U.S. patent number 3,584,243 [Application Number 04/646,551] was granted by the patent office on 1971-06-08 for acoustic transducer.
This patent grant is currently assigned to The Magnavox Company. Invention is credited to Everett L. Fabian.
United States Patent |
3,584,243 |
Fabian |
June 8, 1971 |
ACOUSTIC TRANSDUCER
Abstract
A hydrophone is provided by a piezoelectric shear element
fastened between two masses in various configurations. Sound waves
impinge on and accelerate one mass. The acceleration of the one
mass and the inertia of the other mass set up shearing forces in
the piezoelectric shear element. The piezoelectric shear element
produces a voltage proportional to the shearing forces.
Inventors: |
Fabian; Everett L. (Fort Wayne,
IN) |
Assignee: |
The Magnavox Company (Fort
Wayne, IN)
|
Family
ID: |
24593487 |
Appl.
No.: |
04/646,551 |
Filed: |
June 16, 1967 |
Current U.S.
Class: |
310/329; 310/333;
310/341; 310/359; 367/157 |
Current CPC
Class: |
B06B
1/0648 (20130101) |
Current International
Class: |
B06B
1/06 (20060101); H01v 007/00 (); H04r 017/00 () |
Field of
Search: |
;340/10
;310/8.0,8.4,8.3,8.7,8.5,8.6,9.1,9.5 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
Primary Examiner: Hirshfield; Milton O.
Assistant Examiner: Budd; Mark O.
Claims
What I claim as new and desire to secure by Letters Patent of the
United States is:
1. An improved electroacoustical transducer for detecting sound
energy in a liquid transmission medium comprising: a first
cylindrical mass having a peripheral surface in acoustic contact
with said transmission medium and arranged to be accelerated in
directions substantially at right angles to the longitudinal axis
of said cylindrical mass by impingement of said sound energy upon
said surface, the planes of said surface being parallel to said
longitudinal axis, a first piezoelectric shear type element having
a first shearing portion secured to said first mass for
accelerating said element in response to acceleration of said first
mass, said element having a poling direction substantially at right
angles to the longitudinal axis of said first cylindrical mass, a
second mass shielded from said sound energy and fastened to a
second shearing portion of said piezoelectric element and providing
inertia so that a shearing force is set up in said piezoelectric
element in response to acceleration of said first mass, and
electrodes coupled to said piezoelectric element for deriving an
electrical signal therefrom; said second mass being surrounded by
said first mass and so positioned that it is isolated from direct
acceleration by said sound energy; further comprising a second
piezoelectric shear type element fastened to said first and second
masses, said first and second piezoelectric elements having poling
directions disposed in parallel planes and oriented at
substantially 90.degree. with respect to each other.
2. An improved electroacoustical transducer for detecting sound
energy in a liquid transmission medium comprising: a first mass
having a peripheral surface in acoustic contact with said
transmission medium and arranged to be accelerated in directions
substantially at right angles to the longitudinal axis of said mass
by impingement of said sound energy upon said surface, the planes
of said surface being parallel to said longitudinal axis, a first
piezoelectric shear type element having a first shearing portion
secured to said first mass for accelerating said element in
response to acceleration of said first mass, said element having a
poling direction substantially at right angles to the longitudinal
axis of said first mass, a second mass shielded from said sound
energy and fastened to a second shearing portion of said
piezoelectric element and providing inertia so that a shearing
force is set up in said piezoelectric element in response to
acceleration of said first mass, electrodes coupled to said
piezoelectric element for deriving an electrical signal therefrom,
and further comprising a second piezoelectric shear type element
fastened to said first and second masses, said first and second
piezoelectric elements having poling directions in parallel planes
and oriented at different angles with respect to each other.
