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P. 101

F
                                                                 x                                                      (8.1)
                                                             k
                                               where к is known as the force constant.

                                                         Hook's law  states that the deformation of
                                               an  elastic  body  is  directly  proportional  to  the
                                               applied force.

                                                  Whenever  an  elastic  body  is  distorted  by  a
                                               force applied by some agent, the body exerts an
                                               equal  and  opposite  force  on  the  agent.  Besides,

                                               inside the rod there exists the force   F  which is
                                                                                                 el
                                                                                         
                          Figure 8.1           called the elastic force.As F           F , henc
                                                                                           el


                                                              F    kx.                                              (8.2)
                                                        el
                  The last formula represents Hook's law for the elastic force.

                            The relative deformation (or stretching strain) is a measure  of
                  the deformation and is defined as the ratio of the absolute deformation
                    l   to the initial meaning of the value l .
                                                                    0
                                                             l 
                                                                 .                                                  (8.3)
                                                           l 0

                           The term strain is applied to the relative change occurring in the
                  dimensions or shape of a body when it is subjected to a stress. To solve
                  problems of elasticity in a convenient and consistent way, we introduce
                  the new term stress. When we apply a force to distort a body, internal

                  forces  within  the  body  resist  to  distortion.  For  example,  if  we  try  to
                  stretch a bar (fig. 8.1), the material at the left of some plane S exerts a
                  force  to  the  left  on  the  material  at  the  right  of  S.  Since  the  bar  is  in

                  equilibrium, the material at the right of S exerts an equal and opposite
                  force on the material at the left. The material is said to be under stress.
                  For our bar the stress  is the ratio of the internal force F to the area S

                  over which the force is disturbed
                                                             F
                                                              .                                                  (8.4)
                                                             S
                    The relative deformation or stretching strain is proportional to the
                  mechanical stress

                                                              1
                                                                                                                     (8.5)
                                                              E
                     or




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