Advanced Piezoelectric Materials: Science and TechnologyKenji Uchino Elsevier, 27.09.2010 - 696 Seiten Piezoelectric materials produce electric charges on their surfaces as a consequence of applying mechanical stress. They are used in the fabrication of a growing range of devices such as transducers (used, for example, in ultrasound scanning), actuators (deployed in such areas as vibration suppression in optical and microelectronic engineering), pressure sensor devices (such as gyroscopes) and increasingly as a way of producing energy. Their versatility has led to a wealth of research to broaden the range of piezoelectric materials and their potential uses. Advanced piezoelectric materials: science and technology provides a comprehensive review of these new materials, their properties, methods of manufacture and applications. After an introductory overview of the development of piezoelectric materials, Part one reviews the various types of piezoelectric material, ranging from lead zirconate titanate (PZT) piezo-ceramics, relaxor ferroelectric ceramics, lead-free piezo-ceramics, quartz-based piezoelectric materials, the use of lithium niobate and lithium in piezoelectrics, single crystal piezoelectric materials, electroactive polymers (EAP) and piezoelectric composite materials. Part two discusses how to design and fabricate piezo-materials with chapters on piezo-ceramics, single crystal preparation techniques, thin film technologies, aerosol techniques and manufacturing technologies for piezoelectric transducers. The final part of the book looks at applications such as high-power piezoelectric materials and actuators as well as the performance of piezoelectric materials under stress. With its distinguished editor and international team of expert contributors Advanced piezoelectric materials: science and technology is a standard reference for all those researching piezoelectric materials and using them to develop new devices in such areas as microelectronics, optical, sound, structural and biomedical engineering.
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Seite x
... Driving forces for polarization reorientation 18.4 Polarization as an order parameter 18.5 Groups of unit cells, defects, and domains 18.6 The large field behavior of relaxor single crystals 18.7 Calculation of 'domain engineered ...
... Driving forces for polarization reorientation 18.4 Polarization as an order parameter 18.5 Groups of unit cells, defects, and domains 18.6 The large field behavior of relaxor single crystals 18.7 Calculation of 'domain engineered ...
Seite xii
... Drive M/S 67-119 Pasadena, CA 91109 USA E-mail: yosi@jpl.nasa.gov Chapter 12 Leong-Chew Lim Department of Mechanical Engineering National University of Singapore 9 Engineering Drive 1 Block EA, 07–08 Singapore 117576 E-mail: mpelimlc ...
... Drive M/S 67-119 Pasadena, CA 91109 USA E-mail: yosi@jpl.nasa.gov Chapter 12 Leong-Chew Lim Department of Mechanical Engineering National University of Singapore 9 Engineering Drive 1 Block EA, 07–08 Singapore 117576 E-mail: mpelimlc ...
Seite xvii
... drive generates significant heat generation, while the hysteresis of piezoelectrics is enhanced significantly under high mechanical stress. How to escape from these performance degradation and ageing are discussed in Part III ...
... drive generates significant heat generation, while the hysteresis of piezoelectrics is enhanced significantly under high mechanical stress. How to escape from these performance degradation and ageing are discussed in Part III ...
Seite 26
... drive frequency is adjusted to a mechanical resonance frequency of the device, a large resonating strain is generated. This phenomenon can be understood as a strain amplification due to accumulating input energy with time (amplification ...
... drive frequency is adjusted to a mechanical resonance frequency of the device, a large resonating strain is generated. This phenomenon can be understood as a strain amplification due to accumulating input energy with time (amplification ...
Seite 30
... drive field, and p is the density. Substituting a general solution u = u(x)e." + u;(x)e-" into Eq. (1.27), and with the boundary condition X1 = 0 at x = 0 and L (sample length) (due to the mechanically-free condition at the plate end) ...
... drive field, and p is the density. Substituting a general solution u = u(x)e." + u;(x)e-" into Eq. (1.27), and with the boundary condition X1 = 0 at x = 0 and L (sample length) (due to the mechanically-free condition at the plate end) ...
Inhalt
1 | |
87 | |
Part II Preparation methods and applications | 347 |
Part III Application oriented materials development | 559 |
Index | 660 |
Andere Ausgaben - Alle anzeigen
Advanced Piezoelectric Materials: Science and Technology Kenji Uchino Keine Leseprobe verfügbar - 2016 |
Advanced Piezoelectric Materials: Science and Technology Kenji Uchino Keine Leseprobe verfügbar - 2010 |
Häufige Begriffe und Wortgruppen
acoustic actuators Appl applications bulk ceramics characteristics charge coefficient composition constant coupling dependence deposition developed devices dielectric direction displacement domain drive effect elastic electric field electrode electromechanical energy exhibit fabrication factor ferroelectric Figure flux force frequency function grain growth heat higher increasing ions layer lead LiNbO3 loss materials maximum measured mechanical method mode multilayer observed obtained optical orientation particle performance period perovskite phase Phys piezoelectric materials piezoelectric properties plate PMN–PT polarization poled polymer powder prepared produced range reported resonance respectively response rhombohedral sample shown in Fig shows single crystals sintering solid solution sputtered strain stress structure substrate surface Table technique temperature tetragonal thickness thin films transducer transition typical Uchino ultrasonic various vibration voltage wall wave