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Analytic geometry in space


               8.6.1. Canonical equation of a line



                                                    z                     (l)
                                                                        M




                                                                          −→
                                                                           s
                                                               M 0


                                                                           y
                                                     . . . . . . . . .
                                                      0

                                            x

                                         Figure 8.9 – Canonical equation of a line


                   To solve the task, some special equations of the line in space can be used. Let’s suppose
                                                                                            − →
                                         −→
               line l and non-zero vector s = (m, n, p), which is parallel to this line. Vector s is called the
               directed vector of the line. Point M 0 (x 0 , y 0 , z 0 ) belongs to the line (fig. 8.9). In order to obtain
                                                          −→
               the equation of the line with directed vector s , passing through point M 0 , let’s take any point
                                              −−−→
               M(x, y, z) and consider vector M 0 M = (x − x 0 , y − y 0 , z − z 0 ). It is obvious, that regardless
                                                               −→     −→
               of the position of point M on the line, vectors M 0 M and s are colinear. Therefore, according
               to the condition of colinearity:

                                               x − x 0   y − y 0   z − z 0
                                                       =         =        .                         (8.16)
                                                  m         n         p

                   Equation (8.16) is called the canonical equation of the line.

                                                                            −→
                Remark 8.4. In case one of coordinates of vector s , for example, m = 0, i.e.
                this vector is perpendicular to axis Ox, the canonical equation of the line looks like:
                x−x 0  =  y−y 0  =  z−z 0 . So, the line, which is perpendicular to axis Ox, can be presented
                  0       n      p
                                               {
                                                 x − x 0 = 0,
                                                                                                     −→
                by means of two equations:        y−y 0  z−z 0  In case two coordinates of vector s ,
                                                   n  =    p  .
                for example, m = 0 and n = 0, i.e. this vector is perpendicular to axes Ox and Oy (or
                is parallel to axis Oz), the canonical equation of the line looks like:  x−x 0  =  y−y 0  =  z−z 0  .
                                                                                      0       0      p
                So, the line, which is perpendicular to axis Oz, can be presented by means of two
                            {
                               x = x 0 ,
                equations:              For example, equation   x  =  y  =  z  is the canonical equation of
                               y = y 0 .                        0    0   1
                axis Oz.


                Remark 8.5. In order to pass from the general equation of the line to its canon-
                ical one, it is necessary:
                   — to find any point M 0 (x 0 , y 0 , z 0 ), which belongs to the line. In order to do that,
                      it is sufficient to assume any variable and obtain another coordinates from
                      equation (8.15);
                                             −→
                   — to find normal vector s = (m, n, p). Since line l is the line of crossing two planes
                                                                                    − →
                      (p 1 ) and (p 2 ), then this line is perpendicular to each vector n 1 (A 1 , B 1 , C 1 ) and



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