U.S. patent number 3,659,127 [Application Number 05/075,598] was granted by the patent office on 1972-04-25 for piezoelectric ceramic transformer with specific width to length ratios.
This patent grant is currently assigned to Sumitomo Electric Industries, Ltd.. Invention is credited to Osamu Kumon.
United States Patent |
3,659,127 |
Kumon |
April 25, 1972 |
PIEZOELECTRIC CERAMIC TRANSFORMER WITH SPECIFIC WIDTH TO LENGTH
RATIOS
Abstract
A piezoelectric ceramic transformer of the plate type having a
total length 2L and width W is driven into fundamental mode,
longitudinal vibration by an A.C. input, the wave length of which
is .lambda., that is, 2L = .lambda./2. When the ratio W/L falls
within the range of 0.2 to 1.2 a high voltage output and a high
input-to-output power efficiency are attained. Alternatively, the
piezoelectric ceramic transformer referred to above is driven into
second, higher harmonic mode longitudinal vibrations where 2L =
.lambda.. When the ratio W/L falls within the range of 0.05 to 0.85
the high performance referred to above is also attained.
Inventors: |
Kumon; Osamu (Itami-shi,
JA) |
Assignee: |
Sumitomo Electric Industries,
Ltd. (Osaka, JA)
|
Family
ID: |
27302829 |
Appl.
No.: |
05/075,598 |
Filed: |
September 25, 1970 |
Foreign Application Priority Data
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Oct 1, 1969 [JA] |
|
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44/78855 |
Nov 14, 1969 [JA] |
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44/108808 |
Nov 14, 1969 [JA] |
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44/108809 |
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Current U.S.
Class: |
310/359;
310/368 |
Current CPC
Class: |
H01L
41/107 (20130101) |
Current International
Class: |
H01L
41/107 (20060101); H01v 007/00 () |
Field of
Search: |
;310/8,9.5,9.6,9.7,9.8
;333/72 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Miller; J. D.
Assistant Examiner: Budd; Mark O.
Claims
What is claimed is:
1. A piezo-electric ceramic transformer of generally rectangular,
parallelopiped configuration, said transformer having a
longitudinal length of 2L, a thickness T and a width W, which
comprises:
1. a first region electrically polarized in a thickness-wise
direction;
2. a second region electrically polarized in the longitudinal
direction;
3. a pair of input electrodes applied to opposite surfaces of said
first region for receiving an energizing A.C. voltage from an
external source;
4. an output electrode applied to an end face of said second
region, one of the electrodes associated with said first region
functioning as a common electrode for said output electrode,
wherein
5. for applications where said transformer is driven into
fundamental mode longitudinal vibrations by said source, the
improvement comprises adjusting the dimensions of the transformer
so that the width to length ratio W/L falls within the range of
from 0.2 to 1.2.
2. The piezo-electric ceramic transformer according to claim 1,
wherein the one of said pair of input electrodes connected to a
source of positive potential, with respect to the other one of said
pair of electrodes, is connected to the ground side of the output
circuitry connected to said output electrode as the common
electrode therefor.
3. A piezo-electric ceramic transformer of generally rectangular,
parallelopiped configuration, said transformer having a
longitudinal length of 2L, a thickness T and a width W, which
comprises:
1. a first region electrically polarized in a thickness-wise
direction;
2. a second region electrically polarized in the longitudinal
direction;
3. a pair of input electrodes applied to opposite surfaces of said
first region for receiving an energizing A.C. voltage from an
external source;
4. an output electrode applied to an end face of said second
region, one of the electrodes associated with said first region
functioning as a common electrode for said output electrode,
wherein
5. for applications where said transformer is driven into second
harmonic longitudinal vibrations by said source, the improvement
comprises adjusting the dimensions of the transformer such that the
width to length ratio W/L falls within the range of from 0.05 to
0.85.
4. The piezoelectric ceramic transformer according to claim 3
wherein the one of said pair of input electrodes connected to a
source of positive potential, with respect to the other one of said
pair of electrodes, is connected to the ground side of the output
circuitry connected to said output electrode as the common
electrode therefor.
Description
BACKGROUND OF THE INVENTION
This invention relates to an improved piezoelectric ceramic
transformer for high voltage generation and, more particularly, to
a structure for the above type transformer which gives a large
voltage step-up ratio, hitherto unattained in such
transformers.
