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 VD n( )  2
                               J n( )   Jo   m   
                                            5 
                                                 1 
                                            2           .
                                           1
                               To
                                    J 0   
                Also  draw  the  diagram   J     J  зв   n   in  MathCAD  app
                                           2 зв
           (see fig. 1.6).

            1.8 Determination of equivalent moment of restriction forces
                   during one cycle of mechanism’s steady motion

                Magnitude  of  equivalent  moment  of  restriction  forces  is
           determined for every position of an input link by the next formula
                     F 0  D              F                     F  
                                                                      D
                                               D
              о
                                                            0
            М зв   n       n   cos F 0   D   0    n   cos 180     0  1    n  .
                                                1
                         1
                Useful effort  F 0   1150 N acts during working motion of the
           mechanism, i.e. at motion of the slider to up. If the slider moves
           down –  F 0    0.
                Add next fragment to the program for determination  М  о зв   n










             1.9 Determination of work of restriction and motion forces
                   during one cycle of mechanism’s steady motion

                Work  of  restriction  forces  is  determined  by  approximate
                                                       о
           numerical method. Let’s integrate function  М  by the formula
                                                       зв
                                               о
                                     о
                                   M зв      M зв
                  A O   n   A O  1n       1n  2    n   
                                                        (J),
           where     2 12 .

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