U.S. patent number 3,833,825 [Application Number 05/349,937] was granted by the patent office on 1974-09-03 for wide-band electroacoustic transducer.
This patent grant is currently assigned to Honeywell, Inc.. Invention is credited to David E. Haan.
United States Patent |
3,833,825 |
Haan |
September 3, 1974 |
WIDE-BAND ELECTROACOUSTIC TRANSDUCER
Abstract
A thickness-mode electroacoustic transducer wherein an active
body of non-uniform thickness is employed to provide uniform
wide-band frequency response. The body may be wedge-shaped, having
non-parallel planar major surfaces. At least one of the major
surfaces is subdivided into a two-dimensional array of poles by
means of grooves formed in the surface for the purpose of providing
improved frequency and directional response. BACKGROUND OF THE
INVENTION The invention herein described was made in the course of
or under a contract, or subcontract thereunder, with the Department
of the Navy. This invention pertains generally to acoustic
transducers, and more specifically to thickness-mode
electroacoustic transducers having relatively uniform frequency and
directional response over a wide band of frequencies. For purposes
of the following discussion, it is pointed out that certain terms
used as a matter of convenience are most commonly associated with
projection of acoustic energy. However, the discussion applies to
both acoustic projectors and hydrophones. Commercial and military
interest in transmitting and receiving underwater acoustic signals
has increased rapidly in recent years. One of the most widely used
items of equipment for this purpose is the electroacoustic
transducer. Most prior art electroacoustic transducers are
inherently relatively narrow frequency band devices. A basic reason
for this is that each transducer, including its transducing element
and associated electrodes, acoustic decouplers and housing,
comprises a dynamic structural system having a fundamental resonant
frequency and other dynamic characteristics which limit its
frequency response. One common type of electroacoustic transducer,
known as a thickness-mode transducer, employs a transducing element
of which the lateral dimensions are larger than the thickness. The
transducing element is polarized so that its thickness changes in
response to a changing electrical potential applied across the
element. Conversely, any mechanical force which changes the
thickness of the element results in generation of a changing
electrical potential thereacross. Thickness-mode transducers as
described above are entirely adequate for many underwater
electroacoustic transducer applications. Further, such transducers
of conventional narrow frequency band design have the added
advantage that problems in achieving satisfactory frequency and
directional response are generally minimized. Nevertheless, they
frequently exhibit somewhat anomalous frequency and directional
response characteristics. Such characteristics become increasingly
pronounced and troublesome in transducers designed for operation
over wider bands of frequencies. A variety of techniques have been
devised in attempts to minimize side lobes and other unwanted forms
of radiation which to some degree, degrade the response patterns of
all transducers. One such technique involves forming grooves in a
face of the transducing element. The grooves have the effect of
interrupting the propagation of unwanted (typically radial or
lateral) modes of vibration in the element, thereby minimizing
undesired patterns of radiation. Transducers employing this
technique are described in greater detail in U.S. Pat. Nos.
2,956,184 and 3,470,394 issued respectively to Hyman Pollack on
Oct. 11, 1960 and Rufus Cook et al. on Sept. 30, 1969. Another
prior art technique (also described in U.S. Pat. No. 2,956,184)
involves contouring the transducing element so that an electrical
signal applied between opposing faces thereof subjects the center
of the element to a higher electrical gradient than that near its
outer edge. According to the patent, the outer edge of the element
is believed to be principally responsible for radiating side lobes.
Hence, by differentially polarizing the transducing element so that
its outer edge is driven less vigorously than its central portion,
directional response is improved. Yet other techniques which have
been attempted for minimizing unwanted transducer radiation include
mechanical tuning of the transducing element-housing assembly, the
use of electrical signal shaping circuitry, and the use of
acoustical baffles for defining a window through which radiation is
permitted. Whereas conventional narrow-band transducers have been
generally satisfactory for many past transducer applications, an
increasing number of requirements are now developing for
transducers capable of efficient operation over an extended band of
frequencies. Wide-band operation greatly increases the severity of
problems involved in achieving acceptable directional response, and
necessitates the use of special features to minimize such problems.
The transducer disclosed in previously identified U.S. Pat. No.
