
classical defectoscopy, layer thickness measurement,
medical applications). This paper is intended as a
presentation of our solutions for the ultrasonic
technology experts.
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Elements of the Ultrasonic Hardware |
We can offer three elements
based on our own design, partially patented, which
depending on the software used can be employed to various
applications.
- Ultrasonic PC card, particularly well suited
to automatic measurements using mechanical or
electronic scanners. It can directly control
such devices (it only generates control
signals, step motors require an additional
driver unit).
- Pulser and receiver circuit with an active
switch and input amplifier, the size of a
matchbox, powered and controlled by the
ultrasonic PC card.
- Ultrasonic transmitter, capable of
generating very short pulses and having a
broad bandwidth as a receiver.
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Additionally, we can offer
our own designs of step motor controllers, power
supplies etc. (Full information regarding the above
products is available on the Internet *.
The PC card comprises
not only an input amplifier, a high-speed A/D converter
(it has a sampling frequency of 80MHz, a 120 MHz version
is under development) but also a control circuit. This
means that all control signals required for the
measurement process are generated by the card. This kind
of design allows us to achieve a sufficiently small time
skew between different channels (or scanner positions)
which is less than 1 ns. Thanks to the independent
control system, the CPU is not directly involved in the
measurement process, therefore a high performance PC is
not essential. The card has a simple design achieved
through the use of highly integrated circuits and can be
offered at a reasonable price.
Our pulser circuit also
provides an inexpensive solution. It is based on a
unique design: in order to generate a pulse we first
charge the transducer to a required voltage (max. 600V)
which takes a few microseconds, then we discharge it in
a very short period of time (at the moment this time is
around 20ns). This approach results in a simple and
inexpensive circuit which generates very clean pulses
with practically any transducer (only transducers with a
parallel inductance cannot be used).
| Fig.
1: Pulse of the transducer, received with a
hydrophone (50 ns/div)
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| Fig.
2: Pulse of the transducer, received with the
same transducer
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All
the electronic circuits we have developed would not be
sufficient if we did not have transducers capable of
generating very short pulses while having broad
bandwidths as receivers. We had tested a number of
designs proposed by others as well as products available
on the market and we were convinced that there was only
one solution: to find a new way. It had to lead to a
design which would not only satisfy all the technical
requirements but also enable cheap production and
repeatable parameters.
We have succeeded in
developing a transducer satisfying the above
requirements for which a patent application has been
submitted. Fig. 1 shows a pulse generated by our
transducer (a hydrophone made of PVDF film has been used
for the measurement, 50 ns/div). Fig. 2 presents the
signal received in the transceiver mode (100 ns/div).
The difference between the two signals results from the
fact that our transducer works differently as a
transmitter and as a receiver. This property is also
exhibited by other types of transducers, though the
differences are usually much smaller. It is possible to
develop a transducer which would have practically
identical signals in both the transmitter and receiver
modes (corresponding roughly to the signal shown in Fig.
1), but it would have certain drawbacks (particularly
when used in the design of our camera). Therefore we
have decided to use the standard transducers which
receive slightly longer impulse response (as shown in
Fig. 2). How do the signal level and sensitivity compare
with other designs? The signal level generated in the
transmitter mode is at least two times higher and the
sensitivity in the receiver mode is slightly lower.
Hence, the overall signal level in the measurement cycle
is comparable. A better sensitivity can be achieved
today, however it entails some deterioration of the
receiver bandwidth (this in turn can be improved at the
cost of the signal level). Since the development of the
new transceivers has not been completed yet, we expect
considerable improvement.
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Ultrasonic Camera applied to Material Testing |
Our technique allows not
only the observation of finger ridge patterns but also
other objects. An example of such an application is a
device suitable for detecting material defects in
objects as well as for medical measurements. It has been
created on the basis of our electronic circuits,
transducers as well as mechanical elements of our
ultrasonic camera. Its basic idea is similar to that
behind our ultrasonic camera. Fig. 3 shows a schematic
diagram of the device:
| Fig.
3: Schematic diagram of the device.
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The motor M moves the
transducer T around the object S under measurement,
sending toward it an ultrasonic wave. Signals reflected
by the object are received by the same transducer and
processed in a similar way as is done in our camera.
Only image reconstruction procedures need to be modified.
| Fig.
4: Echoes from the brass cylinder
| 5.View
of the bottom of the brass cylinder
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The device has
initially been developed for finger imaging. We would
like to see a cross-section of a finger and subsequently
a three dimensional structure (using tomographic
reconstruction procedures). Using the same device, it is
possible to observe other types of objects, both natural
and man-made, in order to find material defects. Since
the device has just recently been developed, the images
it produces are far from perfect. Both reconstruction
procedures and the device elements need to be refined.
However, it is obvious today that in the future our
device will provide a means of high-resolution imaging
of internal structures of various objects. Fig. 4 shows
an image of echoes, coming from a brass cylinder which
has 4 holes of 1 mm diameter drilled in it (its view is
shown in Fig. 5). Each hole produce an echoe, that could
be seen on the picture as a sinus line or a part of it.
I anticipate that I will be shortly able to present the
NDT-Journal readers pictures, that show the internal
structure of such a cylinder and are of much higher
quality.
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References |
1. Wieslaw
Bicz et al; Fingerprint structure imaging based on an
ultrasound camera
NDTnet Journal, http://www.ndt.net, Vol. 3 No. 5 (May
1998)
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| Author |
Wieslaw Bicz
Studierte Physik (Spezialität: optische Holographie) in
Breslau, lebte einige Jahre in Deutschland (um
Frankfurt), wo auch die Geschichte der
Fingerabdruckerkennung mit Ultraschall anfing. Geschäftsführer
der Firma Optel, die das Projekt zum erfolgreichen Ende
bringen will.
Optel sp. z o.o.
ul Otwarta 10 a
50-212 Wroclaw
Phone: 004871 3296853, Fax: 004871 3296852
Email: W.Bicz@optel.pl
Homepage: http://www.optel.pl
Visit Optel
on NDTnet
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