3. An improved hydrophone comprising: a first mass of material, a
first piezoelectric shear-type element having one active surface
fastened to said first mass, a second mass of material fastened to
another active surface of said piezoelectric element, said first
mass surrounding at least a portion of said second mass and said
piezoelectric element so that impinging sound energy accelerates
said first mass only to set up stresses in said piezoelectric
element and so that said piezoelectric element produces a voltage
which varies as a function of said stresses, and a second
piezoelectric shear-type element having one active surface fastened
to said first mass and having another active surface fastened to
said second mass so that impinging sound energy accelerates said
first mass to set up stresses in said second piezoelectric element,
and so that said second piezoelectric element produces a voltage
which varies as a function of said stresses, said first and second
piezoelectric elements have their poling directions lying in
parallel planes but extending at right angles with respect to each
other.
4. An improved hydrophone comprising: a cylindrically shaped inner
mass concentrically positioned along a longitudinal axis, a first
piezoelectric shear-type element having one active face operatively
fastened to one end of said inner mass and symmetrically positioned
relative to said longitudinal axis, a second piezoelectric
shear-type element having one active face operatively fastened to
the other end of said inner mass and symmetrically positioned
relative to said longitudinal axis, said first and second
piezoelectric elements having poling directions disposed in planes
that are substantially parallel to each other, a hollow outer mass
positioned around said inner mass and said first and second
piezoelectric elements and spaced from said inner mass, said outer
mass being symmetrically positioned relative to said longitudinal
axis and being fastened to respective second active faces of said
first and second piezoelectric elements so that acceleration of
said outer mass in a direction lateral to said axis creates
shearing stresses in said first and second piezoelectric elements,
means connected to said first and second piezoelectric elements
deriving electrical signals therefrom, third and fourth
piezoelectric shear-type elements respectively operatively secured
between said first and second piezoelectric elements and said outer
mass, said third and fourth piezoelectric elements having poling
directions disposed in planes parallel to the planes of the poling
direction of said first and second piezoelectric elements extending
in a first direction and those of said third and fourth
piezoelectric elements extending in a second direction.
5. An improved hydrophone comprising: a cylindrically shaped inner
mass concentrically positioned along a longitudinal axis, a first
piezoelectric shear-type element having one active face operatively
fastened to one end of said inner mass and symmetrically positioned
relative to said longitudinal axis, a second piezoelectric
shear-type element having one active face operatively fastened to
the other end of said inner mass and symmetrically positioned
relative to said longitudinal axis, a hollow outer mass positioned
around said inner mass and said first and second piezoelectric
elements and spaced from said inner mass, said outer mass being
symmetrically positioned relative to said longitudinal axis and
being fastened to respective second active faces of said first and
second piezoelectric elements so that acceleration of said outer
mass in a direction lateral to said axis creates shearing stresses
in said first and second piezoelectric elements, means connected to
said first and second piezoelectric elements deriving electrical
signals therefrom, wherein said first and second piezoelectric
elements having poling directions that lie in parallel planes but
that are positioned at an angle with respect to each other.
Description
BACKGROUND OF THE INVENTION
My invention relates to an improved electroacoustic transducer, and
particularly to such a transducer for use in liquids.
Electroacoustic transducers are used in liquids for converting
applied electrical energy or signals into acoustical energy or
sound for transmission through the liquid, and for converting
acoustical energy or sound in the liquid into electrical energy or
signals for use in an electrical circuit. When operated in the
latter mode, such transducers are commonly referred to as
hydrophones. Hydrophones are extensively used in water for
detecting acoustical energy which may be relatively weak and which
may have frequencies covering a relatively wide band. Hydrophones
are also used to detect the direction of the source of acoustical
energy with respect to some reference direction.
