(1969)3456134_PIEZOELECTRIC_ENERGY_CONVERTER_F

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Piezoelectric Energy Harvesting using Single Crystal PMN-PT Device 2009

Piezoelectric Energy Harvesting using Single Crystal PMN-PT Device 2009
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(Churchill et al., 2003; Mohammadi et al., 2003; Sodano et al., 2004; Lee et al., 2005; Platt et al., 2005; Sodano et al., 2005). Improvement of materials property, and proper design of device configuration have been investigated to achieve a more efficient electromechanical coupling between the device and the vibration sources (Baker et al., 2005; Cho et al., 2005; Yang et al., 2005). The most commonly used piezoelectric devices for energy harvesting are cantilever beams or plates (Gurav et al., 2004; Ng and Iiao, 2005) because they can be easily implemented and are quite effective for harvesting energy from ambient vibrations using the mechanical amplification mechanism (bending mode). A similar way of improving the efficiency of piezoelectric energy harvesting is to use piezoelectric composite devices called ‘cymbal’ and ‘drum’ (Kim et al., 2004; Wang et al., 2007). Again mechanical amplification is achieved by converting normal force or stress into transverse stress in the piezoelectric devices. To get the maximum energy conversion, a method of tuning the resonant frequency of the harvesting devices to match the frequency of the ambient vibrations was also studied (Cornwell et al., 2005).

英文版原子物理课件

英文版原子物理课件
Shanxi University Atomic Physics
1.1 Introduction
The origins of atomic physics :quantum mechanics Bohr model of the H This introductory chapter surveys some of the early ideas: Spectrum of atomic H and Bohr Theory Einstein's treatment of interaction of atom with light the Zeeman effect Rutherford scattering And so on
Shanxi University Atomic Physics
1.2 Spectrum of atomic hydrogen_3
Wavenumbers may seem rather old-fashioned but they are very useful in atomic physics
the characteristic spectrum for atoms is composed of discrete lines that are the ‘fingerprint' of the element.
In 1888, the Swedish professor J. Rydberg found that the spectral lines in hydrogen obey the following mathematical formula:
Shanxi University Atomic Physics
Lyman series: n’ = 2; 3; 4; … n = 1. Balmer (n = 2), Paschen series: (n = 3), Brackett (n = 4) and Pfund (n = 5)

Mechanical and Aerospace Engineering and

Mechanical and Aerospace Engineering and
Submitted to Journal of Reinforced Plastics and Composites
ANISOTROPIC NONLINEAR PIEZO-ELECTRO-CHEMOTHERMO-VISCOELASTICITY: CHARACTERIZATION, SIMULATIONS AND PROBABILISTIC STRUCTURAL INTEGRITY1 Harry H. Hilton2
Aeronautical and Astronautical Engineering Department National Center for Supercomputing Applications Center for Simulation of Aபைடு நூலகம்vanced Rockets University of Illinois at Urbana-Champaign 104 South Wright Street, MC-236 Urbana, IL 61801-2935 USA
Portions of this paper were presented at the Eleventh International Conference on Composite Materials (ICCM–11). Gold Coast, Australia, July 1997, and at the ONR US - Pacific Rim Workshop on Composite Materials, Honolulu, April 1998. 2 Professor Emeritus of Aeronautical & Astronautical Engineering and Senior Academic Lead, Computational Structural Mechanics, NCSA. Corresponding author. Voice: 217-333-2653 FAX: 217-244-0720 Email: h-hilton @ uiuc,edu 3 H. Fletcher Brown Professor of Mechanical and Aerospace Engineering and the Center for Composite Materials. Voice: 302-831-2338 FAX: 302-831-3619 Email: vinson @ 4 Senior Lecturer in Mechanical and Production Engineering and Director, Electronic Packaging Strategic Research Program. Voice: 65-799-6239 FAX: 65-792-4062 Email: msyi @ .sg 5 Bachelor of Science in Aeronautical & Astronautical Engineering Candidate, UIUC. Now Master of Science in Aeronautics & Astronautics Candidate, Massachusetts Institute of Technology.

