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Touchdown and pull-in voltage behavior of a MEMS device with varying dielectric properties

机译:介电特性变化的MEMS器件的触地电压和吸合电压行为

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摘要

The pull-in voltage instability associated with a simple MEMS device, consisting of a thin dielectric elastic membrane supported above a rigid conducting ground plate, is analyzed. The upper surface of the membrane is coated with a thin conducting film. In a certain asymptotic limit representing a thin device, the mathematical model consists of a nonlinear partial differential equation for the deflection of the thin dielectric membrane. When a voltage V is applied to the conducting film, the dielectric membrane deflects towards the bottom plate. For a slab, a circular cylindrical, and a square domain, numerical results are given for the saddle-node bifurcation value V-*, also referred to as the pull-in voltage, for which there is no steady-state membrane deflection for V > V-*. For V > V-* it is shown numerically that the membrane dynamics are such that the thin dielectric membrane touches the lower plate infinite time. Results are given for both spatially uniform and nonuniform dielectric permittivity profiles in the thin dielectric membrane. By allowing for a spatially nonuniform permittivity pro. le, it is shown that the pull-in voltage instability can be delayed until larger values of V and that greater pull-in distances can be achieved. Analytical bounds are given for the pull-in voltage V-* for two classes of spatially variable permittivity profiles. In particular, a rigorous analytical bound V-1, which depends on the class of permittivity pro. le, is derived that guarantees for the range V > V-1 > V-* that there is no steady-state solution for the membrane deflection and that finite-time touchdown occurs. Numerical results for touchdown behavior, both for V > V-1 and for V-* < V < V-1, together with an asymptotic construction of the touchdown pro. le, are given for both a spatially uniform and a spatially nonuniform permittivity profile.
机译:分析了与简单的MEMS器件相关的引入电压不稳定性,该MEMS器件由支撑在刚性导电接地板上的薄介电弹性膜组成。膜的上表面涂覆有导电薄膜。在代表薄器件的某个渐近极限中,数学模型由用于薄介电膜挠曲的非线性偏微分方程组成。当将电压V施加到导电膜时,介电膜向底板偏转。对于平板,圆柱和正方形区域,给出了鞍节点分叉值V-*(也称为吸合电压)的数值结果,对于该鞍形节点分叉值V- *没有稳态膜偏斜> V- *。对于V> V- *,数值显示膜动力学是这样的:薄电介质膜无限次地接触下板。给出了薄介电膜中空间均匀和不均匀介电常数分布的结果。通过允许在空间上不均匀的介电常数。如图1e所示,拉入电压的不稳定性可以被延迟直到更大的V值并且可以实现更大的拉入距离。给出了两类空间可变介电常数曲线的吸合电压V- *的分析界限。特别是严格的解析界限V-1,取决于介电常数pro的类别。推导le,从而确保在范围V> V-1> V- *时,没有针对膜挠度的稳态解并且发生了有限时间的触地得分。 V> V-1和V- *

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