The Design Considerations Free-Standing

46 electronic applications, usually the AC voltages generated by a micro-generator are converted to usable DC voltage. In this conversion, diodes are normally used for simple full wave direct rectification, which need a minimum forward voltage of 300 mV for each diode to operate. The minimum voltage was able to be reduced to 150 mV by replacing the diodes with active switches in a four stages voltage multiplier circuit as studied by Saha et al [89]. A few tens of micro-watts of electrical power are needed for powering ultra low-power electronics, MEMS sensors and RF communications system. As reported by Torah et al [65], 58 W of power is needed to power an accelerometer based micro-system.

3.4 Theoretical Analysis of Multilayer Structures

Generally, the base excited harmonic motion is modelled as a spring-mass-damper system with the equation of motion [90], 3-1 where y denotes the displacement of the base and x the displacement of the mass from its static equilibrium position. The vibration body is assumed to have a harmonic motion, 3-2 By defining the relative displacement z = x – y . The magnitude of the displacement and acceleration can be derived as, 3-3 3-4 and the phase difference is, 3-5          y x y x b x M      t Y t y  sin                   Y r r r Z 2 2 2 2 2 1                   Y r r Z     2 2 2 2 1 1           2 1 1 2 tan r r   47 where r and ζ is the frequency and damping ratio respectively as, 3-6 3-7

3.4.1 Natural Frequency of a Unimorph Cantilever

From the Bernoulli-Euler equation derivation, a thin cantilever beam with one end clamped and the other end free, the natural transverse vibration can be written as, 3-8 where v i is a coefficient related to boundary conditions, h is the total thickness of the cantilever beam, l b is the length of the cantilever beam, e T is the resultant elastic modulus and  is the density of the structure. However, for a more detail analysis on each layer of the structure, the Bernoulli-Euler equation can be derived in a term related to bending modulus Appendix B as, 3-9 where m w is the mass per unit area. The coefficient, v i of the first three modes are: 3-10 The natural frequency of a multilayer cantilever consists of piezoelectric and electrode can be calculated accurately, if the thicknesses of the piezoelectric layer, h p and electrode layer, h e are known. Assume that the lengths of the piezoelectric and electrode are similar to the beam length, l b and thickness of upper electrode and lower electrode are h e . The mass per unit area of the cantilever for a unimorph as shown in Figure 3-2 is n r    n M c   2  w b i i m D l v f 2 2 2   875104 . 1 1  v 694091 . 4 2  v 854757 . 7 3  v   T b i i e l h v f      2 2 2 2