基尔斯特 603C 微型压电压力传感器-测量和测试的应用说明书

基尔斯特 603C 微型压电压力传感器-测量和测试的应用说明书

© 2017 ... 2022 Kistler Group, Eulachstraße 22, 8408 Winterthur, Switzerland Tel.+41522241111,****************,. Kistler Group This information corresponds to the current state of knowledge. Kistler reserves the right to make technical changes. Liability for consequential damage resulting Page 1/8PressurePiezoelectric pressure sensorfor Test & Measurement applications603C _003-288e -11.22Type 603C...• • Acceleration compensated • Small sensor size• • • DescriptionDue to their high natural frequencies, piezoelectric pressure sensors can be used for a variety of applications where dynam-ic pressures need to be measured. Another unique character-istic of piezoelectric pressure sensors is their ability to measure small pressure fluctuations that are superimposed on top of high static pressures with exceptional resolution. By contrast, piezoresistive pressure sensors are the right choice when mea-suring static pressure curves.At the core of the all-welded, hermetically sealed 603C series there is a Quartz crystal. The pressure to be measured acts on the sensor’s diaphragm and compresses the Quartz crystal. The compressed crystal produces a charge which is proportional to the pressure. Finally, the charge signal needs to be converted, by a charge amplifier, into a voltage which can then be read.Typical applications• High pressure measurements on hydraulic and pneumatic systems, etc.• Highly dynamic pressure measurements on shock tubes, blast tests, etc.Charge (PE) vs. Voltage (IEPE) outputOne of the most important selection criteria for piezoelectric pressure sensors is the output signal. Two variants of the sen-sor are available, charge output (PE) and voltage output (IEPE resp. Piezotron).Piezoelectric pressure sensors are connected to an electronic circuit which converts the charge generated by the sensor into a proportional voltage. If the electronic circuit is integrated into the sensor housing, it is referred to as an IEPE sensor. If the electronics is an external device (charge amplifier), it is referred to as a PE sensor. Depending on the application, PE or IEPE sensors may be better suitable.IEPE sensors are the ideal solution for the long-term measure-ment of small pressure pulsations (without any static pressure content) or the measurement of dynamic pressure profiles (up to a few tenths of a millisecond only). IEPE sensors will how-ever, due to the built-in electronics, only work at moderate temperatures and come with a fixed measuring range.PE sensors on the other hand are the right solution for the long-term measurement of small pressure pulsations (without any static pressure content), quasi-static or dynamic pressure profiles (up to a few minutes). PE sensors will, due to the ex-ternal charge amplifier, operate at extreme temperatures too and allow for adjustable measuring ranges.The instruction manual and pressure catalogue provides fur-ther details on PE and IEPE sensors, measuring chains as well as applications each technology is best suited for.Page 2/8603C _003-288e -11.22© 2017 ... 2022 Kistler Group, Eulachstraße 22, 8408 Winterthur, Switzerland Tel.+41522241111,****************,. Kistler Group This information corresponds to the current state of knowledge. Kistler reserves the right to make technical changes. Liability for consequential damage resulting Technical data – IEPE sensors 1)Type 603CBA... 00014.0 00035.0 00070.0 00350.0 00690.0 01000.0Output signal V Voltage (IEPE)Pressure range bar 14 35 70 350 690 1 000psi200 500 1 000 5 000 10 000 15 000Maximum pressure bar / psi 1 000 / 15 000Overloadbar / psi 1 100 / 15 950Sensitivity (nom.) mV/bar 357 143 71 14 7 5 mV/psi 25 10 5 1 0.5 0.3Linearity%FSO ≤±1.0Operating temperature range °C / °F -55 ... +120 / -67 ... +248Rise time (10 ... 90%) μs<0.4Natural frequency 2)kHz >500Time constant (nom.) s 2 3Low frequency response -3 dB Hz 0.080 0.053 -5% Hz 0.242 0.161Noise (1 Hz ... 