It is an object of the present invention to provide a piezoelectric
ceramic transformer having a width-to-length ratio such that, when
driven into fundamental mode longitudinal vibration, the
transformer gives a high voltage output and power efficiency.
It is another object of the present invention to provide a
piezoelectric ceramic transformer having a width-to-length ratio
such that, when driven into second harmonic mode longitudinal
vibration, the transformer gives a high voltage output and power
efficiency.
It is an additional object of the present invention to provide a
novel connection for a piezoelectric ceramic transformer, which
relates to the direction of polarization and the ground side of an
output circuit of the transformer and gives a higher voltage output
than the other connections give.
SUMMARY OF THE INVENTION
In accordance with the present invention, a piezoelectric ceramic
transformer of the plate type having a width W and a total length
2L is driven into a fundamental mode, longitudinal vibration under
the condition that the width-to-length ratio W/L falls within the
range of 0.2 to 1.2.
In accordance with a second feature of the present invention, the
above transformer is driven into a second, higher harmonic mode of
longitudinal vibration, under the condition that the
width-to-length ratio W/L falls within the range of 0.05 to
0.85.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a perspective view of a piezoelectric, ceramic
transformer with electrical connections thereto;
FIG. 2 is a view showing schematically two vibration modes of the
ceramic transformer wherein a solid curve a depicts the magnitude
of displacement of the lengthwise vibration in the fundamental mode
(.lambda./2 mode) and a dotted curve b depicts the magnitude of
displacement in a second, higher harmonic mode (.lambda.mode);
FIG. 3 is a graph showing a voltage step-up ratio versus the ratio
between the width and the length of the ceramic transformer, in
fundamental mode vibration;
FIG. 4 is a graph showing the voltage step-up ratio versus the
ratio between the width and the length of the ceramic transformer
in a second, higher harmonic mode vibration;
FIGS. 5A and 5B are diagrammatic side views diagrammatic of the
ceramic transformer showing the relationship between the
polarization direction and the electrode connection where FIG. 5A
relates to a conventional connection system and FIG. 5B to the
present invention.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Referring to FIG. 1, showing the general structure of a
piezoelectric ceramic transformer PCT, it is well known in the art
that a transformer function can be produced by plating electrodes
E.sub.IN, E.sub.IN ' and E.sub.OUT on a plate of ferro-dielectric
material and by effecting a polarization process in two directions,
perpendicular to each other, as shown by the arrows P. Such ceramic
transformers, manufactured as above described, have a high degree
of frequency selectivity, and may seem to be a constant voltage
source for a high resistance load and a constant current source for
a low resistance load.
When operated as a constant voltage source, the voltage step-up
ratio G.infin. of the ceramic transformer with no load across
output terminals may be given by:
where,
Q.sub.m is indicative of the degrees of mechanical vibration,
K.sub.31, K.sub.33 are electro-mechanical coupling factors in the
direction perpendicular to the polarization direction and in the
same direction, respectively,
L is the length of the sample,
and T is the thickness of the sample.
It is known in the art that the dimension of a ceramic plate
transformer affects its step-up ratio and that the step-up ratio is
proportional to the length, and inversely proportional to the
thickness, of the plate, as seen from the above equation (1), but
heretofore qualitative information relative to the width of the
plate was not known.
In driving a ceramic transformer, there are principally two modes
of lengthwise vibration, as shown schematically in FIG. 2, which
provide useful voltage step-up ratios. In this drawing the curve a
illustrates the magnitude of displacement in fundamental mode
vibration, in which the length 2L of the transformer is equal to
.lambda./2, ".lambda." being the wave length of the A.C. input
voltage, and the curve b illustrates the magnitude of displacement
in second, higher harmonic mode vibrations in which 2L =
.lambda..
The data plotted in FIG. 3 was obtained by connecting, as shown in
FIG. 1, an A.C. voltage source OSC across electrodes E.sub.IN,
E.sub.IN ' and an output circuit, consisting of a voltage doubler
rectifier, comprising diodes D.sub.1 and D.sub.2, and a load
resistor R.sub.L, across the output electrode E.sub.OUT and the
ground electrode E.sub.IN '.
