USPatent applicationPatented

Piezoelectric component

Granted 7 Oct 2008 · 1 office action

Current assignee: TDK Electronics AG · originally TDK Corporation

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Inventors: Marion Ottlinger, Heinz Florian · Examiner: Darren Schuberg · AU 2834 · TC 2800

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Abstract

A piezoelectric component includes a stack of ceramic layers and electrode layers between ceramic layers in the stack. The electrode layers contain copper and the ceramic layers contain lead-zirconate-titanate that is doped with Nb. The ceramic layers are made from a material having a composition of Pb 0.988 V 0.012 (Zr 0.504+x Ti 0.472−x Nb 0.024 )O 3.000 , where −0.05≦x≦0.05.

Description

4 parts
›TECHNICAL HELD

The invention relates to the development of piezoelectric ceramic materials for use in multilayer components with Cu internal electrodes, which are characterized by a low power loss with good deflection.

›BACKGROUND

A solution known from WO 01/45138 is based on the use of a ceramic material of the composition Pb 0.97 Nd 0.02 (Zr 0.5515 Ti 0.4485 )O 3 in piezostacks with Cu internal electrodes, the production thereof is carried out by binder removal and sintering in air.

The properties of the known actuators with the ceramic composition Pb 0.97 Nd 0.02 (Zr 0.5515 Ti 0.4485 )O 3 with in each case 360 internal electrodes and a ceramic layer thickness of 80 μm in sintering together with Cu internal electrodes are summarized in the following table, such as they are measured after a polarization with E=2 kV/mm (a) at room temperature and (b) at 180° C. Apart from the small-signal properties of the dielectric constants (DC) and the temperature dependence of the DC, the large-signal dielectric constant is also indicated here, which can be calculated from the polarization by means of a voltage, which for example leads in the case of the actuators to a deflection of 40 μm.

By means of the polarization at higher temperature, the efficiency is improved from 50% to 56% and the energy loss is reduced from 50 mJ to 34 mJ.

›SUMMARY

A ceramic material of the composition Pb 0.988 V 0.012 (Zr 0.504+x Ti 0.472−x Nb 0.024 )O 3.000 is specified according to the invention, whereby −0.05≦x≦0.05.

Furthermore, additional advantageous aspects of the invention are:

1. Adjustment of the Ti/Zr ratio to the morphotropic phase boundary.

2. Incorporation of Nb 5+ on Zr/Ti locations in the perovskite structure with donor function according to the composition Pb 0.988 V 0.012 (Zr 0.504+x Ti 0.472−x Nb 0.024 )O 3.000 , whereby V stands for a vacancy.

3. Sintering together with Cu internal electrodes at 1000° C.

Further advantages are:

1. The verification that an Nb-doped, Ag-free ceramic of the composition Pb 0.988 V 0.012 Zr 0.504+x Ti 0.472−x Nb 0.02403 is adapted in an advantageous way to the morphotropic phase boundary. With the formula Pb 0.988 V 0.012 Zr 0.504 Ti 0.472 Nb 0.02403 , a suitable analytical composition has been obtained that leads to small piezoelectric losses with acceptable deflection.

2. The deflection and energy loss of the actuator are determined through the defined incorporation of Cu 2 O during the sintering and the control of the grain-size growth through the Nb incorporation and the appropriate sintering temperature.

3. The incorporation of Nb 2 O 5 is already successful during the conversion of the raw material mixture together with the other oxide raw materials in air at 925° C.

4. After the sintering of the ceramic material Pb 0.988 V 0.012 Zr 0.504 Ti 0.472 Nb 0.024 O 3 with Cu internal electrodes under reduced oxygen partial pressure, such as corresponds to the Cu/Cu 2 O equilibrium, the dielectric constant displays a smaller dependence over temperature than with the use of an Nd-doped ceramic body Pb 0.97 V 0.1 Zr 0.55515 Ti 0.4485 O 3 .

