Abstract

Parametric resonance, as a resonant amplification phenomenon, is a superior mechanical amplifier than direct resonance and has already been demonstrated to possess the potential to offer over an order of magnitude higher power output for vibration energy harvesting than the conventional direct excitation. However, unlike directly excited systems, parametric resonance has a minimum threshold amplitude that must be attained prior to its activation. The authors have previously presented the addition of initial spring designs to minimise this threshold, through non-resonant direct amplification of the base excitation that is subsequently fed into the parametric resonator. This paper explores the integration of auto-parametric resonance, as a form of resonant amplification of the base excitation, to further minimise this activation criterion and realise the profitable regions of parametric resonance at even lower input acceleration levels. Numerical and experimental results have demonstrated in excess of an order of magnitude reduction in the initiation threshold amplitude for an auto-parametric resonator (∼0.6 ms−2) as well as several folds lower for a parametric resonator with a non-resonant base amplifier (∼4.0 ms−2), as oppose to a sole parametric resonator without any threshold reduction mechanisms (10's ms−2). Therefore, the superior power performance of parametric resonance over direct resonance has been activated and demonstrated at much lower input levels.

Highlights

  • Vibration energy harvesting (VEH) has gained immense popularity in recent years

  • This paper presents the potential of auto-parametric resonance for vibration energy harvesting

  • The use of an initial spring to amplify the base excitation fed into the parametric resonator has shown nearly an order of magnitude lower initiation threshold amplitude (4.0 ms−2) compared to a plain parametric resonator (>20 ms−2)

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Summary

Introduction

Vibration energy harvesting (VEH) has gained immense popularity in recent years. the absolute attainable power level remains an issue in practical applications. Attempts to improve the power output, based on design and mechanical mechanisms, include: system parameter optimisation [3], array addition around the same frequency range [4], bending of resonant peaks due to Duffing nonlinearities [5,6], jumping of potential wells for bi-stabile [7,8] or multi-stable systems [9], stochastic resonance [10], coupling of multiple transducers such as piezoelectric and electromagnetic transducers [11] as well as frequency up conversion of either linear [12,13] or rotational generators [14,15]. Despite the promising potential of parametric resonance over its direct counterpart, the drive acceleration must attain a dampingdependant initiation threshold amplitude prior to activating it altogether [20,21]

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