10 kHz) (typ.) μbar rms 32 79 160 810 1 620 2 268Acceleration sensitivity (axial) (typ.) bar/g 0.00014psi/g 0.00200Acceleration sensitivity (radial) (typ.) bar/g 0.0001psi/g 0.0015Supply voltage (by IEPE-Coupler) VDC 22 … 30Supply current (by IEPE-Coupler) mA 2 … 20Output bias voltage (nom.) VDC 11Output voltage FSO V±5Weightgrams 4.0Housing and diaphragm material– 17-4 S.S.1) Indications are valid for 23°C / 73°F (if not specified otherwise)2)Calculated from rise timeRise time (10 ... 90%)μs <0.4Natural frequency2)kHz>500Noise (1 Hz ... 10 kHz)(typ.)μbar rms 126Acceleration sensitivity (axial) (typ.)bar/g psi/g 0.000140.00200Acceleration sensitivity (radial) (typ.)bar/g psi/g 0.00010.0015Insulation resistance Ω≥1013WeightType 603CAA / 603CABgram 4.8 / 2.2Housing and diaphragm material17-4 S.S.Technical data – PE sensors 1)Type 603CA...Output signal pC Charge (PE)Pressure range bar 0 ... 1 000psi 0 ... 15 000Calibrated partial range % 7; 100Overloadbar psi 1 10015 950Sensitivity (nom.)pC/bar pC/psi -5.0-0.35Linearity (typ.) (max.)%FSO %FSO ≤±0.4≤±1.0Operating temperature range°C °F-196 ... +200-321 ... +392Page 3/8603C _003-288e -11.22© 2017 ... 2022 Kistler Group, Eulachstraße 22, 8408 Winterthur, Switzerland Tel.+41522241111,****************,. Kistler Group This information corresponds to the current state of knowledge. Kistler reserves the right to make technical changes. Liability for consequential damage resulting Mounting (sensors with standard housing)Sensors with charge output (PE) and voltage output (IEPE) are available with standard housing. Sensors with a standard hou-sing can either be installed directly or with an adapter.Direct MountingWhen the mounting location space is restricted, the sensor can be located in an appropriately dimensioned mounting bore, and then held in place with a floating clamp nut. Please note that for a reliable and accurate pressure measurement a precise machining of the mounting hole with special reamers and taps is required. F or details on mounting hole fabrication please check the manual.Adapter MountingFitting sensors into a mounting adapter greatly simplifies the installation process (when space and wall thickness are not a premium). Use of a Kistler mounting adapter will eliminate the need to provide a precise mounting configuration and allow the installer to provide only a threaded hole of the size and depth required for the adapter selected. Special reamers or taps are not required when using an adapter. For details on mounting thread fabrication please check the manual. All sen-sors and adapters are available for download as 3D CAD files from Kistler’s webpage.Cable with 10-32 connector(e.g. 1631C)Sensor with standard housing(e.g. 603CAA, 603CBAxxxxx.x)(e.g. 1131Bxx.xx)Adapter seal (e.g. 1113C0C)Direct Mounting Type 6503CxA Adapter Type 6503CxD Adapter Type 6507BxA Adapter Type 6503C3A Adapter Type 6509B Adapter • Flush mounting • C omplex drilling with special tool • M in. structuralinfluences on pressure measurement (mech-anical decoupling)• I deal for close matrix alignment of sensors• M10 and 3/8-24 UNF • S tainless steel (1.4542)• Flush mounting • M ax. Pressure1 000 bar (14 500 psi)• M10 and 3/8-24 UNF • Ground Isolating • P EEK GF30(glass fiber reinforced high performance plastic)• M ax. Pressure 100 bar (1 450 psi)• M ax. temperature 100°C (212°F)• M3 and 5-40 UNC • S tainless steel (1.4542)• Recessed mounting • M ax. Pressure 300 bar (4 350 psi)• 1/8-27 NPTF • S tainless steel (1.4542)• Almost flush mounting • M ax. Pressure1 000 bar (14 500 psi)• M14x1.25• Water Cooling • S tainless steel (1.4542)• M ax. Pressure 300 bar (4 350 psi)•Max. temperature400°C (752°F)Page 4/8603C _003-288e -11.22© 2017 ... 2022 Kistler Group, Eulachstraße 22, 8408 Winterthur, Switzerland Tel.