H. Jung, K. H. Baek, S. Hidaka, D. Song, Se Bin Kim, T. Sung
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引用次数: 2
摘要
为了比较在悬臂梁上施加相同能量时的应变变化效应和冲击效应,提出了两种传递旋转能量给压电材料的能量收集系统模型。对于给定高脉冲、低位移的压电系统,在低阻性负载下产生较高的输出功率。相反,对于一个在低脉冲下具有高位移的系统,在高电阻负载下输出功率更高。在阻抗匹配时,二次冲击系统比低阻负载下的冲击系统产生更高的功率输出。二次冲击系统在频率为60 Hz、低电阻负载为1 k Ω时的响应得到了优化。测量产生的输出功率为124 mW,对应于整个悬臂梁的功率密度为140 mW/cm3,仅压电材料体积的功率密度为342 mW/cm3。对于低阻性负载(1 k Ω)下无二次脉冲的系统,优化频率在20至30 Hz之间,输出功率为22 mW,对应于整个悬臂梁的功率密度为25 mW/cm3,仅压电材料体积的功率密度为60 mW/cm3。
Design and optimization of secondary shock type piezoelectric system
Two models for energy harvesting system imparting rotational energy to piezoelectric materials are presented in order to compare the effects of applying identical amounts of energy to a cantilever beam by strain-changing and shock application. For a piezoelectric system given a high impulse with low displacement, higher power outputs were generated at lower resistive loads. Conversely, for a system with high displacement at a low impulse, power output was higher at high resistive loads. At matched impedance, the secondary shock system generated higher power output than the hitting system did at low resistive load. Optimized response of secondary shock system was obtained at a frequency of 60 Hz with a low resistive load of 1 k Ω. The generated output power was measured 124 mW, which corresponds to power density of 140 mW/cm3 for entire cantilever beam and power density of 342 mW/cm3 for only piezoelectric material volume. For a system without a secondary impulse at low resistive loads (1 k Ω), the optimizing frequency was between 20 and 30 Hz, with an output power of 22 mW, which corresponds to a 25 mW/cm3 power density for entire cantilever beam and power density of 60 mW/ cm3 for only piezoelectric material volume.