›DETAILED DESCRIPTION

Examples of embodiment are described in the following. The precursor (Zr, Ti)O 2 and PbCO 3 or Pb 3 O 4 , produced from TiO 2 , ZrO 2 or one produced by mixed precipitation, and doping agents such as Nb 2 O 5 or another oxide of the raw material mixture consisting of rare earth elements, is weighed-in with a composition corresponding to the morphotropic phase boundary and a PbO excess of at most 5% to promote to the sintering densification, subjected to a grinding stage for the equal distribution of the components in aqueous suspension and, after filtering and drying, calcined at 900 to 950° C. in air. A piezoceramic perovskite mixed crystal phase is thus formed. In order to achieve sintering densification in 2-8 hours at 1000° C. below the melting temperature of copper, fine grinding is required down to an average grain size of 0.4-0.6 μm. The sintering activity of the powder then proves to be sufficient to produce a densification >97% of the theoretical density with at the same time adequate grain growth and adequate mechanical strength in the ceramic structure.

By using a dispersing agent, the finely ground powder is suspended to form an aqueous slurry with approx. 70 m % solid content, which corresponds to approximately 24 vol. %. The proportion of dispersing agent that is just needed for optimum distribution is ascertained separately in a series of tests, this being able to be detected when a viscosity minimum is reached. For the formation of the piezoceramic green films, approx. 6 m-% of a commercially available binder that is thermohydrolytically degradable is added to the dispersed solid powder suspensions. An aqueous polyurethane dispersion proves to be advantageous for this. Mixing is carried out for example in a Dispermat mill and a slurry suitable for the film-drawing process or for the production of a spray granulate is thus obtained.

Disc-shaped pressed pieces produced from the granulate, or multilayer platelets “MLP”, obtained by stacking one on top of another and lamination from 40 to 50 μm thick green films without printing with Cu electrode paste, can be liberated from binder down to a residual carbon <300 ppm in an inert-gas atmosphere containing H 2 O vapor at a defined oxygen partial pressure that meets the condition of the coexistence of PbO-containing piezoceramic material and copper. The hydrolytic separation of the binder takes place mainly at the relatively low temperature of 220±50° C. at a water-vapor partial pressure greater than 200 mbar. The oxygen partial pressure is adjusted to a value that is compatible with the Cu-containing electrodes. This takes place by gettering of the oxygen from the gas flow at large surfaces of Cu or by the metered addition of hydrogen. The electrode layers do contribute to binder removal insofar as they provide preferred paths for transporting away the binder, nonetheless a considerable binder removal time is required, especially for actuators with a large number of electrodes.

The electrical properties of the compact samples in the series of variable composition and those of actuators with Cu internal electrodes with optimized ceramic composition are given in the following tables.

It can be seen that the d33 value runs through a maximum value at x=0. The composition for this Ti/Zr ratio also has the lowest energy loss. Accordingly, the formula Pb 0.988 V 0.012 (Zr 0.504 Ti 0.472 Nb 0.024 )O 3.000 corresponds to a ceramic material which is adapted to the morphotropic phase boundary. The energy loss is reduced by the polarization at 120° C. and higher field strength.

The properties of the constituted actuators with Cu internal electrodes with adaptation to the morphotropic phase boundary are described in tables 2 and 3.

Compared with the actuators containing a ceramic material Pb 0.97 V 0.02 (Nd 0.02 Zr 0.5515 Ti 0.4485 )O 3.000 , the values in table 2 reveal an improvement in properties with respect to the piezoelectric losses and the temperature dependence of the small-signal capacity. With a deflection of the actuators of 30 μm, an energy loss of 20 mJ is measured. The temperature dependence of the dielectric small-signal capacity in the range between 20° C. and 60° C. is much less than with the use of the Nd-doped ceramic material. The results of the fatigue tests are shown in table 3.

Table 4 compares results of sintered and passivated actuators, when the pressure on the actuator is varied. Whilst the energy that is required for the extension of 30 μm remains of equal magnitude between 500 and 1000 N, the efficiency increases with a tendency from 61% to 63%.