+41522241111,****************,. Kistler Group This information corresponds to the current state of knowledge. Kistler reserves the right to make technical changes. Liability for consequential damage resulting Mounting (sensors with short housing)Sensors with charge output (PE) are also available with short housing. For the mounting of these sensors a connector ex-tender of Type 6482A is required. This mounting form is mostly only used where mechanical structures cannot be weakened.Connector extenders are made to order and are therefore not stock items (unlike floating clamp nuts of Type 6423B). Cus-tomers can choose between three different connectors, two different threads and a variable length (see ordering key).Please note that for a reliable and accurate pressure meas-urement a precise machining of the mounting hole with special reamers and taps is required (same as for direct mounting, see previous datasheet page). For details on mounting hole fabri-cation please check the manual. All connector extenders are available for download as 3D CAD files from Kistler’s webpage.10-32 connector BNC connectorTNC connectorSmall coaxial 10-32 connectors are widely used in the sensor in-dustry and therefore comes with a wide range of high impe-dance cable options. The small size further allows for sealing the sensor connector with thermo shrink slee-ves. Attention needs to be payed to clean-liness of these small connectors.The BNC connector (bayonet lock) is much bigger and therefor sturdier and less sensitive to con-taminations than the widely used 10-32 connector. It’s large dimensions and big mass as well the dif-ficulty to be sealed might however be a criterion for exclu-sion in some applica-tions.The TNC connector (thread lock) has about the same size, and offers the same advantages and disadvantages, as the BNC connector. Thanks to the thread lock a good sealing against exterior influ-ences is achieved and is therefore the pre-ferred choice when conducting tests outside a laboratoryenvironment.Ordering key (connector extender)Connector type BNC 0TNC 110-322Mounting thread M7x0.7505/16-24 UNF 1Length (in mm)10-1013 (200)-SP O rdering example Type6482A with BNC, M7 thread, 10 mm length 6482A00-106482A with TNC, M7 thread, 15 mm length 6482A10-SP156482A with 10-32, UNF thread, 125 mm length 6482A21-SP125Cable with 10-32, BNC orTNC connectorConnector Extender(6482Axxx)(603CAB)Sensor seal Max. operating temperaturePage 5/8603C _003-288e -11.22© 2017 ... 2022 Kistler Group, Eulachstraße 22, 8408 Winterthur, Switzerland Tel.+41522241111,****************,. Kistler Group This information corresponds to the current state of knowledge. Kistler reserves the right to make technical changes. Liability for consequential damage resulting Waterproof solution (IP68)F or pressure sensors subject to water splashes or even used under water the IP68 rated cable Type 1983A shall be used. The Type 1983A cable, made of FKM rubber, comes with a vulcanized 10-32 connector and is only compatible to pressure sensors with a standard housing.The Type 1983A cable can be screwed like any other standard cable, or optionally even be welded, to the pressure sensor. Welding, instead of screwing, the cable connector to the sen-sor offers protection against detachment of the cable in case of strong vibrations. Requirements to weld the connector to the sensor need to be stated at the time of order (see below ordering keys).Both, screwed and welded, solutions have successfully been qualified for IP68 rating in water with pressures ranging from vacuum to 16 bar.Ordering key (PE sensor with welded 1983A cable)Floating clamp nut Type 6423B00A 6423B11BCable Type1983AD (with BNC pos. connector)A 1983AC (with 10-32 pos. int. connector)BCable length (in m)1 m (for 1983AC cable only)1,02 m (for 1983AC and 1983AD cable)2,03 m (for 1983AC cable only)3,05 m (for 1983AD cable only)5,0Customized cable length (0.1 to 30.0 m)SPOrdering exampleType603CAA with 6423B00 and 2 m 1983AD cable 603CAA-WAA2,0603CAA with 6423B00 and 6 m 1983AD cable 603CAA-WAASP6,0603CAA with 6423B11 and 0.5 m 1983AC cable603CAA-WBBSP0,5Ordering key (IEPE sensor with welded 1983A cable)Ordering exampleType603CB00014.0 with 6423B00 and 2 m 603CBA-W00014.0-AA2,0 1983AD cable603CB00070.0 with 6423B00 and 6 m 603CBA-W00070.0-AASP6,0 1983AD cable603CB00350.0 with 6423B11 and 7 m 603CBA-W00350.0-BBSP7,01983AC cableCable with 10-32 connector (e.g. 1983AC, 1983AD)Floating clamp nut (e.g. 6423B00)Sensor with standard housing (e.g. 603CAA, 603CBAxxxxx.x)Sensor seal (e.g. 1131Bxx.xx)Sensor with welded cable and attached floating clamp nut (e.g. 603CAA-W, 603CAB-W)Page 6/8603C _003-288e -11.22© 2017 ... 