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Claims  |
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We claim:
1. A piezoelectric ceramic composition for actuators, which consists
essentially of a composite of perovskite compounds represented by the
formula
Pb.sub.(1-x) La.sub.x [z {(Zn.sub..alpha. Mg.sub.(1-.alpha.)).sub.1/3
Nb.sub.2/3 }+(1-z){]Zr.sub.y Ti.sub.(1-y) }].sub.(1-x/4) O.sub.3
wherein 0.03.ltoreq.x.ltoreq.0.07, 0.50.ltoreq.y.ltoreq.0.65, 0<z<0.20, and
0<.alpha.<1.
2. The composition according to claim 1, wherein
0.045.ltoreq.x.ltoreq.0.07, and 0.02.ltoreq.z.ltoreq.0.12.
3. The composition according to claim 1, wherein x=0.045, y=0.55, and
z=0.12.
4. The composition according to claim 1, wherein x=0.06, y=0.57, and
z=0.02.
5. The composition according to claim 1, wherein x=0.06, y=0.58, and
z=0.02.
6. The composition according to claim 1, wherein x=0.06, y=0.565, z=0.10,
and u=0.3.
7. The composition according to claim 1, wherein x=0 06, y=0.57, z=0 10,
and u=0.3.
8. The composition according to claim 1, wherein x=0.06, y=0.57, z=0.10,
and u=0.5. |
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Claims  |
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Description  |
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The present invention relates to a piezoelectric ceramic composition for
actuators.
Here, actuators are devices which utilize a reverse piezoelectric effect
i.e. an effect to convert electrical energy to mechanical energy, and they
are designed to perform fine displacement of micron or submicron order
accurately. In recent years, research and development have been actively
conducted for their applications, for example, to precise control of the
sound of a buzzer or the flow rate of a pump or a valve, to auto-tracking
of a VTR head, to auto-focussing, or to apparatus for precise positioning
of a mechanical cutting tool in a submicron order or for fine positioning
for the production of semiconductors.
Heretofore, a lead zirconate titanate ceramic composition (PZT) is known to
have excellent piezoelectric properties as a piezoelectric material for
actuators. Various improvements have been made depending upon the
particular purposes. For example, there have been improvements in the
properties of the piezoelectric material for actuators, effected by a
method wherein a part of the lead zirconate titanate is substituted by a
bivalent ion such as Ba.sup.2+, Sr.sup.2+ or Ca.sup.2+, or by a trivalent
ion such as Bi.sup.3+ or La.sup.3+, or by a method wherein a solid
solution with a composite of perovskite compounds such as Pb(Ni.sub.1/2
W.sub.1/2)O.sub.3, Pb(Co.sub.1/3 Nb.sub.2/3)O.sub.3 and Pb(Ni.sub.1/3
Nb2/3)O.sub.3, is prepared. Unimorph-type, bimorph-type and laminate-type
are known for piezoelectric actuator elements for controlling fine
displacement with a precision of micron or submicron order. They are
required to have a high piezoelectric strain constant (e.g., transverse
mode piezoelectric strain constant d.sub.31 >300.times.10.sup.-12 C/N) and
a high Curie temperature (Tc>150.degree. C.).
In general, with a material having a high piezoelectric strain constant,
the Curie temperature is low. For example, with a conventional material
having a high piezoelectric strain constant at a level of a transverse
mode piezoelectric strain constant (d.sub.31) exceeding
300.times.10.sup.-12 C/N, the Curie temperature Tc tends to be as low as
about 100.degree. C., whereby the upper limit of the practical temperature
of the element used to be from 50.degree. to 60.degree. C., and the
application as a practical element has been limited. On the other hand, a
material having a high Curie temperature tends to have a low piezoelectric
strain constant, whereby a high voltage used to be required for the
operation of such an element. Accordingly, it has been desired to develop
a material having a high piezoelectric strain constant at a level of a
transverse mode piezoelectric strain constant (d.sub.31) exceeding
300.times.10.sup.-12 C/N and a high Curie temperature (e.g. Tc>150.degree.
C.) at the same time.
The present inventors have conducted detailed studies of the compositions
to solve the above problems. As a result, it has been found that a
piezoelectric ceramic composition represented by the formula
Pb.sub.(1-x) La.sub.x [z {(Zn.sub..alpha. Mg.sub.(1-.alpha.)).sub.1/3
Nb.sub.2/3 }+(1-z){Zr.sub.y Ti.sub.(1-y) }].sub.(1-x/4) O.sub.3
has a high electromechanical coupling factor, a high piezoelectric strain
constant and a high Curie temperature. The present invention has been
accomplished on the basis of this discovery.
