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 3
... frequency. increasing the frequency (shorter wavelength) leads to the better ... resonance in the piezoelectric material, a 12.5/2 = 6.25 cm thick quartz ... resonance frequency around 40 khz. This sandwich structure is called A ...
... frequency. increasing the frequency (shorter wavelength) leads to the better ... resonance in the piezoelectric material, a 12.5/2 = 6.25 cm thick quartz ... resonance frequency around 40 khz. This sandwich structure is called A ...
Seite 11
... antiresonance frequency almost twice the resonance frequency, i needed to believe the incredibly high k value. The author still remembers that the first submission of our manuscript was rejected because the referee could not T ...
... antiresonance frequency almost twice the resonance frequency, i needed to believe the incredibly high k value. The author still remembers that the first submission of our manuscript was rejected because the referee could not T ...
Seite 25
... resonance spectrum. When the motional admittance Ym is plotted around the resonance frequency w0, the mechanical quality factor QM is defined with respect to the full width [2Dw] at Ym/ 2 as: Q M = w 0 /2Dw 1.18 Also note that QM–1 is ...
... resonance spectrum. When the motional admittance Ym is plotted around the resonance frequency w0, the mechanical quality factor QM is defined with respect to the full width [2Dw] at Ym/ 2 as: Q M = w 0 /2Dw 1.18 Also note that QM–1 is ...
Seite 26
... resonant displacement and strain. The vibration amplitude at an off-resonance frequency (dE·L, L: length of the sample) is amplified by a factor proportional to QM at the resonance frequency. For example, a longitudinally vibrating ...
... resonant displacement and strain. The vibration amplitude at an off-resonance frequency (dE·L, L: length of the sample) is amplified by a factor proportional to QM at the resonance frequency. For example, a longitudinally vibrating ...
Seite 31
... resonance frequency fR is calculated from Eq. (1.32) (by putting wL/2v = p/2), and the fundamental frequency is given by f v L L s R R 11E = /2 = /2 = 1/(2 ) wp r 1.34 on the other hand, the antiresonance state is generated for zero ...
... resonance frequency fR is calculated from Eq. (1.32) (by putting wL/2v = p/2), and the fundamental frequency is given by f v L L s R R 11E = /2 = /2 = 1/(2 ) wp r 1.34 on the other hand, the antiresonance state is generated for zero ...
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