Page 38 - Schaum's Outline of Theory and Problems of Applied Physics
P. 38

CHAP. 2]                                 VECTORS                                       23



                      ◦
              equal to 90 . Since φ = θ = 90 ,
                                     ◦
                                                              ◦
                                                         ◦
                                            φ = 90 − θ = 90 − 63 = 27 ◦
                                                 ◦
              The resultant R has a magnitude of 11.2 km, and its direction is 27 east of north.
                                                              ◦











                                                    Fig. 2-11


        RESOLVING A VECTOR
        Just as two or more vectors can be added to yield a single resultant vector, so it is possible to break up a single
        vector into two or more other vectors. If vectors A and B are together equivalent to vector C, then vector C is
        equivalent to the two vectors A and B (Fig. 2-12). When a vector is replaced by two or more others, the process
        is called resolving the vector, and the new vectors are known as the components of the initial vector.














                                                 Fig. 2-12

            The components into which a vector is resolved are nearly always chosen to be perpendicular to one another.
        Figure 2-13 shows a wagon being pulled by a man with force F. Because the wagon moves horizontally, the
        entire force is not effective in influencing its motion. The force F may be resolved into two component vectors
        F x and F y , where
                                        F x = horizontal component of F

                                        F y = vertical component of F
        The magnitudes of these components are
                                        F x = F cos θ  F y = F sin θ
        Evidently the component F x is responsible for the wagon’s motion, and if we were interested in working out the
        details of this motion, we would need to consider only F x .
            In Fig. 2-13 the force F lies in a vertical plane, and the two components F x and F y are enough to describe it.
        In general, however, three mutually perpendicular components are required to completely describe the magnitude
        and direction of a vector quantity. It is customary to label the directions of these components the x, y, and z axes,
        as in Fig. 2-14. The components of some vector A in these directions are accordingly denoted A x , A y , and A z .Ifa
        component falls on the negative part of an axis, its magnitude is considered negative. Thus if A z were downward
        in Fig. 2-14 instead of upward and its length were equivalent to, say, 12 N, we would write A z =−12 N.
        [The newton (N) is the SI unit of force; it is equal to 0.225 lb.]
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