Abstract: A micromechanical micromotion amplifier has an integrated structure formed primarily of silicon and comprises a plurality of long slender flexible beams which are released from a silicon substrate for movement with respect to fixed points of reference upon the substrate. By arranging these beams in cooperating perpendicular pairs as micromotion amplifier stages, an input axial force/movement applied to a moveable free end of a first beam generates a transverse motion or buckling movement which in turn, translates or induces buckling movement in the connected second beam. The resultant output buckling of the second beam is an order of magnitude greater than the initial movement applied as an input to the first beam. Thus, beam pairs can be arranged as micromotion amplifier stages to amplify minute amounts of movement. Beam pairs or stages can also be cascaded to form integrated devices capable of producing greatly increased measurable effects in response to minute amounts of input.

Abstract: A micromechanical micromotion amplifier has an integrated structure formed primarily of silicon and comprises a plurality of long slender flexible beams which are connected in a predetermined manner. The beams are released from a silicon substrate for movement with respect to fixed points of reference upon the substrate. Each beam thereby has a fixed end and a relatively moveable free end. Compressive axial force induced by axial movement, applied to the moveable end of a beam, will cause that beam to deform or buckle. Buckling occurs transversely in-plane due to a high aspect ratio profile of each beam. The amount of lateral or transverse movement of a beam due to buckling is relatively large in relation to the applied axial force or axial movement which causes it. By arranging these beams in cooperating perpendicular pairs as micromotion amplifier stages, an input axial force/movement applied to the moveable free end of a first beam generates a transverse motion or buckling movement of that beam.