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Goldschmidtboeing F and Woias P, Characterization of different beam shapes for piezoelectric energy harvesting, J. Micromech. Microeng., Vol. 18, pp. 104013 (2008). [3] e-mail: [email protected] [4] Keywords: Energy harvesting, Organic micro-beam, Trapezoid, Comsol simulation [5] [6] 1"mm" 500"µm" 700"µm" 1"mm" 700"µm" 1"mm" Anchor"pad" 150"µm" Top"view" 10"µm" Anchor'Pad' Tip2mass' Anchor'pad' Tip2mass' 500"µm" 1"mm" 500"µm" 1"mm" Ag+epoxy' a)# Tip+mass" SU28' Ag+epoxy' Microcan-lever' 500'µm' b)# SU28' Microcan-lever' 500'µm' Substrate) Cross"sec9on" Figure 1. Dimensions of the designed micro-beams Figure 2. Optical images of the fabricated microbeams 8E-6 0.8 0.7 0.6 0.5 7E-6 Experimental FEM Trapezoidal 6E-6 Rectangle 0.4 0.3 Strain Displacement (µm) With the miniaturization, the systems consume less energy allowing the elaboration of autonomous systems where an energy harvesting device is directly integrated. In the case of vibration energy harvesting, energy sources are characterized by a relatively low acceleration (< 1 g) [1] and a low vibration frequency (< 1kHz) [2]. In accordance with the environmental sources of mechanical vibrations, the majority of vibrational energy harvesters developed to date are based on a mechanical spring-mass system providing a maximum power at the resonance frequency. The main techniques for the processing of organic MEMS are molding or printing using piezoelectric conversion [3,4]. In this work, an original mechano-electrical conversion based on electrostriction is selected, where a strain dependent permittivity induces changes in the capacitance of the electrostrictive material [5]. In case of a vibrating micro-beam, the capacitance variation will depend on the micro-beam’s strain under vibration [6]. In this context, flexible micro-beams based on organic materials are of particular interest for this application, with a trapezoidal shape and a seismic mass [6]. Indeed, finite element simulations using Comsol confirm that trapezoidal micro-beams appear to be the most relevant because of their low resonance frequency and a uniform strain profile under vibration. Based on these simulations, two types of beams with a tip-mass are fabricated and characterized: a rectangular one used as reference, and the optimized trapezoidal one. Their dimensions are specified on Fig. 1. An original method of fabrication combining photolithography and screen-printing has been developed for the fabrication of these micro-structures. Concretely, the micro-beams are patterned by photolithography. The photosensitive epoxy-based resist SU-8 3050 is selected because of its low Young's modulus to achieve large strain under deflection (E = 3GPa). Then the tip-mass is screen-printed using an epoxy paste loaded with Ag (ESL1901-SD). This paste presents a relatively high density (ρ ≈ 4700kg/m3) allowing an important decrease of the resonance frequency as desired. A thick and rigid anchor pad is also screen-printed using this Ag-epoxy based paste. Figure 2 shows examples of successfully fabricated organic beams. The dynamic behavior of the fabricated micro-structures is characterized thanks to a laser doppler vibrometer (Polytec MSA-500). From one hand, the measurements show clearly the influence of the trapezoidal geometry of the structure with a tip-mass, with a low resonance frequency in the range of environmental vibrations (Fig. 3), compared to the rectangular shape. On the other hand, the experimental beam’s strain profiles are also obtained at resonance and compared to the simulated ones. We see in figure 4 that the strain is nearly constant along x for the trapezoidal structure, a clear benefit for an efficient mechano-electrical transduction. A good correlation with finite element simulations is observed, in terms of both frequency values and strain profiles. The calculations of the theoretical harvesting power, based on previous results, show that the power generated by the trapezoidal structure is 2.2 times higher than the one generated by the rectangular shape. This is due to the uniform strain along the surface in the optimized trapezoidal structure. This geometry allows moreover a remarkable decrease in the resonance frequency, making this design clearly suitable for the fabrication of efficient mechanical energy harvesters. Work is now under progress to integrate the electrostrictive material and validate the resulting devices as a new generation of vibration energy harvesters. 500"µm" Université de Bordeaux, Laboratoire IMS, UMR 5218, Talence Cedex, 33405, France 50"µm" [2] H. Nesser , H. Debéda, I. Dufour, C. Ayéla 1"mm" [1] 100"µm" Design and fabrication of trapezoidal organic micro-beams for mechanical energy harvesting from environmental sources 4E-6 2E-6 0.1 1E-6 250 300 350 400 450 Frequency (Hz) 500 Figure 3. Measured and simulated resonance spectra of the rectangular and trapezoidal microbeams. Rectangle 3E-6 0.2 0 Trapezoidal 5E-6 Experimental FEM 0E+0 0 100 200 300 400 500 Profile x (µm) 600 700 Figure 4. Measured and simulated strain profiles along x for the two designs.
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