The present invention provides a piezoelectric ceramic composition for
actuators, which consists essentially of a composite of perovskite
compounds represented by the formula
Pb.sub.(1-x) La.sub.x [z {(Zn.sub..alpha. Mg.sub.(1-.alpha.)).sub.1/3
Nb.sub.2/3 }+(1-z){]Zr.sub.y Ti.sub.(1-y) }].sub.(1-x/4) O.sub.3
wherein 0.03.ltoreq.x.ltoreq.0.07, 0.50.ltoreq.y.ltoreq.0.65, 0<z<0.20, and
0<.alpha.<1.
Now, the present invention will be described in detail with reference to
the preferred embodiments.
In the accompanying drawings:
FIG. 1 is a photograph showing the structure of particles when the
thermally etched surface of a piezoelectric ceramic composition for
actuator according to the present invention was observed by a scanning
electron microscope (.times.5000).
FIG. 2 is a graph showing the relation between the intensity of electric
field and the strain induced in the longitudinal direction (i.e. the
direction of electric field) when an electric field of 1.0 KV/mm is
applied to a polarized piezoelectric ceramic composition for actuators in
the same direction as the direction for polarization treatment.
The ceramic composition of the present invention has a very high
piezoelectric strain constant. The composition at the morphotropic phase
boundary (MPB) of the perovskite crystals of the above formula wherein
0.045.ltoreq.x.ltoreq.0.07 and 0.02.ltoreq.z.ltoreq. 0.12, has a
transverse piezoelectric strain constant (d.sub.31) exceeding
300.times.10.sup.-12 C/N and a Curie temperature (Tc) of at least
150.degree. C., whereby the above problems can be overcome, and thus it is
very suitable as a material for piezoelectric actuators.
Among them, those having compositions wherein x=0.045, y=0.55, z=0.12 and
.alpha.=0.5; x=0.06, y=0.57, z=0.02 and u=0.5; and x=0.06, y=0.58, z=0.02,
and .alpha.=0.5 (Examples 5, 6 and 7) have a transverse mode piezoelectric
strain constant (d.sub.31) exceeding 300.times.10.sup.-12 C/N and a Curie
temperature of at least 200.degree. C. and thus have a merit that they can
be used within a wide range of the temperature conditions as materials for
piezoelectric actuators. Further, those having compositions wherein
x=0.06, y=0.565, z=0.10 and u=0.3; x=0.06, y=0.57, z=0.10 and u=0.3; and
x=0.06, y=0.57, z=0.10 and u=0.5 (Examples 10, 11 and 14), have a
transverse mode piezoelectric strain constant (d.sub.31) exceeding
350.times.10.sup.-12 C/N and a Curie temperature of higher than
150.degree. C., and they are very excellent as materials for piezoelectric
actuators.
Here, if the amount of La exceeds 0.07, Tc is likely to be less than
150.degree. C., and d.sub.31 will be small at a level of not more than
250.times.10.sup.-12 C/N, such being unsuitable as a material for
piezoelectric actuators. If the amount y of Zr is less than 0.50 or more
than 0.65, the Zr/Ti ratio departs substantially from the morphotropic
phase boundary of the perovskite crystals, whereby d.sub.31 will be low.
If the amount z of (Zn.sub..alpha. Mg.sub.(I-.alpha.)).sub.1/3 Nb.sub.2/3
is more than 0.20, Tc tends to be less than 150.degree. C., and a
pyrochlore phase tends to be present in the sintered product, whereby the
piezoelectric strain constant will be low, such being undesirable.
An element such as a piezoelectric actuator wherein a mechanical
displacement induced by an electric field is utilized, is required to have
high mechanical strength. The mechanical strength of a ceramic material
depends largely on the sinterability of ceramics and the size of the
crystal particles. In general, the finer and the denser the crystal
particles of the sintered ceramic product, the higher the mechanical
strength.
The densities of the sintered products obtained by the present invention
were compared with the theoretical densities calculated from the X-ray
diffraction angles, whereby all of them were at least 97% of the
theoretical densities.
Further, the surface of the obtained sintered product was polished to
obtain a specular surface and then subjected to thermal etching treatment.
