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Summary                               225



                     DOT PRODUCT (OR SCALAR PRODUCT)           A   B   AB cos u   A B   A B   A B                  (7.6; 7.8)
                                                                                 x x    y y   z z
                     OF TWO VECTORS


                     WORK DONE BY CONSTANT GRAVITATIONAL       W   mgh                                                (7.11)
                     FORCE (Descending from a height h)


                     WORK DONE BY A VARIABLE FORCE                   b                             This area is work done  (7.15)
                                                                                                   by F x  during motion
                     In one dimension                          W       F (x) dx                 F x  from x = a to x = b.
                                                                      x
                                                                    a




                                                                                                             x
                                                                                                  a       b

                     In two or three dimensions                                                                       (7.16)
                                                               W     F # ds


                                                                        2
                                                                             2
                                                                     1
                     WORK DONE BY A SPRING                     W    k (b   a )                                        (7.17)
                                                                     2
                     (Moving from x   a to x   b)
                     KINETIC ENERGY                                1  2                                               (7.23)
                                                               K   mv
                                                                   2

                     WORK–ENERGY THEOREM                       ¢K   W                                                 (7.25)



                     GRAVITATIONAL POTENTIAL ENERGY            U   m g y                                              (7.29)



                     RELATION BETWEEN WORK AND CHANGE          W   ¢U                                                 (7.31)
                     IN POTENTIAL ENERGY


                     MECHANICAL ENERGY                         E   K   U                                              (7.34)



                     CONSERVATION OF MECHANICAL ENERGY         E   K   U   [constant]                                 (7.35)



                                                               1  2         1   2             y
                     CONSERVATION OF MECHANICAL ENERGY         mv   mg y   mv   mg y   2                              (7.37)
                                                                  1
                                                                         1
                                                                                2
                                                               2            2
                     AT TWO POINTS                                                                       1  2
                                                                                                         2
                                                                                           P 1        F =   mv 1  + mgy 1
                                                                                                           1  2
                                                                                                        F =   mv 2  + mgy 2
                                                                                                           2
                                                                                           y 1
                                                                                          y 2
                                                                                           O                    x
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