用于三角翼控制的面外坡莫合金磁致动器

Chang Liu, T. Tsao, Y. Tai, T. Leu, Chih-Ming Ho, Weilong Tang, D. Miu
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引用次数: 60

摘要

这个项目的目标是证明一个微机械执行器的集合可以控制一个宏观对象,只要有一个适当的控制机制存在。在我们的案例中,我们打算使用平面外磁致动器的线性阵列来在无尾三角翼模型上产生滚动力矩,利用三角翼理论中的已知机制,允许微驱动具有放大的宏观效应。三角翼是产生升力的基本构型之一,其气动控制在航空学界具有重要意义[1,2]。当层流气流以一定迎角撞击机翼的两个前缘时(在我们的例子中为30”,图la,b),两个反向旋转的前缘涡流从层流中分离出来,并在机翼顶部传播(图IC)。这两个高动量、低压涡流在机翼两侧产生相同的涡流升力,它们的总和是总升力的- 40%。这两个涡旋的强度和位置取决于它们分离点附近的边界层条件。风洞流速小于20 m/s时边界层厚度约为1 ~ 2mm;随着流速的增加,厚度会减小。两个线性阵列的表面微加工的面外致动器(微襟翼)被放置在机翼底部的两个前缘(图1)。未偏转时,襟翼阵列保持在边界层底部,对流动和涡旋没有影响;然而,当一个阵列向下偏转时,它与边界层相互作用,改变了相应前缘涡的分离点。机翼顶部的展向涡结构变得不平衡,从而产生整体滚动力矩。三角翼的跨度为38厘米,顶角为67度;它在风洞中测试,最高速度为20米/秒。这里选择硅微机械执行器是因为它们具有重量轻和潜在大带宽的附加优势。为了控制这种机翼,微襟翼需要偏转1-2毫米(或匹配边界层厚度),并承受数百pN的大气动载荷。使用磁致动是因为与大多数其他驱动方法相比,它可以产生更强、更长的力[3,4,51]。几种类型的磁性微致动器已经被证明,但没有一种可以很容易地满足当前系统的要求。贝克等。Al .[6]将永磁体片后处理手动附着在微加工板上,并利用面内线圈产生的外磁场驱动永磁体。手动装配不适合我们,因为有大量的交流
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Out-of-plane permalloy magnetic actuators for delta-wing control
INTRODUCTION The goal of this project is t o demonstrate that a collection of micro-machined actuators can control a macro object, provided that a proper controlling mechanism exists. In our case, we intend t o use a linear array of out-of-plane magnetic actuators t o crea te a rolling moment on a tail-less delta-wing model, utilizing a known mechanism in delta-wing theory that allows micro actuation to have an amplified, macro effect. A delta-wing is one of the fundamental configurations for generating lift forces and its aerodynamic control is of great importance t o the aeronautics society [1,2]. When laminar air flow hits the two leading edges of the wing at a certain angle-of-attack (30" in our case, Fig. la,b), two counter-rotating leading-edge vortices are separated from the laminar flow and propagate over the wing's top (Fig. IC). These two high-momentum, low-pressure vortices contribute identical vortex lifting forces on the two sides of the wing, the sum of these being -40 % of the total lifting forces. The strength and position of these two vortices are determined by the boundary layer conditions near their separation points. A boundary layer is roughly 1-2 mm thick at a windtunnel flow speed of less than 20 m/s; the thickness will decrease when the flow speed is increased. Two linear arrays of surface micro-machined out-ofplane actuators (micro-flaps) are placed along two leading edges at the bottom of the wing (Fig. Id) . When un-deflected, flap arrays remain a t the bottom of the boundary layer, having no effect on the flow and vortices; when one array is deflected downward, however, it interacts with the boundary layer and changes the separation point of the corresponding leading-edge vortex. The span-wise vortex structures over the top of the wing become unbalanced, and an overall rolling moment can be created. The delta-wing has a 38-cm span and a 67 O top angle; it is tested in a wind-tunnel with a top speed of 20 m/s. Silicon micro-machined actuators are chosen here because of their added advantages of light weight and potentially large bandwidth. To control this wing, micro-flaps are required to deflect 1-2 mm out-of-plane (or t o match the boundary-layer thickness), and withstand large aerodynamic loading on the order of several hundred pN. Magnetic actuation is used because it is known to generate stronger and longer-range forces [3, 4, 51 compared with most other driving methods. Several types of magnetic micro-actuators have been previously demonstrated, but none can readily fulfill the current system requirements. Beneck et . al. [6] performed post-processing manual attachments of permanent magnet pieces on micromachined plates and actuated the magnet with an external magnetic field generated by in-plane coils. The manual assembly is unsuitable for us because a large number of ac-
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