2022 Kistler Group, Eulachstraße 22, 8408 Winterthur, Switzerland Tel.+41522241111,****************,. Kistler Group This information corresponds to the current state of knowledge. Kistler reserves the right to make technical changes. Liability for consequential damage resulting SensorsType 603CAA(dimensions in mm [inch])Type 603CAB(dimensions in mm [inch])Type 603CBAxxxxx.x (dimensions in mm [inch])Note: Mounting holes, tightening torques and more can be found in the instruction manual.3D CAD data can be downloaded free of charge from/cad-catalogSensor Typ 603CAAType 1131BB0.20(dimensions in mm [inch])Type 1131BC1.15(dimensions in mm [inch])Seals (Sensors)Floating clamp nutType 6423B00(dimensions in mm)HEX8HEX 7,1 /9/32"Type 6423B11(dimensions in inch)Page 7/8603C _003-288e -11.22© 2017 ... 2022 Kistler Group, Eulachstraße 22, 8408 Winterthur, Switzerland Tel.+41522241111,****************,. Kistler Group This information corresponds to the current state of knowledge. Kistler reserves the right to make technical changes. Liability for consequential damage resulting Note: Mounting holes, tightening torques and more can be found in the instruction manual.3D CAD data can be downloaded free of charge from/cad-catalogAdapterType 6503C0A(dimensions in mm)Type 6503C0D (dimensions in mm)Type 6507B0A(dimensions in mm)Type 6503C1A(dimensions in inch)Type 6503C1D(dimensions in inch)Type 6507B1A(dimensions in inch)Type 6503C3A(dimensions in inch)Type 6509B(dimensions in mm)Type 6501B0A(dimensions in mm)Page 8/8603C _003-288e -11.22© 2017 ... 2022 Kistler Group, Eulachstraße 22, 8408 Winterthur, Switzerland Tel.+41522241111,****************,. Kistler Group This information corresponds to the current state of knowledge. Kistler reserves the right to make technical changes. Liability for consequential damage resulting Accessories (included)Type/Art.-No.• Sensor seal copper (5 pcs.) 1131BA0.15Accessories (optional) Type/Art.-No.• Sensor seal copper (100 pcs) 1131BA0.15• Sensor seal nickel (100 pcs) 1131BB0.20• Floating clamp nut M7x0.75 6423B00• Floating clamp nut 5/16-24-UNF 6423B11• Adapter M10x11)6503C0A • Adapter seal (S.S. / 25 pcs) for 6503C0A 1113C0B • Adapter seal (Cu / 25 pcs) for 6503C0A 1113C0C • Adapter 3/8-24-UNF 1) 6503C1A • Adapter seal (S.S. / 25 pcs) for 6503C1A 1113C1B • Adapter seal (Cu / 25 pcs) for 6503C1A 1113C1C • Adapter M3x0.51)6507B0A • Adapter 5-40 UNC 1)6507B1A• Adapter seal for 6507BxA 1117B0C• Lubrication grease (Adapter) 1063• Adapter M10x1 (ground isolated) 6503C0D • Adapter 3/8-24 UNF (ground isolated) 6503C1D• Adapter 1/8-27 NPTF 6503C3A • Adapter M14x1.25 6501B0A• Adapter seal (S.S / 1pc) for 6501B0A 1100A11• Adapter M14x1.25 (water cooling) 6509B • Adapter seal (Cu / 1pc) for 6509B 1111• Temperature conditioning system 2621G • Connector extender (configurable product) 6482A • Extraction tool 1311• Dummy sensor (standard housing) 6487AA • Dummy sensor (short housing) 6487AB • Step reamer (SC H7 Ø6.35/Ø5.58) 1331C • Thread cutter M7x0.75 1351A0• Thread cutter 5/16-24 UNF 1351A1• RTV tool 1300A195• RTV seal (S.S. / 25 pcs) 1131BC1.15• RTV 1007A1)All of the adapters are delivered with 1 pc. of each adapter seal type and 1 pc. lubrication grease Type 1063 (except adapters Type 6503C0D, 6503C1D, 6503C3A).Ordering key (sensor)Output signal Charge (PE)A Voltage (IEPE)B HousingStandard housing (PE and IEPE)A Short housing (only PE)B Pressure range (only IEPE)14 bar / 200 psi 00014.035 bar / 500 psi 00035.070 bar / 1 000 psi 00070.0350 bar / 5 000 psi 00350.0690 bar / 10 000 psi 00690.01000 bar / 15 000 psi 01000.0O rderingexample Type PE sensor with standard housing 603CAAPE sensor with short housing 603CABIEPE sensor (350 bar / 5 000 psi) 603CBA00350.0。

