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physics  the  word  work  is  used  in  a  restricted  and  carefully  defined
                  method.
                  External  forces  cause                    the  alteration  of  mechanical  motion.
                                                     A
                  The  elementary  work                       A    of  the  force  F  on  the  small

                                                                    displacement  dr  of  the  point  of
                                                                    force  application  is  the  scalar
                                                                    product of vectors F and dr (Fig.

                                                                    4.3)
                                                                                     
                                                                          A   (F      ) r d                     (5.9)

                                                                    or in scalar form

                                Figure 5.3                                 FA    dS   cos  ,          (5.10)
                                                                    where dS   is elementary distance
                                                                              
                                                                     dS      r d   and     angle between

                  force end displacement
                  (Note  that  we  use  designation  A ,  because    A     is          not  the  total
                  differential of continuous function , i.e. there is no sense to define work in

                  a point  without  displacement)
                            Work is measured in joule (J): 1J = N m. One joule is the work done
                  when a force of one newton acts through a distance of one meter.

                            The work is not produced   if                   when the force vector is
                                                                           2
                  perpendicular to the direction of the velocity .

                          If  force is variable quantity given by function    S            f  (t ) work done
                  by this variable force  can calculated  as definite integral

                                                         S 2
                                                              A      f  (S )ds                                             (5.11)

                                                         S 1
                  i.e  sum of elementary work
                                                              A   f ( S) dS                                              (5.12)

                                                                           Suppose,  force-distance  graph
                                                                   is  arbitrary  curve  as  shown  in

                                                                   fig.5.4
                                                                   Consider so small distance  dS  that
                                                                   force F is constant , then   we can
                                                                   assume    that    elementary  work

                                                                    A   FdS   is  numerically  equal
                                                                   area of     thin strip  with height F
                                                                   and initially  small width dS

                                                                    Obviously , the total work done by
                                  Figure 5.4

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