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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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