python能量谱代码

python能量谱代码

python能量谱代码计算信号的能量谱是一种常见的信号处理任务,可以使用Python 中的库来实现。

以下是一个使用Python 中的NumPy 和Matplotlib 库计算和绘制信号能量谱的简单示例:```pythonimport numpy as npimport matplotlib.pyplot as pltdef calculate_energy_spectrum(signal, sampling_rate):"""计算信号的能量谱参数:- signal: 输入信号- sampling_rate: 信号的采样率返回:- frequencies: 能量谱的频率- energy_spectrum: 信号的能量谱"""n = len(signal)frequencies = np.fft.fftfreq(n, 1/sampling_rate)energy_spectrum = np.abs(np.fft.fft(signal))**2 / nreturn frequencies, energy_spectrum# 生成一个示例信号,比如正弦波sampling_rate = 1000 # 采样率t = np.arange(0, 1, 1/sampling_rate) # 1秒钟的信号frequency = 5 # 5 Hz的正弦波signal = np.sin(2 * np.pi * frequency * t)# 计算能量谱frequencies, energy_spectrum = calculate_energy_spectrum(signal, sampling_rate)# 绘制信号及其能量谱plt.figure(figsize=(10, 6))plt.subplot(2, 1, 1)plt.plot(t, signal)plt.title('原始信号')plt.xlabel('时间(秒)')plt.ylabel('幅度')plt.subplot(2, 1, 2)plt.plot(frequencies, energy_spectrum)plt.title('能量谱')plt.xlabel('频率(Hz)')plt.ylabel('能量')plt.tight_layout()plt.show()```这段代码使用NumPy 中的FFT 函数来计算信号的频谱,然后计算能量谱。