Because of the many uses and applications of hydrophones, there is
always a need and desire for better hydrophones, especially those
which have directional characteristics. Directional information may
be obtained by utilizing two or more normally nondirectional
hydrophones or transducers in spaced arrays. Other hydrophones,
such as the velocity ribbon type, have directional characteristics
because of the nature of their construction. The spaced array uses
pressure sensitive hydrophones which are spaced so that the
pressure gradient of the acoustic signal and its direction relative
to the source may be determined. Generally, four such pressure
sensitive hydrophones are positioned in a circular array 90.degree.
apart. The two pressure sensitive hydrophones along one axis
provide a voltage indicative of the pressure gradient along the one
axis, and the two pressure sensitive hydrophones along the other
axis provide a voltage indicative of the pressure gradient along
the other axis. This spacing technique can be used with many types
of hydrophones; however, at relatively low acoustic frequencies,
the pressure gradients are relatively small so that the hydrophones
must be spaced relatively far apart in order to provide a usable
sensitivity. The velocity ribbon type of hydrophone utilizes a
metallic strip which is positioned in a magnetic field. An
impinging acoustic wave causes movement of the strip with the
result that it produces a voltage in the magnetic field. Two such
ribbons may be oriented at 90.degree. with respect to each other so
as to provide a directional hydrophone. However, this type of
hydrophone is relatively expensive and is not as rugged and
reliable as may be required in certain applications.
Accordingly, an object of my invention is to provide an improved
sound transducer particularly for use in water.
Another object of my invention is to provide an improved acoustic
transducer or hydrophone for producing electrical signals in
response to sound energy that covers a relatively wide band of
frequencies, the electrical signals having characteristics
indicative of the characteristics of the sound energy.
Another object of my invention is to provide an improved acoustic
transducer that is relatively rugged and strong, and that is
capable of functioning under various marine and environmental
conditions.
Another object of my invention is to provide an improved hydrophone
which has directional characteristics, and which is easily packaged
and deployed.
Another object of my invention is to provide a transducer device
which is not only easily fabricated, but which also has directional
characteristics that are not dependent upon the operational
frequency or upon the matching of the sensitivity of separate
transducers as in spaced directional arrays.
Some of the prior art electroacoustic transducers or hydrophones
are sensitive to rotational velocities. Such velocities may cause
erroneous output signals to be produced, or may distort or ruin the
desired output signal so that a useless or erroneous signal is
provided.
Accordingly, another object of my invention is to provide an
improved hydrophone which is relatively insensitive to rotational
velocities about its center of mass.
SUMMARY OF THE INVENTION
Briefly, these and other objects are achieved in accordance with my
invention by a hydrophone having at least one piezoelectric shear
type element fastened to two masses. One of the masses is arranged
so that it is exposed to sound energy which is to be detected. This
sound energy strikes or impinges on the one mass and accelerates it
so that a shearing force is set up in the piezoelectric shear
element because of the inertia of the other mass. This shearing
force causes the piezoelectric shear element to create a voltage
indicative of the shearing force. This voltage may be derived by
electrical connections to the usual piezoelectric surface
electrodes or to the two masses, where the masses act as such
electrodes or are electrically connected to such electrodes. In a
preferred embodiment, the one mass is a hollow cylinder that is
closed at its ends by a top and a bottom. The other mass is a solid
cylinder positioned coaxially within the hollow cylinder. A first
piezoelectric shear element is fastened between one end of the
solid cylinder and the top, and a second piezoelectric shear
element is fastened between the other end of the solid cylinder and
the bottom. The poling direction or axis of greatest sensitivity of
the first piezoelectric shear element is preferably positioned at
90.degree. with respect to the poling direction or axis of greatest
sensitivity of the second piezoelectric shear element so that the
hydrophone can respond to signals from all directions. Two or more
piezoelectric shear elements may be fastened between one end of the
solid cylinder and the top, and two or more piezoelectric shear
elements may be fastened between the other end of the solid
cylinder and the bottom. The piezoelectric shear elements may be
connected so that the hydrophone does not produce signals in
response to rotational motion about its center of mass, but does
produce signals in response to impinging sound waves.