The frequency of the input voltage was selected so as to drive the
transformer into fundamental mode longitudinal vibrations.
In FIG. 3, the ordinate represents the voltage step-up ratio
(V.sub.2 /V.sub.1) between the input voltage V.sub.1 (r.m.s. volts)
and the output voltage V.sub.2 (r.m.s. volts) after rectification,
and the abscissa represents the width-to-length ratio (W/L) between
the width W and half of the total length 2L of the test
piezoelectric ceramic transformer PCT.
As will be seen from the graph of FIG. 3, the step-up ratio,
without load, is as high as 300, or more, for a W/L range of 0.2 to
1.2, but with a W/L ratio falling without the above range, no
substantial amount of lengthwise vibration in the longitudinal
direction is produced and the step-ratio is small, due to the
influence of other mode vibrations.
Accordingly, when driven in fundamental mode with a W/L range of
0.2 to 1.2, the step-up ratio, with no load at the output, becomes
300 or more, and the step-up ratio with a load resistor of 100
M.OMEGA. for example, becomes 100, or more. It will be noted that
with L = 5 - 80 mm and T/L = 0.02 - 0.4, the maximum output voltage
was 30 KV.
Similarly, FIG. 4 illustrates the relationship between the voltage
step-up ratio and the width-to-length ratio when the ceramic
transformer was driven in a second higher harmonic mode. As will be
seen from the graph of FIG. 4, the step-up ratio with no load is as
high as 300 or more for a W/L range of from 0.05 to 0.85.
Accordingly, when driven in second, higher harmonic mode, with a
W/L range of 0.05 to 0.85, the step-up ratio, with no load, is 300
or more, and the step-up ratio with a load resistor of 100
M.OMEGA., for example, is 100, or more. It will be noted that with
L = 5 - 80 mm, and T/L = 0.02 - 0.4, the maximum output voltage is
30 KV.
It is also found that within the foregoing W/L ranges, in either
vibration mode, the input-to-output power efficiency is also
high.
Piezo-ceramic material develops an effective piezoelectric
performance only when a high D.C. voltage (about 2 KV/mm) is
applied thereto. The polarization appears in the directions shown
by the arrows in FIGS. 5A and 5B where, in FIG. 5A which shows a
conventional connection, the downward short arrow on the left
represents the fact that a positive potential was applied to the
upper electrode E.sub.IN when the polarization process took place.
Thus, the lower electrode E.sub.IN ' which was supplied with a
negative potential at the time of polarization is connected to the
ground side of the output circuitry.
In accordance with the present invention, however, the lower input
electrode E.sub.IN, in FIG. 5B, which shows the connection
according to the present invention, and which was supplied with a
positive potential when the polarization process took place, is
connected to the ground side of the output circuitry, and the
direction of polarization is upward.
Table 1 below shows the voltage step-up ratio (V.sub.2 /V.sub.1)
obtained using the conventional connection shown in FIG. 5A the
ratio (V.sub.2 '/V.sub.1 ') and obtained using the present
connection, as shown in FIG. 5B.
TABLE 1
Dimension: L = 28 mm T = 3.5 mm W = 15 mm Load: 100 M.OMEGA.
step-up ratio Sample (b)/(a) No. (a) V.sub.2 /V.sub.1 (b) V.sub.2
'/V.sub.1 ' 1 270 283 1.05 2 283 300 1.06 3 277 290 1.05 4 297 305
1.03 5 270 290 1.07 6 277 290 1.05 7 303 330 1.09 8 273 295 1.08 9
300 320 1.07 10 297 307 1.03
as seen from Table 1, the step-up ratio of a transformer using the
electrical connection according to the present invention is higher
than that of a conventional connection by from 3 to 9 percent.
However, no difference between the present connection and a
conventional connection was noted with respect to other
characteristics, such as resonance frequency, output voltage
regulation, self heating, and the like.
A piezoelectric ceramic transformer, in accordance with the present
invention, has a specific width-to-length ratio (W/L), which
results in a high voltage output heretofore unattainable in the
art. Further, the transformer is very reliable with respect to its
insulation characteristics and is noncombustible, so that the
present invention is very effective for practical use in high
voltage and power generation.
* * * * *