MEMS electrostatic energy harvesters with end-stop effects

CP Le, E Halvorsen - Journal of Micromechanics and …, 2012 - iopscience.iop.org
Journal of Micromechanics and Microengineering, 2012iopscience.iop.org
In micro scale energy harvesting devices, end-stops that limit the proof mass motion are
inevitable from reliability concerns and can even be exploited as a functional element to
achieve a broadband response. To investigate how these can be modelled, both
characterization and modelling of vibration energy harvesters with end-stop effects are
presented in this paper. A Hertz contact model of the impact force between the proof mass
and the end-stops is analysed and compared to a linear stiffness model. The resulting …
Abstract
In micro scale energy harvesting devices, end-stops that limit the proof mass motion are inevitable from reliability concerns and can even be exploited as a functional element to achieve a broadband response. To investigate how these can be modelled, both characterization and modelling of vibration energy harvesters with end-stop effects are presented in this paper. A Hertz contact model of the impact force between the proof mass and the end-stops is analysed and compared to a linear stiffness model. The resulting impact force model is then included into a SPICE model of an electrostatic harvester. The performance prediction of the model is validated by comparing simulations and measurements on two different prototypes, one with mechanical quality factor Q m= 5.7 and one with Q m= 203.5. The electromechanical coupling factors of the two devices are respectively k 2= 1.44% and 2.52%. Both devices display the well-known jump phenomenon and output voltage saturation during, respectively, frequency and amplitude sweeps. Under low-level broadband excitations, the high-Q m device performs in agreement with linear theory at an efficiency of 71.8%. For sufficiently high acceleration power spectral density (PSD), it displays a soft limit on the output power and a bandwidth increase, eg a factor 3.7 increase of 3 dB bandwidth when increasing the acceleration PSD from 0.34× 10− 3 to 0.55× 10− 3 g 2 Hz− 1. The end-stop effects reduce the device efficiency down to 35.4% at 1.69× 10− 3 g 2 Hz− 1. A comparison between model and experiment shows that a model with end-stop stiffness extracted from the contact analysis can adequately model the nonlinear end-stop effects both for narrow-and broadband accelerations.
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