Then, the fine structure was observed by means of a scanning electron
microscope, whereby it was found to be composed of crystal particles
having a diameter at a level of from 2 to 5 .mu.m, and it had a highly
dense, uniform and fine structure. Thus, the ceramic composition of the
present invention is excellent in the sinterability, whereby it is
possible to obtain a sintered product having a uniform particle size of
fine particles. Also from this viewpoint, the ceramic composition of the
present invention is suitable for an element such as a piezoelectric
actuator wherein a mechanical displacement is utilized. In the composition
of the present invention, the quantitative relation of the respective
components, particularly the relation of the total amounts of Zn, Mg and
Nb, and La and Zn, Mg, Nb, Zr and Ti, should preferably be as represented
by the above-mentioned formula. However, so long as a composite compound
obtained essentially has a perovskite structure, and the nature of the
perovskite structure substantially governs the entire composition as a
whole, such a composition should be regarded as included in the scope of
the present invention even if the composition departs from the above
formula to some extent.
The ceramic composition of the present invention may be obtained, for
example, by weighing powder starting materials for a predetermined
proportions, mixing the mixture in a wet system from 12 to 24 hours by
e.g. a ball mill, then presintering it at a temperature of from
850.degree. to 950.degree. C. for 1 to 2 hours, pulverizing the
presintered product again for from 12 to 24 hours in a ball mill, followed
by sintering at a temperature of from 1,100.degree. to 1,200.degree. C.
for from 1 to 16 hours. The sintered product thus obtained is electroded
by firing and then subjected to polarization treatment by a usual method.
In the case of the composition of the present invention, it is preferred
that it is converted to a piezoelectric ceramic material by a mild
polarization treatment, for example, at a temperature of from 20.degree.
to 80.degree. C. at an electric field intensity of from 1.0 to 3.0 KV/mm
for a period of from 3 to 20 minutes.
Now, the present invention will be described in further detail with
reference to Examples. However, it should be understood that the present
invention is by no means restricted by such specific Examples.
EXAMPLES 1 to 22 and COMPARATIVE EXAMPLES 1 to 8
PbO, TiO.sub.2, ZrO.sub.2, La.sub.2 O.sub.3, MgO, ZnO and Nb.sub.2 O.sub.5
(3N reagents, manufactured by Furuuchi Kagaku K.K.) were weighed to bring
the proportions as identified in Table 1 and then mixed in a wet system
for 24 hours together with ethanol in a ball mill by means of zirconium
oxide (ZrO.sub.2) balls. After completion of the mixing, the mixture was
dried, uniaxially pressed under a molding pressure of 1 ton/cm.sup.2 and
then presintered at 900.degree. C. for 2 hours. The presintered product
was manually pulverized and then subjected again to pulverization by a
ball mill for 24 hours to obtain a powder for sintering. The powder for
sintering was preliminarily molded in a mold having a diameter of 20 mm
and then finally molded by a rubber pressing method under a molding
pressure of 1 ton/cm.sup.2.
The molded product thus obtained was put into a high alumina crucible, then
covered with a powder for a lead atmosphere and sintered at 1,200.degree.
C. for 8 hours.
FIG. 1 is a photograph of the particle structure when the surface of the
sintered product obtained in Example 10 was polished to a specular
surface, subjected to thermal etching treatment and then observed by a
scanning electron microscope (.times.5000). From this FIG., it is evident
that the product is a ceramic sintered body having a dense structure with
uniform particles size of from 2 to 5 .mu.m. The disc shaped sintered
product thus obtained was polished to have a thickness of 1 mm, and a
silver paste was screen-printed to each side and fired at 600.degree. C.,
to obtain a sample for measuring the Curie temperature.
The disc-shaped sintered product was polished in the same manner to a
thickness of 1 mm and then punched out into a shape of 12 mm in length, 1
mm in thickness and 3 mm in width by means of a supersonic cutter. Then, a
silver electrode was fired in the same manner to obtain a sample for
measuring the piezoelectric strain constant (d.sub.31). The Curie
temperature was determined by measuring the dielectric constant at a
measuring frequency of 100 KHz.
The piezoelectric strain constant d.sub.31 was measured as follows. The
sample for the transverse mode obtained by punching out was immersed in a
silicon oil bath, the sample was polarized by applying electric field of
from 1.5 to 3.0 KV/mm at 70.degree. C., and then aged for 24 hours, and
then d.sub.31 constant was measured by means of a vector impedance
analyzer at a measuring temperature of 20.degree. C.
The results of the measurements of the piezoelectric properties and the
Curie temperatures are shown in Table 1. In Table 1, .epsilon..sub.33
T/.epsilon..sub.0 represents the dielectric constant, K.sub.31 represents
the electromechanical coupling factor, d.sub.31 represents the transverse
mode piezoelectric strain constant (unit:.times.10.sup.-12 C/N},
S.sub.11.sup.E) represents the elastic compliance (unit:.times.10.sup.-
m.sup.2 /N), and Tc represents the Curie temperature.
