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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Im Buch
Seite 1
... charges on their surfaces as a consequence of applying mechanical stress. The induced charges are proportional to the ... charge/voltage from quartz and other materials. The root of the word 'piezo' means 'pressure' in Greek; hence the ...
... charges on their surfaces as a consequence of applying mechanical stress. The induced charges are proportional to the ... charge/voltage from quartz and other materials. The root of the word 'piezo' means 'pressure' in Greek; hence the ...
Seite 18
... charge/voltage via the piezoelectric effect in BaTio3. J. Ryu et al. extended the magnetoelectric composite idea into a laminate structure.35 They used Terfenol-D and high g soft PZT layers, which are much superior to the performances ...
... charge/voltage via the piezoelectric effect in BaTio3. J. Ryu et al. extended the magnetoelectric composite idea into a laminate structure.35 They used Terfenol-D and high g soft PZT layers, which are much superior to the performances ...
Seite 30
... charge increment, 0D3/0t, and the total current is given by: - - L - L X l =JCOW s D3 dx =JCow s. (d51X1 + 8.33E,)dy d51 *-(+), + £33E, dx 1.31 Síl Sí1 Using Eq. (1.29), the admittance for the mechanically free sample is calculated to ...
... charge increment, 0D3/0t, and the total current is given by: - - L - L X l =JCOW s D3 dx =JCow s. (d51X1 + 8.33E,)dy d51 *-(+), + £33E, dx 1.31 Síl Sí1 Using Eq. (1.29), the admittance for the mechanically free sample is calculated to ...
Seite 32
... charge up the static capacitance (called damped capacitance). Thus, the antiresonance frequency fA will approach the resonance frequency fR. The general procedure for calculating the electromechanical parameters (k31, d31, sE11, and ...
... charge up the static capacitance (called damped capacitance). Thus, the antiresonance frequency fA will approach the resonance frequency fR. The general procedure for calculating the electromechanical parameters (k31, d31, sE11, and ...
Seite 76
... general problem encountered for these traveling wave type motors. 1.58 Stator structure of Sashida's motor.111 Charge output PZT L Bolt to support the engine 1.61. © Woodhead Publishing Limited, 2010 76 Advanced piezoelectric materials.
... general problem encountered for these traveling wave type motors. 1.58 Stator structure of Sashida's motor.111 Charge output PZT L Bolt to support the engine 1.61. © Woodhead Publishing Limited, 2010 76 Advanced piezoelectric materials.
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