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 2 EJ
                               P         min  ,
                                кр        2                         (5.11)
                                        l

          where    – built rod length ratio ( Yasinsky’s ratio).
          The  value  l    l    is  called  erected  length.  This  conventional
                      зв
          hinged prop rod length for which the critical force is critical force
          for a given rod length  l .
          Coefficient   depends on three factors:
              1)  character of ligature that imposed on end and intermediate
                 cross-sections of the rod;
              2)  type  of  rod  load  external  forces  (concentrated  or
                 distributed) and place of application;
              3)  nature of the change of cross section of the rod along its
                 length.
          Consider  the  impact  of  the  first  factor  is  the  influence  of  the
          fixing  rod  conditions.  Formula  (5.11)  can  be  obtained  if  we
          consider  the  equation  of  the  fourth  order  longitudinal  bending
          obtained by double differentiation ratio (5.3):

                                        2
                               4
                             d y     2  d y
                                   k       0.                     (5.12)
                             dx 4     dx 2

          The general integral of this equation is

                       y   A sin kx B  coskx Cx D    .          (5.13)
          Constant  A  ,  ,  , B C D   are  determined  from  the  boundary
          conditions.  For  example,  in  the  second  case,  the  consolidation
          (fig. 5.4, b):

                    y     0 ;  y    0 ;  y    0 ;  y  .      (5.14)
                                                      0
                     x 0     x 0      x l     x l

          Using  these  conditions,  we  obtain  a  system  of  homogeneous
          equations
                       B D    0,
                      
                       Ak C    0,
                                                                   (5.15)
                       A sin kl B  coskl Cl D      0,
                      
                       A sin kl B  coskl   0.
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