BRIEF DESCRIPTION OF THE DRAWING
The subject matter which I regard as my invention is particularly
pointed out and distinctly claimed in the claims. The structure and
operation of my invention, together with further objects and
advantages, may be better understood from the following description
given in connection with the accompanying drawing, in which:
FIG. 1 shows a side elevational view of a simplified embodiment of
my invention;
FIG. 2 shows a top plan view of the simplified embodiment of FIG.
1;
FIG. 3a shows a longitudinal cross-sectional view of a preferred
embodiment of a hydrophone constructed in accordance with my
invention;
FIG. 3b shows a simplified equivalent electrical circuit of the
hydrophone of FIG. 3a;
FIG. 4a shows a longitudinal cross-sectional view of another
preferred embodiment of a hydrophone constructed in accordance with
my invention;
FIG. 4b shows a simplified equivalent electrical circuit of the
hydrophone of FIG. 4a;
FIG. 5 shows a typical output response curve with respect to
frequency of the hydrophone of FIGS. 4a and 4b;
FIG. 6a shows an exploded perspective view of a hydrophone
constructed in accordance with my invention that is relatively
insensitive to rotational motion;
FIG. 6b shows a simplified equivalent electrical circuit of the
hydrophone of FIG. 6a;
FIG. 7a shows an exaggerated cross-sectional view of the hydrophone
of FIG. 6a when subjected to rotational motion about its center of
mass;
FIG. 7b shows a simplified equivalent electrical circuit of a
portion of the hydrophone under the conditions shown in FIG.
7a;
FIG. 8a shows an exaggerated cross-sectional view of the hydrophone
of FIG. 6a when subjected to an impinging sound wave; and
FIG. 8b shows a simplified equivalent electrical circuit of a
portion of the hydrophone of FIG. 8a.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
FIGS. 1 and 2 show side elevation and top plan views of a
simplified representation of a hydrophone constructed in accordance
with my invention. Although other configurations of the
piezoelectric element may be used, my hydrophone as shown in FIG. 1
comprises a piezoelectric shear type element 10 in the
configuration of a plate or layer which is connected or fastened to
a mass M.sub.1 and a mass M.sub.2. The piezoelectric element 10 may
be of any suitable piezoelectric material having the desired shear
properties. Examples of such materials are: lead zirconate, lead
titanate, sodium niobate, potassium niobate, or crystalline quartz.
As known in the art, these materials, when properly polarized,
produce voltages at their outer electrodes in response to shearing
force set up in the material. The materials have a poling direction
or a direction of greatest sensitivity as indicated by the arrow in
FIG. 1 and in FIG. 2. This poling direction is the direction along
which a given shearing force causes the piezoelectric element 10 to
produce the greatest voltage at its electrodes. One such
piezoelectric element 10 is commercially available from the Clevite
Corporation of Bedford, Ohio, under the designation PTZ-5. With
reference to FIG. 1, if a force F is applied to the mass M.sub.1 at
an angle .theta. (Theta) with respect to the poling direction, the
mass M.sub.1 and the mass M.sub.2 are accelerated in a direction
parallel to the poling direction by a force F cos .theta.. The
acceleration of the mass M.sub.1 and the inertia of the mass
M.sub.2 introduces a shearing force M.sub.2 (F cos .theta.)
/(M.sub.1 +M.sub.2) along the poling direction. With respect to
FIG. 2, if the force F is at an angle .phi. (Phi) with respect to
the poling direction, the mass M.sub.1 and the mass M.sub.2 are
accelerated in a direction parallel to the poling direction by a
force F cos .phi.. With respect to FIGS. 1 and 2, the acceleration
of the mass M.sub.1 and the inertia of the mass M.sub.2 introduces
a net shearing force M.sub.2 /(M.sub.1 + M.sub.2) (F cos .theta.
cos .phi.) along the poling direction. Thus, the shear
piezoelectric element 10 produces a voltage in response to a force
F in almost all directions relative to the poling direction. The
magnitude of this voltage is increased as the ratio M.sub.2
/(M.sub.1 +M.sub.2) is increased. Since the effective force
parallel to the poling direction of the shear piezoelectric layer
10 varies as a function of the cosine of the angle of the applied
force with respect to the poling direction, the output of the
piezoelectric element 10 becomes very small as either the angle
.theta. or the angle .phi. approach 90.degree.. Conversely, the
output of the piezoelectric element 10 becomes its greatest when
both the angle .theta. and the angle .phi. approach zero
degrees.