piezoelectric effect 原理英文

piezoelectric effect 原理英文

piezoelectric effect 原理英文Piezoelectric Effect: Understanding the Principle Behind a Key TechnologyIntroductionThe piezoelectric effect is a fascinating phenomenon that has found wide-ranging applications in various fields, from sensors and actuators to medical devices and consumer electronics. This effect occurs in certain materials that exhibit a unique property – the generation of an electric charge in response to mechanical stress or the opposite effect, the generation of mechanical strain in response to an applied electric field. Understanding the principle behind the piezoelectric effect is crucial for harnessing its potential and developing innovative technologies. In this article, we delve into the fundamentals of the piezoelectric effect and explore its implications in modern science and industry.Historical BackgroundThe piezoelectric effect was first discovered by French physicists Jacques and Pierre Curie in 1880. They observed that certain crystals, such as quartz and Rochelle salt, produced electric charges when subjected to mechanical pressure. Thisphenomenon sparked a wave of research into the properties of piezoelectric materials and laid the foundation for the development of piezoelectric technology. Over the years, scientists have identified a wide range of materials that exhibit piezoelectric behavior, including ceramics, polymers, and composites.Principle of the Piezoelectric EffectAt the heart of the piezoelectric effect lies the concept of polarization, where the positive and negative charges within a material become displaced in response to an external stimulus. In piezoelectric materials, such as quartz or lead zirconate titanate (PZT), the crystal structure is asymmetric, with positive and negative charges distributed unevenly along certain axes. When a mechanical force is applied to the material, the crystal lattice deforms, causing the charges to shift and creating an electric field. This leads to the generation of an electric charge on the surface of the material, known as the direct piezoelectric effect.Conversely, when an electric field is applied to a piezoelectric material, the charges within the crystal lattice rearrange, resulting in a change in shape or mechanical strain, known as the inverse piezoelectric effect. This bidirectionalrelationship between mechanical stress and electric field forms the basis of piezoelectric transduction, where energy is converted between mechanical and electrical forms.Applications of the Piezoelectric EffectThe piezoelectric effect has revolutionized a wide range of industries, enabling the development of innovative devices and technologies. Some of the key applications of piezoelectric materials include:1. Sensors and Actuators: Piezoelectric sensors are widely used in industrial applications, such as measuring pressure, force, and acceleration. Likewise, piezoelectric actuators are employed in precision positioning systems, ultrasonic motors, and vibration control devices.2. Energy Harvesting: Piezoelectric materials can convert mechanical vibrations or ambient vibrations into electrical energy, making them ideal for energy harvesting applications in wearable devices, wireless sensors, and self-powered systems.3. Medical Devices: Piezoelectric transducers are used in medical imaging technologies, such as ultrasound andnon-destructive testing. Piezoelectric bone conduction devicesand piezoelectric actuators are also used in hearing aids and implantable medical devices.4. Consumer Electronics: Piezoelectric materials are found ina variety of consumer electronics products, including piezoelectric buzzers, acoustic sensors, and haptic feedback devices in smartphones and tablets.Future Prospects and ChallengesAs the demand for miniaturized, energy-efficient devices continues to grow, the piezoelectric effect holds great promise for future technological advancements. Researchers are exploring new materials, such as flexible and bio-compatible polymers, for unique applications in wearable electronics, biomedical implants, and energy-efficient devices. However, there are still challenges to overcome, such as improving the performance and durability of piezoelectric materials, optimizing energy conversion efficiency, and reducing costs for large-scale production.ConclusionThe piezoelectric effect is a powerful phenomenon that has transformed the way we interact with technology and the world around us. By understanding the principles behind this effectand exploring its diverse applications, we can unlock new opportunities for innovation and create a sustainable future. As we continue to push the boundaries of material science and engineering, the piezoelectric effect will undoubtedly play a key role in shaping the technologies of tomorrow.。

Piezoelectric energy harvesting device optimization by synchronous electric charge extraction

Piezoelectric energy harvesting device optimization by synchronous electric charge extraction

of this, the design of vibration-powered electronic devices is made possible by the recent development of ultralow-power integrated circuits, able for instance, to feed sensors, to carry out fast signal processing, and to radio-transmit data (Elvin et al., 2001; Ayers et al., 2003; Roundy et al., 2003a, b; Amirtharajah and Chandrakasan, 2004).
Various techniques for the construction of such piezoelectric microgenerators have been investigated. Mechanical parts constitute an important aspect in design, but previous studies have shown that electrical energy conditioning system has also a determinant effect on the energy conversion effectiveness (Ottman et al., 2002, 2003).
Vibrations take place in most of the structures, but their potential energy often remains very low. In spite

