Page 198 - Schaum's Outline of Theory and Problems of Advanced Calculus
P. 198

CHAP. 8]               APPLICATIONS OF PARTIAL DERIVATIVES                      189


                                           Gðx 1 ; x 2 ; ... ; x n Þ  F þ   1   1 þ   2   2 þ     þ   k   k  ð23Þ
                     subject to the (necessary) conditions
                                                   @G     @G        @G
                                                      ¼ 0;   ¼ 0; ... ;    0                        ð24Þ
                                                   @x 1   @x 2      @x n
                     where   1 ;  2 ; ... ;  k , which are independent of x 1 ; x 2 ; ... ; x n , are the Lagrange multipliers.


                     APPLICATIONS TO ERRORS
                        The theory of differentials can be applied to obtain errors in a function of x; y; z, etc., when the
                     errors in x; y; z, etc., are known.  See Problem 8.28.



                                                     Solved Problems


                     TANGENT PLANE AND NORMAL LINE TO A SURFACE
                                                                                              2      2
                      8.1. Find equations for the (a) tangent plane and (b) normal line to the surface x yz þ 3y ¼
                             2
                           2xz   8z at the point ð1; 2;  1Þ.
                                                              2
                                                                   2
                                                        2
                           (a) The equation of the surface is F ¼ x yz þ 3y   2xz þ 8z ¼ 0. A normal to the surface at ð1; 2;  1Þ is
                                                             2    2        2
                                        N 0 ¼rFj ð1;2; 1Þ ¼ð2xyz   2z Þi þðx z þ 6yÞj þðx y   4xz þ 8Þkj ð1;2; 1Þ
                                                   ¼ 6i þ 11j þ 14k
                                  Referring to Fig. 8-1, Page 183:
                                     The vector from O to any point ðx; y; zÞ on the tangent plane is r ¼ xi þ yj þ zk.
                                     The vector from O to the point ð1; 2;  1Þ on the tangent plane is r 0 ¼ i þ 2j   k.
                                     The vector r   r 0 ¼ðx   1Þi þð y   2Þj þðz þ 1Þk lies in the tangent plane and is thus perpen-
                                     dicular to N 0 .
                              Then the required equation is
                                    ðr   r 0 Þ  N 0 ¼ 0  i:e:;  fðx   1Þi þð y   2Þj þðz þ 1Þkg f 6i þ 11j þ 14kg¼ 0
                                        6ðx   1Þþ 11ð y   2Þþ 14ðz þ 1Þ¼ 0  or  6x   11y   14z þ 2 ¼ 0
                           (b)Let r ¼ xi þ yj þ zk be the vector from O to any point ðx; y; zÞ of the normal N 0 . The vector from O to
                              the point ð1; 2;  1Þ on the normal is r 0 ¼ i þ 2j   k. The vector r   r 0 ¼ðx   1Þi þð y   2Þj þðz þ 1Þk
                              is collinear with N 0 .  Then

                                                                     i    j
                                                                               k

                                             ðr   r 0 Þ  N 0 ¼ 0  i:e:;      x   1 y   2 z þ 1 ¼ 0


                                                                      6   11   14
                              which is equivalent to the equations
                                     11ðx   1Þ¼  6ð y   2Þ;  14ð y   2Þ¼ 11ðz þ 1Þ;  14ðx   1Þ¼ 6ðz þ 1Þ
                              These can be written as
                                                         x   1  y   2  z þ 1
                                                           6  ¼  11  ¼  14
                              often called the standard form for the equations of a line. By setting each of these ratios equal to the
                              parameter t,we have
                                                 x ¼ 1   6t;  y ¼ 2 þ 11t;  z ¼ 14t   1
                              called the parametric equations for the line.
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