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                                   Microhinges and Microcantilevers: Lumped-Parameter Modeling and Design

                              108   Chapter Three

                                   y1                  y







                                                      O
                              x       O1    w            x1



                                         x1       x

                                              l
                              Figure 3.3  Microhinge with two end reference frames.

                              terms of compliances by means of local frames, which are translated
                              from the global frame. Thus it becomes important to express compli-
                              ances (and stiffnesses, by consequence) in reference frames that are
                              translated from the original ones. Two types of problems relating to
                              compliance transforms by reference frame translation are solved here
                              in a generic fashion, namely, (1) relating the relevant compliances that
                              are formulated in the two reference frames located at the member’s
                              ends and (2) expressing the compliances in a reference frame that is
                              arbitrarily translated from the member’s end in terms of the regular
                              compliances.


                              3.2.1  Compliances in opposite-end
                              reference frames
                              Figure 3.3 shows a microhinge, which has a variable width. This vari-
                              able  width  can be expressed  in terms of two reference  frames,  yOx
                              (which is located at the thinner end) and y 1 O 1 x 1  (which is located at the
                              opposite  end). Compliances are usually calculated,  particularly for
                              microcantilevers which are thinner toward the free end and thicker to-
                              ward the fixed root, in terms of the yOx frame. The necessity arises,
                              however, to  calculate  compliances with respect to the other frame
                              y 1 O 1 x 1 , and therefore it would be useful to express the compliances in
                              the y 1 O 1 x 1  frame in terms of the compliances in the yOx frame, which
                              are usually available  in the  literature for  a  variety of geometric
                              configurations.
                                As previously shown, three compliances define the bending about the
                              y axis, namely, C l  (the linear direct bending compliance), C r  (the rotary
                              direct bending compliance), and C c  (the cross-bending compliance), all




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