Beneficial nonlinear dynamic regimes for energy harvesting

with L. Bergman, S. Chiacchiari, M. Mc Farland, A. Vakakis.

The demand for small-scale, wireless electronic devices (e.g., micro-sensors and actuators, transmitters, controllers) that operate with high efficiency and minimal power consumption has spurred research and development of sustainable, longlife and low-maintenance power sources. Systems that convert available energy from the environment (e.g., kinetic, wind, solar, thermal, chemical) into electrical energy can be used as direct power sources or to charge storage devices such as batteries and supercapacitors. At small scale, these harvesting systems may eventually replace on-board batteries that require periodic replacement, a particularly attractive alternative for devices that are inaccessible. Low power applications such as wireless smart sensors represent a growing market, particularly in the health sciences and in monitoring the state of critical infrastructure. Power consumption of these devices generally ranges from tens of micro- to hundreds of milli-W. Since vibration is pervasive in the environment, kinetic energy generators are an attractive alternative for powering autonomous, small-scale systems, and several recent studies have focused on this alternative. Activities such as walking on a pedestrian bridge and a train wheel traversing a track represent examples of pulse-like excitations applied to flexible structures, capable of producing vibrations suitable for energy harvesting.

A vibration-based electromagnetic bistable energy harvesting system (BNEH) coupled to a directly excited, weakly damped linear primary system (LO) is studied in [1]. The coupled equations governing the dynamics of the two-degree-of-freedom system are used to compute two energy harvesting measures: energy harvesting efficiency and total harvested energy. Mass ratio and damping in the coupling, which is provided by both the mechanical inherent damping of the BNEH and the electromechanical coupling, are found to be the key parameters governing the energy harvesting performance. Under a single impulse, by decreasing the energy level, three different mechanisms are exploited to attain a fast energy capture and harvesting: periodic cross-well oscillations, a regime of aperiodic cross- and in-well oscillations, and fully in-well oscillations. By comparing the energy harvesting capabilities of the system with and without the negative linear coupling stiffness, a significant enhancement in terms of both energy harvesting efficiency and total energy harvested due to the addition of the bistability is observed. For the considered set of parameters, the nonlinear device is found to be able to absorb and harvest above 40 mJ at the highest energy level, 90% of which is harvested in the first 0.4 s, whereas energy of the order of mJ can still be harvested at very low input energy regimes. Energy harvesting capability greater than 400 mJ per applied impulse is achievable for high-energy inputs and for optimal impulse periods.

In order to validate the numerical predictions presented in [1], an experimental investigation of an electromagnetic energy harvester coupled through a bistable, essentially nonlinear element to a weakly damped primary linear oscillator (LO) is reported in [2]. The combined electromagnetic harvester and bistable coupling element represent the so called BNEH. The LO is directly subjected to low energy impulsive excitations. The coupling is represented by a prebuckled clamped-clamped beam constrained to exhibit transverse motion in the direction of its weak bending axis, resulting in a stiffness characteristic at its connection to the harvester containing both negative linear and cubic terms. A computational model representing the experimental apparatus is developed, and the performance of the system is studied experimentally and computationally under both isolated and repeated impulses. A model is also developed for the monostable counterpart, and comparisons are made demonstrating the superior performance of the bistable configuration.

[1] Chiacchiari S., Romeo F., Mc Farland M., Bergman L., Vakakis A.I., Vibration energy harvesting from impulsive excitations via a bistable nonlinear attachment, Int. J. of Nonlinear Mechanics, 94, 84-97, 2017.

[2] Chiacchiari S., Romeo F., Mc Farland M., Bergman L., Vakakis A.I., Vibration energy harvesting from impulsive excitations via a bistable nonlinear attachment – Experimental Study, Mechanical Systems and Signal Processing, in press.

Model of the two coupled oscillators.
Contour plots of the efficiency measure η% resulting from the application of a single impulse to the primary linear system, harvested up to time τ = 60, as function of the inherent viscous damping of the coupling ζ and the amplitude of the impulse (a) monostable configuration; (b) bistable configuration. Regions I, II and III refer to different dynamic regimes.
Sketch of the coupled harvesting device and experimental apparatus (UIUC) of the energy harvesting system.
Dynamics of the two-DOF system for the high input energy level (I0=0.25 m/s): time histories of the LO velocity (a) and BNEH relative velocity (b); (d) and (e) corresponding wavelet transform spectra; (c) measured voltage; (f) total energy harvested by the BNEH. Blue lines refer to the corresponding numerical simulation.
Comparison of the total energy harvested by single impulse by different types of Energy Harvesters (EH): (Black) — current bistable EH, - - - current monostable EH; (Red) — optimal bistable EH, - - - optimal cubic EH; (Blue) linear EH with optimal linear stiffness coefficient.