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| United States Patent | 3973235 |
| Link to this page | http://www.wikipatents.com/3973235.html |
| Inventor(s) | van der Burgt; Cornelis Martinus (Eindhoven, NL) |
| Abstract | Apparatus for the detection of an acoustic image by means of an election
tube including a face plate and an electronically scanned transducer made
of a thin foil of polymer material whose acoustic wave velocity of
propagation is less than 1.8 that of a liquid imaging medium. The face
plate also is made of a polymer material having a velocity of propagation
less than 1.8 that of said liquid. Preferably, the transducer foil is much
thinner than the face plate and has a thickness approximately 0.5 times
the acoustic wavelength. |
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Title Information  |
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Drawing from US Patent 3973235 |
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Device for the detection of an acoustic image |
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| Publication Date |
August 3, 1976 |
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| Filing Date |
April 15, 1974 |
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| Priority Data |
Apr 24, 1973[NL]7305667 |
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Title Information  |
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Claims  |
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What is claimed is:
1. An electron vacuum tube comprising a face plate which is capable of
withstanding the pressure difference between the inside and outside of the
tube and which is made of a polymer material having a low velocity of
acoustic propagation, a transducer for converting an acoustic image into a
corresponding electric charge image and located inside of the tube
adjacent the face plate, said transducer being formed of a stretched thin
foil made of a polymer material which also has a low velocity of acoustic
propagation and has a remanent electrical polarization, the velocity of
acoustic propagation of the face plate and transducer material each being
less than 1.8 times that of a liquid medium used to image the acoustic
wave image onto the transducer via said face plate, the transducer being
thinner than the face plate and approximately 0.5 times the acoustic
wavelength, and means for electronically scanning the transducer charge
image.
2. An electron tube as claimed in claim 1, characterized in that at least
prior to evacuation of the tube the face plate has an outwardly curved
shape so as to be better able to withstand said pressure difference.
3. Apparatus for the detection of an acoustic image comprising, an electron
vacuum tube including a non-piezoelectric face plate, a transducer for
converting an acoustic image into a charge image and means for
electrically scanning the transducer charge image, acoustic imaging means
including a liquid medium and an acoustic lens for imaging acoustic waves
of said image onto the transducer, the transducer being separated from the
liquid medium by the electron tube face plate which is capable of
withstanding the difference in pressure that exists between the vacuum
inside the tube and the surrounding liquid, wherein the face plate is made
of a polymer material having a velocity of propagation for acoustic waves
which in relation to that of the liquid is less than 1.8, the transducer
comprises a thin foil of polymer material applied to the face plate and is
appreciably thinner than the face plate and has a thickness approximately
0.5 times the acoustic wavelength, and the velocity of propagation for
acoustic waves in the transducer material in relation to that of the
liquid is less than 1.8.
4. Apparatus as claimed in claim 3 wherein the transducer comprises
polyvinylidene fluoride having a remanent electric polarization.
5. Apparatus for the detection of an acoustic image of an object
comprising, a liquid medium for the propagation of acoustic wave energy, a
source of acoustic wave energy for irradiating the object via the liquid
medium, an electron tube having a non-piezoelectric face plate the outer
surface of which is adjacent the liquid medium and the inner surface
supporting a transducer for converting acoustic energy into an electric
charge image, means for focusing the acoustic image reflected from the
object onto said transducer via the liquid medium and the tube face plate,
said electron tube including means for electronically scanning a charge
image formed on the transducer, wherein the improvement comprises a face
plate made of a polymer material having a velocity of propagation for
acoustic waves which is less than 1.8 the acoustic wave velocity of
propagation of the liquid medium, a transducer made of polymer material
whose velocity of propagation for acoustic waves is less than 1.8 the
acoustic wave velocity of propagation of the liquid medium, the thickness
of the transducer being less than that of the face plate and approximately
0.5 times the acoustic wavelength.
6. Apparatus as claimed in claim 5 wherein the transducer comprises a thin
film of polymer material having a remanent electric polarization.
7. Apparatus as claimed in claim 5 wherein the transducer material is
polyvinylidene fluoride.
8. Apparatus as claimed in claim 5 wherein the face plate is made of a
material selected from the group of materials consisting of polystyrene
and polyethylene materials.
9. Apparatus as claimed in claim 5 wherein the thickness of the face plate
is approximately 50 times greater than that of the transducer and both
have approximately the same velocity of propagation for acoustic waves. |
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Claims  |
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Description  |
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The invention relates to a device for the detection of an acoustic image,
the acoustic waves being imaged via acoustic imaging means, which comprise
at least a liquid medium and an acoustic lens, onto a transducer, which is
incorporated in an electron tube, for converting acoustic vibrations into
a charge image which can be scanned electronically, the transducer being
separated from the liquid medium by a non-piezoelectric face plate which
is mounted on the electron tube, which face plate should be capable of
withstanding a difference in atmospheric pressure.
Such a device is, for example, used in industry to detect internal flaws in
moving or stationary workpieces, in underwater investigations where
obstacles or lost objects are to be traced or, for example a drilling site
at the bottom of the sea is to be surveyed, in hospitals for ultrasonic
diagnosis, for example for the localisation of tumors in the brain,
breasts or uterus or in observing the cardiac action. In all these
instances a visual display with at least 25 complete images per second is
aimed at, so that rapidly moving objects or object portions (pulsating
arteries, cardiac valve, foetus) can also be observed accurately and can
be recorded on film or video tape.
