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are then called rectangular components. For analytical work we can
         represent these components in one  of  two  ways,  using  either scalar
         notation or Cartesian vector notation.
              Scalar Notation. The rectangular components of force F shown
         in Fig. 1-1 are found using the parallelogram law, so that F  = F x  + F .
                                                                        y
         Because these components form a right triangle, their magnitudes can
         be determined from F =  F cosθ  and F =  F sinθ .
                             x
                                             y














                        a                                b
                                     Fig. 1-1.

              Instead of using the angle, however, the direction of F can also
         be defined using a small “slope” triangle, such as shown in Fig. 1-1,b.
         Since this triangle and the larger  shaded triangle  are similar, the
         proportional length of the sides gives
                                   F x  =  a                                                  1-1
                                   F    c
         or
                                           a
                                          
                                    F =  F                          1-2
                                     x
                                           c
                                          
         and
                                    F y  =  b                         1-3
                                    F    c
         or



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