The output voltage V produced by a piezoelectric element 10 may be
determined by the following equation:
In this equation, g.sub.15 is the piezoelectric shear constant
in
t is the thickness in centimeters of the shear element, M.sub.2 is
the mass of the mass that is the last to be accelerated, F is the
component of force acting on mass M.sub.1, .theta. and .phi. are
the angles at which the force F is applied relative to the poling
direction, A is the area of the shear element in square
centimeters, N is the number of shear elements, and M.sub.1 is the
mass of the mass receiving the applied force F (i.e., the first
mass to be accelerated). Calculations for a typical piezoelectric
element that is 1.3 centimeters long, 103 centimeters wide, and
0.845 centimeter thick indicate that such an element has a
sensitivity of -120 db. (reference to 1 volt per microbar) for an
applied force of 0.132 dyne. Such forces are typically produced by
relatively weak underwater acoustic signals or waves. Hence, the
output voltage of a piezoelectric shear element is practical for
available acoustic forces, and the sensitivity of the element may
be easily calculated.
FIG. 3a shows a longitudinal cross section of a hydrophone
constructed in accordance with my invention and which uses the
principles outlined in connection with FIGS. 1 and 2. In FIG. 3a, I
provide an inner, solid metallic cylinder 12 which serves as the
mass M.sub.2 or FIG. 1. This cylinder 12 is positioned
concentrically along a longitudinal axis 14. At the upper end of
the cylinder 12 I provide a piezoelectric shear element 16 which
may have a left-right poling direction in the plane of FIG. 3a. For
convenience, this is referred to as the north-south (N-S)
direction. At the lower end of the cylinder 12 I provide a
piezoelectric shear element 18 which may have a poling direction
perpendicular to the plane of FIG. 3a. For convenience, this is
referred to as the east-west (E-W) direction. These elements 16, 18
are fastened to the inner inertial mass 12 by any suitable
electrically conductive securing means such as a conducting epoxy.
A circular metallic upper plate 20 is fastened to the outer face of
the element 16, and is positioned concentrically about the axis 14.
A similar circular metallic lower plate 22 is fastened to the outer
face of the element 18, and is positioned concentrically with
respect to the axis 14. The upper and lower plates 20, 22 are
electrically connected to the shear elements 16, 18 respectively by
any suitable electrically conductive securing means such as a
conducting epoxy. The hydrophone is closed by a hollow, metallic
cylinder 24 which is positioned between and fastened to the upper
and lower plates 20, 22 so that it is concentric with respect to
the axis 14. The cylinder 24 is electrically insulated from the
plates 20, 22 as indicated by the insulation layers 26, 27, which
may be a nonconducting epoxy. The hollow cylinder 24 and the plates
20, 22 act or serve as the mass M.sub.1 of FIG. 1. The inner
cylinder or mass 12 is electrically connected to the cylinder 24 by
a connection 30 which preferably is a soft or pliable material that
does not transmit mechanical vibrations between the inner cylinder
12 and the outer cylinder 24. A first terminal 32 is connected to
the upper plate 20, a common or second terminal 34 is connected to
the cylinder 24, and a third terminal 36 is connected to the lower
plate 22. The piezoelectric elements 16, 18 have their respective
poling directions lying in parallel planes but positioned at right
angles relative to each other. Thus, the hydrophone shown in FIG.