For this purpose it is known to expose the object under test or to
irradiate said object with acoustic waves (in this respect the term
acoustic denotes both audible and ultrasonic sound waves, for example up
to a frequency of 10 MHz). After being focussed the acoustic waves then
impinge on a so-called Sokolov tube, which incorporates said transducer,
where a charge image which corresponds to the acoustic images is formed,
which can subsequently be scanned with an electron beam.
A drawback of the Sokolov tube is that the piezo-electric transducer, which
at the same time forms a wall of the tube, must be very thin to attain the
highest sensitivity and the highest resolving power for the acoustic waves
to be detected. In order to obviate said drawback it has been proposed to
provide the tube with an external face plate so that it is better able to
withstand the difference in pressure between the inside and outside of the
tube, thus enabling the use of cheap, large screens. The invention is
based on the following considerations:
1. The minimum size of a picture element that can still be resolved
approximately equals the thickness of the piezoelectric transducer plate
of the Sokolov tube, said thickness preferably being approximately equal
to half an acoustic wavelength. When using a monocrystalline quartz in
X-cut this means a thickness of approximately 2 and 1 mm respectively for
acoustic waves having a frequency of approximately 11/2 and 3 MHz
respectively. The resolving power is then still inadequate.
2. A quartz plate of the said small thickness is only capable of
withstanding by itself a pressure difference of 1 atmosphere if it has a
small diameter. For piezoelectric materials other than quartz the maximum
permissible diameter is even smaller. A much greater diameter is required,
i.e. a high linear aperture.
3. Acoustic rays which reach the piezo-electric transducer surface at an
angle of incidence greater than 3.degree. to 4.degree. do not exclusively
produce the desired thickness vibrations in the transducer, but bending or
surface waves will also propagate along the plate surface, as a result of
which the image is disturbed. This "angular aperture" is unsatisfactorily
low.
The invention is characterized by the following combination:
a. the face plate is made of a polymer having a velocity of propagation for
acoustic waves whose ratio to that of the liquid is smaller than 1.8.
b. the thickness of the transducer is appreciably smaller than that of the
face plate and equals approximately 0.5 times the acoustic wavelength;
c. the transducer is also made of a polymer, viz. a polymer with remanent
electrical polarization, and is applied to the face plate as a thin film;
and
d. the velocity of propagation for acoustic waves of the transducer
material in proportion to that of the liquid is also smaller than 1.8.
Owing to the provision of the face plate the problem which is caused by
said atmospheric pressure difference reduces the provision of an element
which is adapted as well as possible to the further acoustic arrangement.
Generally, water will be selected as a liquid medium and the material of
the screen plate, provided that its velocity of propagation is not too
high relative to that of water, will only cause a slight diffraction of
the acoustic waves at the interface between liquid and screen plate.
Moreover, possible bending or surface waves should be damped out as
rapidly as possible so as to ensure that the acoustic image formed on the
transducer is blurred to the least extent. Both requirements are met by a
polymer having an acoustic velocity of propagation which is not too high,
such as polyethylene or polystyrene.
As the transducer is considerably thinner, for example by a factor of 50,
than the screen plate and both have substantially the same velocity of
sound, only a slight disturbing effect will occur at the interface between
screen plate and transducer so that the highest possible resolving power
is maintained. In this respect it is also of importance that when using
said materials for the face plate and the transducer undesired surface
waves are damped out.
A particularly suitable material for such a transducer is polyvinylidene
fluoride in the form of a stretched and polarised foil. At a high
temperature, for example 100.degree. to 150.degree.C such a foil can
mechanically be stretched uniaxially or biaxially up to 2 to 3 times its
original dimensions. Simultaneously or later the stretched foil is
subjected to a strong electric field, for example with a field strength of
300 to 1000 kV/cm, for approximately 1 hour at 50.degree. to 150.degree.C,
so that a powerful remanent electrical polarisation persists in the foil
after it has been cooled down to room temperature at approximately the
same field strength. It is of particular importance that such a foil
readily adapts itself to the shape of the face plate. To this end the face
plate may, for example, be curved outwards slightly so as to be better
able to withstand said pressure difference, the foil readily following
this curved shape.
Compared with the use of said quartz materials for the transducer it
appears that the resolving power is improved in accordance with the ratio
of the velocities of sound in quartz and in polyvinylidene fluoride
respectively, i.e. by a factor of more than 2.
The FIGURE shows an embodiment of the invention.
The ultrasonic sound source is formed by a quartz half wavelength
oscillator 1 whose vibrations irradiate an object 10. This object is in
direct acoustical contact with a space 11 which is closed by a flexible
rubber diaphragm 3 and which is in engagement with the object 10 via a
viscous coupling layer 2. The space 11 is filled with a liquid, for
example, water, and furthermore comprises an acoustic lens 4, for example
Perspex, by which the acoustic vibrations can be imaged onto a transducer
6, which is incorporated in an electron tube 12, i.e. is mounted on a face
plate 5 which is capable of withstanding the difference in pressure
between the liquid in the space 11 and the vacuum inside the tube 12. If
necessary, the face plate may previously be curved outwardly so that it
straightens after evacuation of the tube 12. The thin transducer 6, which
is formed by a foil, can readily follow the variations of the shape of the
plate 5. The advantage of this is that the screen plate may be slightly
thinner.
By imposing the requirements outlined above on the material of the face
plate 5, for example polystyrene or polyethylene, and of the transducer 6,
for example polyvinylidene fluoride, a high resolving power in combination
with a screen of reasonably large dimensions is obtained. The electrical
charge image obtained on a transducer is scanned in the usual manner with
the aid of an electron beam and converted into an electrical signal, which
in its turn can be recorded either on a film or by means of a video
recorder.
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Description  |
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