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marco: Piezo Ceramic Componentspb |
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Piezoceramic materials are used to convert mechanical energy into electrical energy and vice versa.
The materials, based on lead-zirconate-titanate, are optimized for various specifications, thus making them suitable for many different applications in the sensor and actuator technologies.
Our manufacturing technology makes it possible to produce piezoceramics in varied and complex geometries to better serve your applications.
A large proportion of our piezoceramic products is used in our own components, actuator and sensor systems. We also supply half-finished products and components customized to our customers' needs. Our designers are at your service with their expertise in the field of production and application of piezoceramic materials, components and systems.
FPM 110
FPM 110 is a hard piezo electric material with small hysteresis and a very
high mechanical quality factor. As a hard material,
it is characterized by a
very high load constant.
It is especially suited for high performance ultrasonics. It
can also be used for sensors in multilayer technology.
Its deformation is particularly high for a hard material (
at 2 kV/mm).
FPM 231
FPM 231 is a soft material with a high deformation (
bei 2 kV/mm) and thus an excellent material for actuators such as
marco's Torque-Blocks®, bending elements and multilayer stacks.
It is a soft piezoelectric material with a low mechanical
quality factor and relatively high dielectric constant. FPM 231 is
characterized by a very high piezoelectric load constant.
The material can be manufactured in film technology.
FPM 220
FPM 220 is also a soft piezoceramic material which is mainly used for
high-voltage actuators. FPM 220 is a standard material with a high piezo
electric load constant and a medium mechanical quality factor.
The deformation of this material is slightly lower than that of FPM 231 with
at 2 kV/mm.
FPM 202
This soft material features high electromechanical coupling factors, a low relative dielectric constant, and high piezoelectric load and pressure constants. It can be used for air ultrasonic sensors, modular transducers, accelerometers, and similar devices. Its high Curie temperature makes it suitable for use in extended temperature ranges.
FPM 203
FPM 203 is specially designed for high-voltage actuators used in an extended
temperature range. Its high Curie temperature is, however,
coupled with greater temperature coefficients of the dielectric constant.
Its low dielectric constant and high deformation (approx. 1.8
)
present great advantages for the
multilayer actuator technology. FPM 203 can also be used for ultrasonic
applications. Its frequency constants are very similar to those of FPM\
202.
FPM 240
FPM 240 is specially designed for bender actuators.
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Plates
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Side Dimensions a x b [mm]: min 2x2 to max 50x50; 70x20
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Thickness d [mm]: 0.2; 0.5; 1; 1.5 - 5
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(depending on side dimensions)
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e.g.: pb/202/v/p2/27x5
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Discs/Cylinders
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Diameter Ø [mm]: 5; 10; 15; 16; 20; 25; 30
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Thickness d [mm]: 0.2; 0.5; 1; 1.5 - 15
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(depending on diameter)
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e.g.: pb/110/v/d0,5/10
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adhesive multi-layer metallization with a Cu-Ni coating
as the standard metallization, easily soldered
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Cu coatings are available for special applications
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One Electrode with side contact and indent
One Electrode with contact to other side
Special electrodes
Piezo Electric Ceramic Specifications, Low-Level Signal Values
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Electromechanical
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Symbol
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Unit
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Material
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Parameter
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FPM 202
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FPM 203
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FPM 231
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FPM 220
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FPM 240
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FPM 110
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Density
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7,71
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7,64
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7,7
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7,8
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7,82
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7,68
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Relative
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1560
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800
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2990
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2650
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3680
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1075
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Dielectric Constant
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1600
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1160
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2930
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2085
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3650
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1480
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950
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700
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2180
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1385
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2090
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910
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780
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370
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1410
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1260
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1470
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648
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Dielectric
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tan |
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18
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21
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22
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20
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19
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6
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Loss Factor
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· |
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Curie Temperature
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°C
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365
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360
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192
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220
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202
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272
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Electromechanical
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62
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62
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61
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63
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69
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51
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Coupling Factor
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35
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32
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39
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32
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43
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32
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%
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65
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64
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63
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66
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72
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64
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44
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51
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50
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46
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50
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43
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64
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63
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50
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58
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65
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62
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Piezoelectric
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C/N (m/V)
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330
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220
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500
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430
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630
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270
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Load Constant
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-165
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-104
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-260
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-200
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-300
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110
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510
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425
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525
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506
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807
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440
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C/N (m/V)
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Mechanical
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86
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88
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77
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82
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75
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1400
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Quality Factor
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Temperature Coefficient*
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by |
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3,6
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10,4
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8,4
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5
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7,4
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6,4
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by |
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-0,2
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0,9
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-3
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-0,5
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-2,1
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-0,2
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by |
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-0,9
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0,6
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-3
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-0,4
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-2,5
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-0,8
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by |
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1,8
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5
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-0,4
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1
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2,3
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1,3
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by |
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-2,8
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-1,6
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-5
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-2
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-5
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-2,9
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· |
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Elastic
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16
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15
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16
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16
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15
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13
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Compliance
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10
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10
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10
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10
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9
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8
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27
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27
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31
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27
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27
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23
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14
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13
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14
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15
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12
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11
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46
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44
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42
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41
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47
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38
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18
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17
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17
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17
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20
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15
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5
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7
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2
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8
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3
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3
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10
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9
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9
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10
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10
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7
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· |
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Elastic
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14,6
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15,3
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14,8
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15,6
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15,8
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15,1
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Stiffness
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11,8
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11,2
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11,1
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12,2
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12
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12,3
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3,7
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3,7
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3,2
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3,6
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3,7
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4,3
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2,2
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2,3
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2,4
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2,4
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2,1
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2,6
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9,6
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10,7
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8,9
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10,2
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10,6
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11
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0,1
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-1,7
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1,5
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-1,6
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2,1
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1
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-5,5
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-4,9
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-5,3
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-5,2
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-6,6
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-5,7
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planar Poisson's number
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0,296
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0,296
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0,295
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0,297
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0,300
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0,287
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Frequency Constant
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1985
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2035
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1970
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1985
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1910
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2255
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1420
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1490
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1420
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1390
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1450
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1610
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Hzm
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1405
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1440
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1415
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1420
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1335
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1548
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1996
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1969
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1940
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2022
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2000
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2034
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874
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893
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902
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910
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858
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957
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Piezoelectric
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23
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32
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14
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18
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16
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23
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Voltage Constant
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-11
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-15
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-10
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-8
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-9
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-12
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36
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41
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20
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27
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25
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34
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Vm/N
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Specific Resistance
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Ohmm
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2 · |
0,5 · |
0,5 · |
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Measurements were in progress on DIN EN 50324-2 VDE 0336-2 "Piezoelektrische Eigenschaften von keramischen Werkstoffen und Komponenten" Teil 2: Messverfahren - Kleinsignal (Dezember 2002).
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marco Systemanalyse und Entwicklung GmbH Hans-Böckler-Str. 2 . D-85221 Dachau Tel (+49) [0] 8131 5161 0 . Fax (+49) [0] 8131 5161 66 |
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