3a is sensitive to signals or sound waves for 360.degree. around
the axis 14, and is also sensitive to sound waves which reach the
hydrophone at an angle less than 90.degree. with respect to the
axis 14.
FIG. 3b shows a simplified equivalent electrical circuit of the
hydrophone in FIG. 3a. The same reference numerals have been used
for the circuit elements in FIG. 3b which correspond to the parts
in FIG. 3a. In FIG. 3b, it will be seen that voltages or signals
from the upper piezoelectric element 16 may be derived from the
terminals 32, 34, and that voltages or signals from the lower
piezoelectric element 18 may be derived from the terminals 34, 36.
In FIG. 3b, the capacitors shown by the dotted lines between the
terminals 32, 34 and between the terminals 34, 36 represent the
capacitance resulting from the upper plate 20 with respect to the
cylinder 24 and the cylinder 12 and their associated dielectrics;
and likewise, the lower plate 22 with respect to the cylinder 24
and the cylinder 12 and their associated dielectrics. The
hydrophone shown in FIG. 3a was constructed and tested. The inner
mass or cylinder 12 was constructed of type metal having a diameter
of 1.75 inches, and a height of 3.36 inches. The upper and lower
plates 20, 22 were constructed of aluminum, having a diameter of
3.5 inches and a thickness of 0.0625 inch. The cylindrical shell or
hollow cylinder 24 was also constructed of aluminum having an
outside diameter of 3.5 inches, a wall thickness of 0.0625 inch,
and a height of 3.5 inches. The cylinder 24 was joined to the
plates 20, 22 by a nonconducting epoxy having a thickness of
approximately 0.03125 inch at the layers 26, 27. The shear
piezoelectric layers 16, 18 were Clevite PZT-5 having a surface
dimension of 0.5 by 0.5 inch, and a thickness of approximately 0.1
inch. These layers 16, 18 were fastened to the inner mass or
cylinder 12 and to the upper and lower plates 20, 22 respectively
by a conducting type of epoxy. The outer surfaces of the assembled
hydrophone were covered with a nonconducting epoxy for insulation.
The completed hydrophone was tested up to approximately 6,000
cycles per second. At approximately 2,300 cycles per second, the
hydrophone exhibited a self resonance.
FIG. 4a shows another hydrophone in longitudinal cross section.
This hydrophone comprises an inner inertial mass or cylinder having
two solid metallic cylinders 41, 42 joined by an insulating or
nonconducting layer 43 and concentrically positioned on a
longitudinal axis 40. A piezoelectric shear type element 45 is
fastened to and electrically connected to the upper surface of the
cylinder or mass 41, and a piezoelectric shear-type element 46 is
fastened to and electrically connected to the lower surface of the
cylinder or mass 42. As explained in connection with FIG. 3a, the
upper layer 45 has a N-S poling direction in the plane of the paper
of FIG. 4a, and the lower layer 46 has an E-W poling direction
perpendicular to the plane of the paper. Upper and lower circular
metallic plates 48, 50 are concentrically positioned on the axis
40, and are respectively fastened to and electrically connected to
the piezoelectric elements 45, 46. The hydrophone is closed or
surrounded by a concentric, hollow, cylindrical metallic cylinder
51 which is electrically connected to the plates 48, 50. Electrical
signals are derived from a terminal 54 connected to the solid
cylinder 41, a common terminal 55 connected to the hollow cylinder
51 or one of the plates 48, 50, and a terminal 56 electrically
connected to the other solid cylinder 42. The outer surfaces of
this hydrophone need not be insulated from the surrounding liquid
transmission medium, but may be so insulated by a suitable material
if desired. Acoustic signals which reach the outer cylinder or mass
51 cause shearing forces to be set up in the piezoelectric elements
45, 46, so that electrical signals are produced at the terminals
54, 55, 56. FIG. 4b shows a simplified equivalent electrical
circuit of the hydrophone of FIG. 4a. The same reference numerals
have been used for the circuit elements of FIG. 4b which correspond
to the parts in FIG. 4a. In FIG. 4b, the capacitor indicated by
dotted lines and connected between the two inner masses or
cylinders 41, 42 represents that capacitance resulting from the
area between the two masses 41, 42 and the associated dielectric of
the insulating layer 43. The coupling or interaction between the
N-S and E-W circuits which results from this capacitance may be
reduced if a conducting layer is positioned midway between the
outer boundaries of the insulating layer 43 and connected to the
common terminal 55.
