2017
DOI: 10.1016/j.energy.2016.12.035
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Optimum resistance analysis and experimental verification of nonlinear piezoelectric energy harvesting from human motions

Abstract: The complex dynamic behavior of nonlinear energy harvesters make it difficult to identify the optimum mechanical and electrical parameters for maximum output power, when compared to traditional linear energy harvesting devices. In addition, the random and variable characteristics of low-frequency human motion signals provide additional challenges for enhancing the energy harvesting performance, such as the traditional frequency domain analysis method being inappropriate for optimum resistance selection. This p… Show more

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Cited by 101 publications
(42 citation statements)
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“…Average power, however, increases until it reaches the highest value at the optimum load (13.5 Ω for coil-I and 16.5 Ω for coil-II), before decreasing exponentially. With the average power obtained from RMS voltage [64]; using equation = / , maximum powers are delivered across both coils, with load resistances equal to the coil's internal resistance, which satisfies maximum power transfer [65]. The behavior of the upper and lower electromagnetic generators is identical, but with peak voltages at different base accelerations, as depicted in Figure 8.…”
Section: Resultsmentioning
confidence: 99%
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“…Average power, however, increases until it reaches the highest value at the optimum load (13.5 Ω for coil-I and 16.5 Ω for coil-II), before decreasing exponentially. With the average power obtained from RMS voltage [64]; using equation = / , maximum powers are delivered across both coils, with load resistances equal to the coil's internal resistance, which satisfies maximum power transfer [65]. The behavior of the upper and lower electromagnetic generators is identical, but with peak voltages at different base accelerations, as depicted in Figure 8.…”
Section: Resultsmentioning
confidence: 99%
“…Average power, however, increases until it reaches the highest value at the optimum load (13.5 Ω for coil-I and 16.5 Ω for coil-II), before decreasing exponentially. With the average power obtained from RMS voltage [64]; using equation P =…”
Section: Resultsmentioning
confidence: 99%
“…The nonlinear PZT energy harvester with two external rotatable magnetos designed by Zhou et al [58] was used, and the maximum output power was approximately 23 μW when a participant with a weight of 74 kg and a height of 170 cm was running at a speed of 8 km h À1 . Wang et al [59] then investigated the effect of resistance on the nonlinear energy harvesting efficiency for real human motion. The maximum output power harvested from human motion at the optimum load resistance was obtained as 30.55 μW at a running speed of 7 km h À1 .…”
Section: Pztmentioning
confidence: 99%
“…The relationship between potential well depth and tri-stable energy harvester performance was numerically and experimentally studied in [29]. Cao et al [30] investigates the load resistance of tri-stable energy harvesting from real human motion excitation indicate that there always exists an optimum load resistance to maximize the average output power. Zhou et al [31] derived the nonlinear response characteristics of the asymmetric tri-stable energy harvester to improve energy harvesting performance for more general applications.…”
Section: Introductionmentioning
confidence: 99%