FIG. 2 is a graph showing the relation between the strain add the applied
electric field intensity when the strain induced in the longitudinal
direction (i.e. the direction of the electric field) by an application of
an electric field of 1.0 KV/mm in the same direction as the direction for
polarization applied to the sample, was measured by an eddy current type
high sensitivity displacement sensor (resolution: 25.ANG.). The wave form
of the applied voltage was a triangular wave form, and the sweeping was
conducted at a frequency of 4/100Hz. As the sample for the measurement,
the above-mentioned disc-shaped sample was subjected to polarization
treatment under the same condition as mentioned above and then aged for 24
hours, and then the strain was measured.
It is known that the strain in the longitudinal direction of presently
available piezoelectric actuator material is usually at a level of about
0.1% (10.times.10.sup.-4) under an electric field of 1.0 KV/mm. One of
such examples is PLZT (6/58/42) shown as the Comparative Example. Whereas,
the strain of the composition of the present invention e.g. Example 10,
substantially exceeds 10.times.10.sup.-4 and thus is very suitable for use
as a material for piezoelectric actuators.
TABLE 1
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Sintered
mol % .times. 100
density
Tc S.sub.11.sup.E
d.sub.31
x y Z .alpha.
(g/cm.sup.2)
(.degree.C.)
.epsilon..sub.33 T/.epsilon..sub.0
K.sub.31
(.times. 10.sup.-11 m.sup.2 /N)
(.times. 10.sup.-11
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C/N)
Example 1
3.5
50 16 0.3
7.81 237
3240
0.377
1.504 247
Example 2
3.5
51 16 0.3
7.82 234
3332
0.414
1.516 276
Example 3
3.5
52 16 0.3
7.80 230
2603
0.426
1.458 247
Example 4
4.5
54 12 0.5
7.79 222
3555
0.398
1.545 277
Example 5
4.5
55 12 0.5
7.82 217
3670
0.420
1.595 302
Example 6
6 57 2 0.5
7.81 209
4120
0.422
1.572 319
Example 7
6 58 2 0.5
7.82 206
4290
0.441
1.615 345
Example 8
6 59 2 0.5
7.80 202
3790
0.410
1.493 290
Example 9
6 56 10 0.3
7.82 179
5171
0.400
1.506 332
Example 10
6 56.5
10 0.3
7.79 177
5436
0.432
1.588 377
Example 11
6 57 10 0.3
7.78 175
5240
0.410
1.600 353
Example 12
6 58 10 0.3
7.77 171
3967
0.423
1.455 302
Example 13
6 56 10 0.5
7.78 180
5314
0.389
1.539 331
Example 14
6 57 10 0.5
7.79 176
5272
0.429
1.553 365
Example 15
7 58 6 0.3
7.79 157
5230
0.377
1.495 313
Example 16
7 59 6 0.3
7.78 154
5706
0.387
1.509 338
Example 17
7 60 6 0.3
7.78 150
5864
0.394
1.490 346
Example 18
7 61 6 0.3
7.77 146
5688
0.386
1.501 335
Example 19
7 58 6 0.5
7.80 160
5001
0.368
1.471 297
Example 20
7 59 6 0.5
7.76 156
5598
0.385
1.504 332
Example 21
7 60 6 0.5
7.79 153
5807
0.384
1.538 341
Example 22
7 61 6 0.5
7.77 150
5762
0.378
1.498 330
Comparative
Example 1
7 60 0 7.75 172
4305
0.361
1.497 273
Comparative
Example 2
6 58 0 7.74 221
3620
0.419
1.511 291
Comparative
Example 3
5 57 0 7.72 254
2320
0.386
1.495 214
Comparative
Example 4
4 56 0 7.77 252
1669
0.394
1.444 182
Comparative
Example 5
7.5
60 2 0.5
7.79 141
4251
0.331
1.398 239
Comparative Not
Example 6
8 60 2 0.5
7.78 129
measured
Comparative Pyrochlore phase present
Example 7
3.5
53 20 0.5
7.82
Comparative
Example 8
3.5
53 22 0.5
7.83
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The piezoelectric ceramic composition obtained by the present invention has
a high electromechanical coupling factor, a high piezoelectric strain
constant (strain) and a high Curie temperature, and it is a ceramic
composition having excellent sinterability. Therefore, it is useful for
various piezoelectric materials. It has a particularly large piezoelectric
strain constant, thus exhibits a large strain induced by an electric field
and also has a high Curie temperature, whereby the temperature range of
the use of the element is wide, and it is extremely useful as a material
for piezoelectric actuators. Thus, the contribution of the present
invention to the practical industrial application is very significant.
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Description  |
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