The hydrophone of FIG. 4a was constructed and tested. The inner
cylinders or masses 41, 42 were constructed of type metal having a
diameter of 1.75 inches. The cylinders 41, 42 were joined by the
insulation layer 43 having a diameter of 1.75 inches and a
thickness of approximately 0.0625 inch. The combined length of the
joined cylinders 41, 42 was 3.0625 inches. The piezoelectric
elements 45, 46 were made of Clevite PZT-5 having a surface area of
0.5 by 0.5 inch and a thickness of 0.25 inch, and were fastened by
solder. The upper and lower plates 48, 50 were constructed of brass
having a diameter of 4 inches and a thickness of 0.0625 inch. The
outer cylinder or mass 51 was also constructed of brass and had an
inside diameter of 4.0 inches, a wall thickness of 0.0625 inch, and
a height of 3.8125 inches to allow for solder thickness. The
cylinder 51 and plates 48, 50 were soldered together. This
hydrophone was tested with the outer cylinder and end plates
uninsulated from the surrounding liquid transmission medium. Its
response with frequency is shown in FIG. 5. It will be noted that
the hydrophone of FIG. 4a exhibits a resonance at approximately
2,300 cycles per second. However, the response of this hydrophone
is useful and of good quality down to frequencies as low as 20
cycles per second. Generally, the frequency response is a linearly
varying one. The directional response of the hydrophone of FIG. 4a,
as well as the hydrophone of FIG. 3a, generally followed the cosine
function mentioned earlier so that their directional patterns have
the familiar FIG. 8 response. Both hydrophones exhibited a
resonance around 2,300 cycles per second. This resonance may, if
desired, be damped or otherwise controlled by the use of materials
for the inner and/or outer masses which inherently exhibit the
desired resonant characteristics and/or by the addition of suitable
damping material to the masses. In addition, the resonant frequency
may be shifted, if desired, by changing those design parameters
which affect the resonant frequency of the masses.
The hydrophones of FIGS. 3a and 4a were constructed with the idea
that their respective axes 14, 40 would be oriented in a vertical
direction. Thus, sound traveling through water in a generally
horizontal direction would strike or impinge on the hydrophones at
a right angle to these axes 14, 40. If these hydrophones rotate
about a horizontal axis passing through their center of mass, the
acceleration resulting from this rotation causes the piezoelectric
elements to produce a spurious output signal. FIG. 6a shows, in an
exploded perspective view, a hydrophone in accordance with my
invention which reduces the signals resulting from this rotation
about a horizontal axis passing through the center of mass. The
hydrophone comprises an inner mass 60 to which piezoelectric shear
type elements 61, 61a are fastened and poled in an east-west (E-W)
direction. Outer or additional piezoelectric shear type elements
62, 62a poled in a north-south (N-S) direction are respectively
fastened to the outer faces of the east-west elements 61, 61a. The
poling directions lie in parallel planes. End plates 65, 65a are
fastened to the outer faces of the north-south elements 62, 62a
respectively, and the outer mass is completed by an outer
cylindrical shell 66. A simplified equivalent electrical circuit of
this hydrophone is shown in FIG. 6b, where circuit elements in FIG.
