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Elements of Vector Algebra



                this axis.                                                                            ✓

                            −→
                   If vector AB forms an acute angle with axis l, then x 2 > x 1 and projection x 2 −x 1 > 0 (fig.
                               −→
               4.7) b; if vector AB forms an obtuse angle with axis l, then x 2 < x 1 and projection x 2 − x 1 < 0
                                    −→
               (fig. 4.7) c; if vector AB is perpendicular to axis l, then x 2 = x 1 and projection x 2 − x 1 = 0.
                                         −→                             −→
                   A projection of vector AB into axis l is denoted by pr−→AB.
                                                                       l

                                             B                                               B

                                                              B


                              A                                          A               A

                             x 1             x 2              x 2    x 1
                              . . . . . . . . . . . . . . . . . . . . . .
                      O                         l O                         l      O               l
                                                                                        x 1 = x 2
                               A 1         B 1              B 1        A 1
                                            Figure 4.7 – Projection of a vector


                   Let’s concider some main theorems on projections.


                Theorem 4.1.
                The projection of vector a onto axis l equals to the module of vector a , multiplied by cosine
                                        − →
                                                                                  −→
                of angle φ between this vector and axis:

                                                    −→
                                                             −→
                                               pr−→AB = | a | · cos φ                              (4.1)
                                                   l
                                                                                                     ⋆




                                                                   B


                                                          −→
                                                          a


                                                         φ      x
                                             O = A  . . . . . . . .         l
                                                                 B 1

                                            Figure 4.8 – Projection of a vector




                                                     −→
                 PROOF. Projectionx 2 −x 1 ofvector a willnotchangeatanyparalleltransferenceofthisvector.
                                                                      −→
                 Therefore let’s consider the case when the beginning of vector a coincides with the beginning of axis
                                                                                      −→
                 l (point O) ( fig. 4.8). As the coordinate of beginning equals to zero, then pr−→AB = x − 0 = x,
                                                                                     l
                 where x — is the coordinate of the projection of the end of this vector. According to the definition of
                                                             −→
                                                                    −→
                                            −→
                 cosine, cos φ =  x  . So, x = | a | · cos φ or pr−→AB = | a | · cos φ.                2
                                −→
                               | a |                       l

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