It has been shown that the average sintered grain size amounts to 0.7-1.0 μm and that the interior electrodes are free from holes.

›Tables in the description — 5
Small-Large-
signal DCsignal DCTK ppm/KD 33 pm/VWg %E mJ
a1214 ± 303110 ± 873936 ± 82592 ± 1850.4 ± 0.450 ± 2
b2772 ± 50632 ± 1156.5 ± 0.434 ± 1
TABLE 1 — Properties of compact square ceramic samples MLP (edge length a = 11.5 mm, thickness h = 1 mm) in the series Pb 0.988 V 0.012 (Zr 0.504+x Ti 0.472−x Nb 0.024 )O 3.000 for the purpose of determining the morphotropic phase boundary with indication of the average statistical error from, in each case, 5 individual samples after sintering at 1000° C.
Type of∈
polari-(2 kV/D 33Eloss/V
zationxmm)[pm/V][mJ/mm 3 ]η [%]
25° C./E =03043 ± 47572 ± 1231086 ± 32344 ± 0.5
2 kV/mm+0.013469 ± 64524 ± 643313 ± 216930 ± 2
−0.012926 ± 94390 ± 1338801 ± 133426 ± 0.2
120° C./02253 ± 133518 ± 814378 ± 162857 ± 2
3 kV/mm+0.012225 ± 65464 ± 1539035 ± 230537 ± 2
−0.011676 ± 42409 ± 2724627 ± 250448 ± 5
TABLE 2 — Performance data of piezoactuators Low-loss ceramic
MagnitudesUnitin the actuator
Geometry: stackmm 36.8 × 6.8 × 30
Stroke in tube springμm30
Number of individual360
layers
Individual layer thicknessμm75
(sintered)
Small-signal capacityμF2.9 ± 0.05
polarized
Loss angle tan δmJ0.010 ± 0.001
Total energy for 30 μmmJ57.8 ± 1.0
stroke
Voltage U30 for 30 μmV162 ± 2
stroke
Large-signal capacityμF4.39 ± 0.07
Temperature dependence ofppm/K2335 ± 342
the small-signal capacity
(polarized) in the
temperature range between
20° C. 60° C.
Energy loss per 30 μmmJ19.1 ± 0.5
stroke
Triggering field strength forV/mm2160 ± 27
30 μm stroke
D 33 at triggering fieldPm/V510 ± 42
strength
Charge Q30 for 30 μmmC0.712 ± 0.005
stroke
Efficiency for 30 μm stroke%67.0 ± 0.6
TABLE 3 — Results of fatigue tests carried out Change after 4.6.10 8
MagnitudesUnitcycles
Voltage U30V+(4.7 ± 0.9) %
Charge Q30 for 30 μmmC−(2.6 ± 1.7) %
stroke
Energy for 30 μm strokemJ−(3 ± 3) %
Energy loss per 30 μmmJ−(12 ± 6) %
stroke
TABLE 4 — Pressure dependence of the efficiency, measured on sintered actuators after a polarization at room temperature with a field strength of 2 kV/mm
ForceEEloss
[N]U30 [V]EPS large[mWs]Q [mAs]Wg [%][mWs]
500190 ± 32126 ± 5476 ± 40.80 ± 0.0361 ± 130 ± 2
800191 ± 22120 ± 4176 ± 30.79 ± 0.0262.5 ± 0.428 ± 1
1000191 ± 12131 ± 3876 ± 20.80 ± 0.0263.0 ± 0.528 ± 1

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Classifications

6 codes
IPC · International Patent Classification
Section C — Chemistry; metallurgy
  • C04B35/493
Section H — Electricity
  • H10N30/853
  • H10N30/50
  • H10N30/87
  • H10N30/05
USPC · US Patent Classification
310/358

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Darren Schuberg
art unit 2834 · TC 2800
Citations: 9 back · 3 forward

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