Piezoelectric energy harvesting from transverse galloping of bluff bodies

Piezoelectric energy harvesting from transverse galloping of bluff bodies
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Piezoelectric energy harvesting from transverse galloping of bluff bodies
This content has been downloaded from IOPscience. Please scroll down to see the full text. 2013 Smart Mater. Struct. 22 015014 (/0964-1726/22/1/015014) View the table of contents for this issue, or go to the journal homepage for more
0964-1726/13/015014+11$33.00 1
several studies [18–24] have focused on the conversion of aeroelastic vibrations of wings to electrical power. Sirohi and Mahadik [25] proposed harvesting energy from transverse galloping of a prismatic structure that has an equilateral triangle section. Surface-bonded piezoelectric sheets attached to two beams connected to the structure were used to generate power. Their device generated more than 50 mW at a wind speed of 11.6 miles per hour; a power level that is sufficient to supply most of the commercially available wireless sensors. In this work, we consider the exploitation of transverse galloping of a bluff body with different cross-section geometries to harvest energy using a piezoelectric transducer. Transverse galloping of an elastic bluff body occurs when the wind speed exceeds a critical value and consequently the body starts to oscillate [26]. Many studies [27–36] have investigated the effects of various parameters on the galloping of different structures. These studies have also investigated the influence of the geometry of the cross-section
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3,456,134
Patented July 15, 1969
2
small series capacity Co limits the conversion efficiency and hence, the output power eo to a very small value. An attempt to overcome these difficulties is made both by the construction shown in FIG. 2 and the circuit modification of FIG. 4. Referring to FIG. 2, the structure of the implant comprises a container 15 made of metal, glass, or plastic but of such metal, glass, or plastic which would not be affected by the surrounding body elements in which the implant takes place. Inside this sealed container 15 there is found a crystal 10, in the form of a cantilever beam, anchored at 17 to and supported by the container 15. Attached to the free end of the crystal cantilever beam 10 is a weight 18. The relative size of container 15, cantilever beam crystal /10, weight 18, and the placement of the cantilever beam 10 in container 15 should be such that the cantilever beam 10 is free to swing its fullest extent S' without contacting the inner sides of container 15. This amplitude of swing S' is determined by the length and material of cantilever beam 10, the size of weight 18, and in addition, by the amount of movement due to body motion through which container 15 is moved. The body motion which moves container 15 with the end loaded cantilever beam 10 causes the cantilever beam 10 to resonate at a suitable frequency corresponding to the mechanical driving source or body. As the container base is moved periodically, the crystal cantilever beam 10 is caused to vibrate at its natural frequency with varying amplitude. It, thus, generates trains of electrical voltage as shown in FIG. 3. In this figure, the amplitude S is shown in registration for comparison with the voltage Eo generated by the cantilever beam crystal !10. In order to utilize the crystal in the structure described and to fully utilize the capacitance of the crystal, a voltage doubler circuit, as illustrated in FIG. 4, was developed for combination !with the crystal. This circuit uses diodes for rectification, an external capacitor Cand the crystal capacitor Co for voltage doubler; the crystal 10 may be of a type known as a Clevite PZT-5H crystal. With such an energy converter, when the device is driven at a mechanical pulse rate of 80 pulses per minute and with a motion similar to the heart motion of a dog, upon which it was tested, the maximum output is 4.0 volts at 105 ohms load, or 160 microwatts. This power is sufficient to drive a pacemaker and some of the existing implant telemetry systems. In tests, the performance of this new operation mode has been shown to be more desirable than the conventional mode. In addition, this design has eliminated the package problem wherein the implant is placed in the body, while increasing the output of the converter over the original output of prior art converters. It will be obvious to those skilled in the art that various changes may be made without departing from the scope of the invention and the invention is not to be considered limited to what is shown in the drawings and described in the specification. What is claimed is: 1. A converter of body motion to electrical energy for use with electronic implants in the body comprising: a closed container of a material not affected by body fluids, a piezoelectric crystal in the form of a cantilevered beam within said container and extending inwardly from a wall of said container with one end anchored in said container wall and the opposite end free to move, a weight mounted on said free end of said crystal cantilevered beam, and means connecting said crystal to the electronic implants in the body.
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INVENTOR
WEN
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ATTORNEY
United States Patent 0 ce
1
3,456,134 PIEZOELECTRIC ENERGY CONVERTER FOR . ELECTRONIC IMPLANTS Wen H. Ko, Palo Alto, Calif., assignor to the United States of America as represented by the Secretary of 5 Health, Education, and Welfare . Filed Oct. 5, 1967, Ser. No. 673,115 Int. Cl. HOlv 7102 U.S. CI. 310-8.5 3 Claims 10 ABSTRACT OF THE DISCLOSURE A piezoelectric converter for electronic implants for convertin
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