6b are given the same reference numerals as their corresponding
parts in FIG. 6a. A common terminal 68 is connected to the junction
of the elements 61, 62 and to the junction of the elements 61a and
62a. An east-west terminal 67 is connected to the inner mass or
cylinder 60. A north-south terminal 69 is connected to the end
plates 65, 65a and/or the outer mass or cylinder 66. If the
hydrophone of FIG. 6a is rotated about its center of mass 70 in a
clockwise direction as shown by the arrows 71, 72 in FIG. 7a, the
east-west piezoelectric elements 61, 61a will produce the voltage
polarities shown in FIG. 7a at their respective electrodes. FIG. 7a
also shows in exaggerated form the direction in which the
piezoelectric elements 61, 61a, 62, 62a are moved by the external
clockwise rotational force about the center of mass 70. This
movement causes the voltages of the elements 61, 61a to have a
positive polarity at their upper electrodes, and a negative
polarity at their lower electrodes. When these voltages are
combined at the terminals 67, 68 as shown in the partial circuit
diagram of FIG. 7b, it will be seen that no voltage exists between
the terminals 67, 68. In a similar manner, no voltage would be
produced by a counterclockwise rotation about the center of mass
70. Thus, rotational motion or acceleration about the center of
mass 70 produces no net output signal in the combined piezoelectric
elements. A similar condition holds for the north-south elements
62, 62a, but these polarities have not been shown in order to keep
FIGS. 7a and 7b relatively simple. However, if an acoustic signal
or wave strikes the hydrophone as indicated by the arrow 80 in FIG.
8a, the piezoelectric elements take the position indicated in
exaggerated form in FIG. 8a. In this case, the inner electrodes of
the east-west shear piezoelectric elements 61, 61a are negative,
and the outer electrodes are positive. When these voltages are
combined at the terminals 67, 68, a voltage is produced as shown in
the partial circuit diagram of FIG. 8b. A voltage is also produced
by the north-south layers 62, 62a when a north-south signal is
received. Thus, the use of two piezoelectric shear type elements
for each of the two directions, namely east-west and north-south,
compensates for any rotational acceleration about a horizontal axis
passing through the center of mass.
It will thus be seen that my invention provides an improved
hydrophone which can sense sound waves in a liquid such as sea
water, and which can be constructed in a relatively rugged and
compact structure. My hydrophone can be compensated for rotation
about horizontal axes by the use of two shear piezoelectric
elements. Rotation about the control vertical axis can be
compensated with shear piezoelectric elements on that axis or
symmetrically located about that axis. My hydrophone is relatively
insensitive to vibrations that compress the piezoelectric
shear-type elements, or that set up resonant and symmetrical
vibrations that are in opposition relative to the longitudinal axis
of the hydrophone. My hydrophone also provides an improved response
over a wide band of frequencies. While I have shown specific
embodiments of my hydrophone, persons skilled in the art will
appreciate that modifications may be made. For example, the inner
and outer masses may be constructed of other materials such as
plastic, and may have other shapes such as spherical. The inner
and/or outer masses may be covered with material for damping and/or
insulation. Other electrical circuits and electrode configurations
for combining the output voltages of the piezoelectric elements may
also be used. The piezoelectric shear-type elements may have
various configurations such as a circular shape rather than a
square or rectangular shape as shown and described. In addition
more than one piezoelectric element may be used at each end of the
inner mass for a given poling direction, if additional strength or
holding structure is desired between the inner mass and the outer
mass, or if different voltage output levels or impedances are
desired. Additional piezoelectric elements may be used at each end
or at one end of the inner mass to provide two or more poling
directions. Where the additional elements are used, they may be
stacked or may be in a side-by-side configuration. The outer mass
of plates and cylinders need not be supported by the piezoelectric
elements alone, but can be supported to some extent by a mechanical
construction between the inner mass and the outer mass, if such
construction does not reduce the shearing forces below the
necessary level. And finally, other fastening means, such as
welding or mechanical fasteners, may be used. Therefore, while by
invention has been described with reference to particular
embodiments, it is to be understood that modifications may be made
without departing from the spirit of the invention or from the
scope of the claims.
* * * * *