3,470,394 employs a transducing element of which opposite faces are
cross serrated or diced to permit operation over a somewhat wider
band of frequencies than prior art transducers. Although
transducers of this design provide somewhat improved wide-band
performance, they have not been found capable of acceptable
operation over bands of frequencies which are sufficiently wide to
meet various present transducer requirements. The applicant has
discovered an electroacoustic transducer element of unique design
which provides uniform response over a substantially increased band
of frequencies. The design includes features for minimizing
radiated side lobes and other unwanted response characteristics.
Thus, the broad band capabilities may be effectively used to
maximum advantage. SUMMARY OF THE INVENTION The invention herein
described is a thickness-mode electroacoustic transducer comprising
an active body having non-parallel major surfaces for transmitting
or receiving acoustic energy. At least one of the major surfaces is
subdivided by means of grooves to form a two-dimensional array of
poles. The major surfaces are provided with electrode means for
carrying electrical signals to or from the poles. In a preferred
embodiment, the non-parallel major surfaces are planar so that the
body is of a generally wedge-shaped configuration. The grooves may
be located along two intersecting sets of parallel lines so as to
form a regular pattern, and may extend to a uniform distance from
the surface opposite the grooved surface, thereby forming poles of
varying heights. The electrode means may comprise conductive foil
bonded to the major surfaces by means of an adhesive. A principle
object of this invention is to provide an improved electroacoustic
transducer which is capable of efficient operation over a wide
frequency band. A further object is to provide a wide-band
electroacoustic transducer capable of producing a satisfactory
directional response pattern at all frequencies within its
operating frequency band. Yet a further object is to provide a
uniquely configured transducing element which is suitable for
wide-band operation; is simple and economical to produce; and does
not require critical design of the transducer housing and/or
electrical signal processing circuitry. Additional objects of the
present invention may be ascertained from a study of the drawings,
specification, and appended claims.
Inventors: |
Haan; David E. (Edmonds,
WA) |
Assignee: |
Honeywell, Inc. (Minneapolis,
MN)
|
Family
ID: |
23374611 |
Appl.
No.: |
05/349,937 |
Filed: |
April 11, 1973 |
Current U.S.
Class: |
310/320; 310/337;
367/157 |
Current CPC
Class: |
B06B
1/0644 (20130101); G10K 11/32 (20130101) |
Current International
Class: |
G10K
11/32 (20060101); B06B 1/06 (20060101); G10K
11/00 (20060101); H01j 007/00 () |
Field of
Search: |
;310/8,8.2,9.6,9.5
;340/10 ;73/67.5R |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Budd; Mark O.
Claims
What is claimed is:
1. In a thickness-mode electroacoustic transducer of the type
including an active body having two major surfaces, at least one of
which is subdivided by means of grooves to form a two-dimensional
array of poles, and electrode means for carrying electrical signals
to or from the poles, the improvement which comprises an active
body wherein the major surfaces are non-parallel so that said body
is of non-uniform thickness.
2. The transducer of claim 1 further including a fluid tight
housing having a window transparent to acoustic energy, and means
for securing the assembly comprising said body and said electrode
means within said housing.
3. The transducer of claim 2 wherein said body is positioned within
said housing so that said poles are generally directed toward the
window, said assembly being bonded to the window.
4. A wide-band thickness-mode electroacoustic transducer comprising
an active body having two nonparallel major surfaces at least one
of which is subdivided by means of grooves to form a
two-dimensional array of poles, and electrode means for carrying
electrical signals to or from said poles.
5. The transducer of claim 4 wherein said body is of tapered
configuration having planar major surfaces.
6. The transducer of claim 5 wherein the grooves in one major
surface of said body extend to a uniform distance from the other
major surface, thereby forming poles of varying heights.
7. The transducer of claim 6 wherein the grooves are located along
two sets of equally-spaced parallel lines, each set intersecting
the other so as to form a regular pattern.
8. The transducer of claim 7 wherein said electrode means comprises
metal foil bonded to the major surfaces of said body by means of an
adhesive.
