Page 39 - Schaum's Outline of Theory and Problems of Applied Physics
P. 39

24                                      VECTORS                                   [CHAP. 2








                      F x  = F cos q
                      F  = F sin q
                       y
                             F y
                                 F
                                q
                                   F x

                            Fig. 2-13                                    Fig. 2-14
        SOLVED PROBLEM 2.10

              The man in Fig. 2-13 exerts a force of 100 N on the wagon at an angle of θ = 30 above the horizontal.
                                                                               ◦
              Find the horizontal and vertical components of this force.
                  The magnitudes of F x and F y are, respectively,
                                                               ◦
                                        F x = F cos θ = (100 N)(cos 30 ) = 86.6N
                                        F y = F sin θ = (100 N)(sin 30 ) = 50.0N
                                                              ◦
              We note that F x + F y = 136.6 N although F itself has the magnitude F = 100 N. What is wrong? The answer is
              that nothing is wrong. Because F x and F y are just the magnitudes of the vectors F x and F y , it is meaningless to add
              them. However, we can certainly add the vectors F x and F y to find the magnitude of their resultant F. Because F x
              and F y are perpendicular,


                                           2   2          2        2
                                    F =   F + F =   (86.6N) + (50.0N) = 100 N
                                           x
                                               y
              as we expect.
        SOLVED PROBLEM 2.11
              A woman in a car on a level road sees an airplane traveling in the same direction that is climbing at an
              angle of 30 above the horizontal. By driving at 110 km/h she is able to stay directly below the airplane.
                       ◦
              Find the airplane’s velocity.
                  The car’s velocity is equal to the horizontal component v x of the airplane’s velocity v, as in Fig. 2-15. Since
                                                   v x = v cos θ

              the airplane’s velocity v is
                                                    110 km/h
                                               v x
                                          v =     =         = 127 km/h
                                              cos θ  cos 30 ◦














                                                    Fig. 2-15
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