Abstract:Using a commercial finite-element simulation tool, this work considers some of the electromechanical effects commonly neglected during the analysis of electrostatically actuated fixed–fixed beams. These structures are used in many applications of micromechanical systems, from relay switches and RF resonators to thin film characterization tests, but much of the analytical modelling of the device behaviour disregards the effects of electrostatic field fringing, plane-strain conditions and anchor compliance. It i… Show more
“…The difficulty in designing a device with doubly-supported beam actuators is that analytic or empirical equations relating actuator parameters to tuning ranges have not been reported, and reported tuning ranges of this device type are not consistent, with some reports stating that the [4], others suggesting it is fixed at 40% [5], whilst some suggest a 40% minimum but up to 60% [3].…”
Section: Methods Of Extended Tuningmentioning
confidence: 99%
“…Details of the initial calculations of this relationship can be found in [4], where a minimization of potential energy is used to determine the equilibrium that exists between the mechanical restorative forces and electrical driving force, assuming a deformed beam profile of w(x) = w 1 cos 2 (πx/L). The analysis for this work differs from [4] by the inclusion of a fringing field term and a previously discounted strain stiffening term, and makes no a priori assumption about the travel range of the actuator. The result is a relationship between applied voltage, displacement, beam dimensions, material parameters and zero-voltage electrode gap;…”
We have developed a microspectrometer based on monolithic integration of a Fabry-Pérot optical filter directly with a Hg x Cd 1-x Te-based infrared detector. The tunable Fabry-Pérot is created by a parallel plate MEMS fabricated from two dielectric mirror stacks separated by an initial air gap of 1.4 µm. We have measured linewidths as low as 55 nm, switching times of 40 µs and a tuning range of 380 nm. However this tuning corresponds to only 42% of the desired tuning range, from 1.6-2.5 µm (900 nm). The tuning range is limited by a process called "snap down" which occurs when the MEMS is drive by a voltage source. It can be shown that for a parallel plate snap down occurs at 1/3 the initial gap; complete tuning across the SWIR band requires a physical deflection of at least 60% of the gap. We have developed a modified actuator design which allows 60% tuning of the moveable mirror. Further, the method minimizes actuation-induced stress gradients which can lead to substantial bowing of the mirror and subsequently broad optical linewidths. We will compare the results of our current microspectrometer with our new extended tuning designs. These designs are based on Coventorware and analytical mechanical models combined with optical models for the FabryPérot.
“…The difficulty in designing a device with doubly-supported beam actuators is that analytic or empirical equations relating actuator parameters to tuning ranges have not been reported, and reported tuning ranges of this device type are not consistent, with some reports stating that the [4], others suggesting it is fixed at 40% [5], whilst some suggest a 40% minimum but up to 60% [3].…”
Section: Methods Of Extended Tuningmentioning
confidence: 99%
“…Details of the initial calculations of this relationship can be found in [4], where a minimization of potential energy is used to determine the equilibrium that exists between the mechanical restorative forces and electrical driving force, assuming a deformed beam profile of w(x) = w 1 cos 2 (πx/L). The analysis for this work differs from [4] by the inclusion of a fringing field term and a previously discounted strain stiffening term, and makes no a priori assumption about the travel range of the actuator. The result is a relationship between applied voltage, displacement, beam dimensions, material parameters and zero-voltage electrode gap;…”
We have developed a microspectrometer based on monolithic integration of a Fabry-Pérot optical filter directly with a Hg x Cd 1-x Te-based infrared detector. The tunable Fabry-Pérot is created by a parallel plate MEMS fabricated from two dielectric mirror stacks separated by an initial air gap of 1.4 µm. We have measured linewidths as low as 55 nm, switching times of 40 µs and a tuning range of 380 nm. However this tuning corresponds to only 42% of the desired tuning range, from 1.6-2.5 µm (900 nm). The tuning range is limited by a process called "snap down" which occurs when the MEMS is drive by a voltage source. It can be shown that for a parallel plate snap down occurs at 1/3 the initial gap; complete tuning across the SWIR band requires a physical deflection of at least 60% of the gap. We have developed a modified actuator design which allows 60% tuning of the moveable mirror. Further, the method minimizes actuation-induced stress gradients which can lead to substantial bowing of the mirror and subsequently broad optical linewidths. We will compare the results of our current microspectrometer with our new extended tuning designs. These designs are based on Coventorware and analytical mechanical models combined with optical models for the FabryPérot.
“…However, a number of studies [41,42] report that actual boundary conditions such as a pillar support or a step-up anchor have a significant effect on MEM switches performance and that substantial differences exist between the performances of different types of anchors. This is due to the stress absorption and increased compliance of such non-ideal anchors (Fig.…”
Section: Real Anchors In Fixed-fixed Beam Modelmentioning
The residual stress in a polysilicon beam varies throughout its thickness and will cause a freestanding cantilever to curl upwards or downwards. Measurement of stress gradient for cantilever beam MEMS switches was studied by new procedure and its influences on pull-in phenomena of cantilever beam type were studied. The effect of non ideal anchors of fixed-fixed end type MEM switches were investigated in. The Generalized Differential Quadrature Method was used as a high order approximation to discretize the governing nonlinear differential equation yielding more accurate results with a considerably smaller number of grid points. Further, the results obtained were compared with other existing empirical and theoretical models.
“…This assumption is possible due to the high ratio between length and width of the beam [24]. Electrostatic field fringing effect was neglected due to the high ratio between width and air-gap [25], so that implementation of 3-D models was not necessary.…”
Section: Frequency Shift: Analytical Models and Residual Stress Evalumentioning
The dynamic characterization of a set of gold micro beams by electrostatic excitation in presence of residual stress gradient has been studied experimentally. A method to determine the micro-cantilever residual stress gradient by measuring the deflection and curvature and then identifying the residual stress model by means of frequency shift behaviour is presented. A comparison with different numerical FEM models and experimental results has been carried out, introducing in the model the residual stress of the structures, responsible for an initial upward curvature. Dynamic spectrum data are measured via optical interferometry and experimental frequency shift curves are obtained by increasing the dc voltage applied to the specimens. A good correspondence is pointed out between measures and numerical models so that the residual stress effect can be evaluated for different configurations.
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