9. The transducer of claim 8 wherein the assembly comprising said
body and said electrode means is contained within a water tight
housing having a window transparent to acoustic energy, said body
being positioned so that the poles thereof are generally oriented
toward the window, said assembly being bonded to the window.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a perspective view of the applicant's uniquely configured
active body for an electroacoustic transducer;
FIG. 2 is a sectional view of a wide-band sonar transducer
including the active body shown in FIG. 1 with electrodes attached
and mounted in a water tight housing; and
FIG. 3 is a pair of operational curves for illustrating relative
bandwidths of the applicant's transducer and a typical prior art
wide-band transducer .
DESCRIPTION OF THE PREFERRED EMBODIMENT
The transducing element shown in FIG. 1 comprises a body 11 formed
from a thick sheet or plate of piezoelectric ceramic material.
Suitable ceramic materials for this purpose include barium titanate
and lead zirconate titanate. Body 11 has opposing nonparallel major
surfaces 12 and 13. Surfaces 12 and 13 may be planar, thus
providing for a body of wedge-shaped or tapered configuration. Sets
of grooves 14 and 15 are formed in surface 12 to subdivide the
surface into a two-dimensional array of poles 16. Each pole has a
face 17 which lies in surface 12.
Sets of grooves 14 and 15 may be located along two sets of
equally-spaced parallel lines, each set intersecting the other so
as to form a regular pattern. As shown in FIG. 1, sets of grooves
14 and 15 are at right angles to one another. However, such a
geometric relationship is not required for proper operation. The
grooves may, for example, be located along unequally spaced lines.
Further, grooves 14 may be oriented at an acute angle relative to
grooves 15.
Theoretically, the spacing between adjacent grooves should be such
that the maximum cross-sectional dimension of each pole is less
than one wave length at the resonant frequency of that pole. Thus,
the spacings between adjacent grooves may vary depending on the
location of the grooves between the thick and thin edges of the
piezoelectric body. However, from a production viewpoint, it has
been found more practical to evenly space the grooves. Also, it has
been found more effective to space the grooves so that maximum
cross-sectional dimensions of the poles are approximately one-half
wave length at the highest operating frequency of the
transducer.
Operational transducers have been constructed with spacing between
adjacent grooves as small as one millimeter. The width of the
grooves should be as small as possible to minimize the volume of
ceramic material removed, and thereby maximize the power-handling
capabilities of the transducing element. Minimum groove width is
determined by the width of the cutting or forming tool, and may be
in the order of a few thousandths of an inch.
The ceramic material from which body 11 is formed is polarized to
operate in a thickness mode. Stated otherwise, an alternating
electrical potential applied between surfaces 12 and 13 causes
alternating changes in the thickness of body 11. Conversely,
mechanical forces which cause alternating thickness changes result
in generation of an alternating potential between surfaces 12 and
13.
One of the functions of grooves 14 and 15 is to minimize mechanical
coupling between poles 16. Since any solid material connecting
individual poles results in mechanical intercoupling, optimum
operation is achieved if the grooves are as deep as possible.
However, it is also necessary to maintain the structural integrity
of body 11. For operational purposes, the depth of grooves should
be at least 75 percent of the body thickness. It has been found
that forming the grooves to a depth of 85 percent of the minimum
body thickness leaves sufficient material beneath the grooves to
prevent fracture during normal handling and operation. In the
preferred embodiment shown in FIG. 1, the grooves extend to a
uniform distance from surface 13, forming rows of poles of
increasing (or decreasing) height.
From an operational viewpoint, lateral dimensions L.sub.1 and
L.sub.2 of body 11 are dictated by directional response or beam
width requirements. Practical considerations presently limit
dimensions L.sub.1 and L.sub.2 to a maximum of approximately 2
inches. However, the effect of a larger bady can be achieved by
mounting individual bodies side by side and energizing them in
parallel.
Beam width in a given plane is inversely proportional to the
lateral dimension in that plane. Hence, beam width in a plane
parallel with indicated dimension L.sub.1 is inversely proportional
to the magnitude of L.sub.1. The beam width in a plane parallel
with indicated dimension L.sub.2 tends to be inversely proportional
to the magnitude of L.sub.2. However, the asymmetry of body 11 in
planes parallel with dimension L.sub.2 complicates the relationship
between the magnitude of dimension L.sub.2 and beam width in planes
parallel therewith. It has been found that for a thickness taper of
4 degrees, the effective radiating aperture is approximately 0.82
L.sub.2. The multiplying factor is believed to vary inversely with
taper angle.
