Page 119 - The Mechatronics Handbook
P. 119

0066_Frame_C08  Page 10  Wednesday, January 9, 2002  3:48 PM





























                       FIGURE 8.5  First four vibration modes of a cantilever beam.

                       From this transcendental equation the λ i ’s and the circular frequencies ω i  are determined [Butt et al.
                       1995].

                                         ( 2i 1)p         ( 2i 1) p 2  IE  ( 2i 1) p 2  Eh  2
                                                                 2
                                                                                 2
                                                                             –
                                            –
                                                             –
                                    l i L ≅  ----------------------,  w i =  -------------------------- ------- =  -------------------------- ---------  (8.37)
                                            2                4L 2    rA      4L 2    12r
                         Figure 8.5 shows the first four vibrational modes of the cantilever. An important result of the modal
                       analysis is the calculation of the amplitude of thermal vibrations of cantilevers.  As the size of the
                       cantilevers is reduced to nanometer scale, the energy of random thermal excitations becomes comparable
                       with the energy of the individual vibration modes. This effect leads to a thermal noise in nanocantilevers.
                       Using the equipartition theorem [Butt et al. 1995] showed that the root mean square of the amplitude
                       of the tip of such cantilever is

                                                       ------ =
                                                 z ˆ =  kT  0.64 Å  K =  Ewh  3                  (8.38)
                                                  2
                                                                        ------------
                                                            ---------------,
                                                       K       K         4L 2
                       Similar analysis can be performed on vibrations of thin plates such as micromirrors. The free lateral
                       vibrations of such a plate are described by
                                        (
                                     ∂ wx, y, t)  ∂ wx, y, t(  )  ∂ wx, y, t(  )  rh∂ wx, y, t(  )
                                                                               2
                                                               4
                                                   4
                                      4
                                     ----------------------------- + 2----------------------------- + ----------------------------- =  – -----------------------------------  (8.39)
                                                      2
                                        ∂x 4        ∂x ∂y 2      ∂y 4       D     ∂t 2
                         The interested reader is referred to [Timoshenko 1959] for further details on vibrations of plates.
                       8.4 Buckling Analysis
                       Structural instability can occur due to material failure, e.g., plastic flow or fracture, or it can also occur
                       due to large changes in the geometry of the structure (e.g., buckling, wrinkling, or collapse). The latter
                       is the scope of this section. When short columns are subjected to a compressive load, the stress in the
                       cross section is considered uniform. Thus for short columns, failure will occur when the plastic yield
                       stress of the material is reached. In the case of long and slender beams under compression, due to
                       manufacturing imperfections, the applied load or the column will have some eccentricity. As a result the
                       force will develop a bending moment proportional to the eccentricity, resulting in additional lateral
                       deflection. While for small loads the lateral displacement will reach equilibrium, above certain critical


                       ©2002 CRC Press LLC
   114   115   116   117   118   119   120   121   122   123   124