2009
DOI: 10.1108/03321640910940864
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Numerical modeling of 3‐D comb drive electrostatic accelerometers structure (method of levitation force reduction)

Abstract: Purpose -The purpose of this paper is to discuss the numerical modelling of 3D structure of micro-electro-mechanical systems (MEMS) accelerometers. The general idea being discussed is the method of levitation force reduction, as the main source of incorrect mathematical model of comb drive structure. Design/methodology/approach -Accelerometers design is a highly interdisciplinary area and, therefore, different methods and tools have to be exploited. Dynamic accelerometer behaviour modelling has been performed … Show more

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Cited by 9 publications
(9 citation statements)
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“…On the other hand, fostered by the development of new technologies, perspective applications of microactuators, or in general micro-electro-mechanical systems (MEMS), appear more and more in the market. Only in more recent times, however, has the design of MEMS been approached in a systematic way employing automated optimal design [1,8,15]: this trend shortens the gap between academic and industrial research. Following this approach, the design problem is set up as a problem of multivariable non-linear optimization of multiple objective functions subject to a set of constraints.…”
Section: Introductionmentioning
confidence: 99%
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“…On the other hand, fostered by the development of new technologies, perspective applications of microactuators, or in general micro-electro-mechanical systems (MEMS), appear more and more in the market. Only in more recent times, however, has the design of MEMS been approached in a systematic way employing automated optimal design [1,8,15]: this trend shortens the gap between academic and industrial research. Following this approach, the design problem is set up as a problem of multivariable non-linear optimization of multiple objective functions subject to a set of constraints.…”
Section: Introductionmentioning
confidence: 99%
“…Analysing a full multiphysics model at the micro-scale level, encompassing electrostatic and mechanical phenomena, and more generally thermodynamics and fluid dynamics equations, might be computationally unpractical or even prohibitive in terms of cost. So, model complexity should be increased gradually; in this respect, an interesting method based on an object-oriented modelling was recently proposed [8].…”
Section: Introductionmentioning
confidence: 99%
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“…elsewhere on the boundary, with thermal conductivity k = 401 W·m −1 ·K −1 , convection factor h = 5 W·m −2 ·K −1 and T ∞ = 298 K. It can be remarked that the right-hand side of (10) depends on the solution to (8), and-conversely-the lefthand side of (8) depends on the solution to (10) through (9); therefore, a coupled-field boundary-value problem originates. Finally, the Lamé's equation governing the vector displacement u is considered (λ + μ)∇ ∇ · u + μΔu = (3λ + 2μ)β∇T (12) with Lamé's constants λ = 95.149 × 10 9 Pa and μ = 44.776 × 10 9 Pa, corresponding to Young's modulus E = 120 × 10 9 Pa and Poisson's coefficient ν = 0.34, respectively; the thermal expansion coefficient is β = 16.5 × 10 −6 K −1 .…”
Section: Case Study: Electro-thermo-elastic Microactuatormentioning
confidence: 99%
“…1), characterized by (w m , w f , h m , h f ) = (4, 4, 2, 2) (in micrometers), where w and h are width and height of the movable (m) and the fixed ( f ) electrodes, respectively, is assumed as the first case study [8]. The device exhibits 10 + 9 electrodes and the corresponding distribution of electric potential u is shown in Fig.…”
Section: A Device Modelmentioning
confidence: 99%