FIG. 2 shows a complete sonar transducer in which previously
described body 11 is provided with electrodes 20 and 21 and mounted
within a fluid tight housing 22. Surfaces 12 and 13 may be prepared
in a conventional manner for attachment of electrodes 20 and 21.
For example, a silver paste may be screened on the surfaces and
fired, or the surfaces may be sprayed with a silver paint.
Electrodes 20 and 21 are then secured to the prepared surfaces.
In order to achieve optimum operation, there must be uniform
mechanical loading of the poles and minimum mechanical coupling
between poles. It is also important that the electrode on the pole
faces have a smooth and flat exterior surface for mounting against
a flat acoustic window or radiation into a fluid medium. These
requirements impose certain restrictions on electrode 20. One
improved electrode configuration which has been found quite
satisfactory comprises metal foil bonded to the pole faces by means
of an adhesive. Foil tape having a pressure sensitive adhesive
backing has been found satisfactory for this purpose.
Electrode 21 may be of the same type as electrode 20.
Alternatively, if body 11 is of the illustrated configuration
wherein grooves are formed in only one major surface, electrode 21
may be any one of various suitable prior art types of electrodes,
or a simple soldered wire connection.
Electrodes 20 and 21 are attached to insulated conductors 23 and 24
respectively. Conductors 23 and 24 pass through a fluid tight
feedthrough fitting 25 in housing 22 and into a cable 26 which
carries electrical signals between electrodes 20, 21 and
conventional electrical signal processing circuitry not shown in
FIG. 2.
Housing 22 is provided with a window 27 which is suitable for the
transmission of acoustic energy. The transducer embodiment shown in
FIG. 2 is air filled. In such an embodiment, structural acoustic
decouplers are not required. In addition, the assembly comprising
body 11 and electrodes 20, 21 may be secured directly to window 27.
As shown, the assembly is bonded to window 27 by means of a layer
of adhesive 28 between the window and electrode 20. It is, however,
pointed out that the present invention may be equally
advantageously employed in connection with fluid filled
transducers, and in connection with transducers wherein the body -
electrode assembly is not secured to the window, but is mounted
within the housing by methods which may require the use of
structural acoustic decouplers.
The improvement in wide-band response afforded by the applicant's
unique transducer configuration is evident in FIG. 3. Curve 30
represents the sound-pressure level versus frequency characteristic
of a typical transducer in accordance with the present invention.
Curve 31 represents the sound-pressure level versus frequency
characteristic of a typical prior art transducer designed to
operate over substantially the same frequency range. It can be
observed from curve 31 that the prior art transducer has a definite
resonance at a frequency between F.sub.2 and F.sub.3. The
sound-pressure level decreases relatively rapidly at frequencies
below and above the resonant frequency.
Since a relatively constant voltage level versus frequency
relationship is required for practical sonar operation, it can be
observed that the operational frequency range of the prior art
transducer is limited. The useful frequency range can be somewhat
extended by employing electronic compensation to boost voltages
having values below a desired level, and by employing damping to
reduce voltages having values above the desired level. These
techniques obviously involve critical design considerations, and
require additional equipment which increases the complexity of
resulting transducer installations. Further, although some increase
in useful bandwidth can be achieved, the total available
improvement is limited.
As shown by curve 30, the sound-pressure level versus frequency
response of a transducer in accordance with the present invention
is relatively constant, for a constant applied voltage, over a
range of frequencies extending from below F.sub.3 to approximately
F.sub.6. This relationship extends over a considerably greater
range of frequencies than that over which useful operation can be
obtained from a transducer of prior art design. If required, the
operational frequency range can be somewhat further extended by
employing electronic compensation.
Although a single embodiment of the applicant's invention has been
shown and described in detail, a variety of other embodiments and
modifications are within the applicant's contemplation and
teaching. Such embodiments and modifications will be readily
apparent to one skilled in the art having the benefit of the
teachings presented in the foregoing description and drawings.
Accordingly, the applicant does not intend to be limited to the
disclosed embodiment, but only by the terms of the appended
claims.
* * * * *