Page 59 - Basic Structured Grid Generation
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48  Basic Structured Grid Generation

                        Exercise 3. Show (by taking determinants of both sides of eqn (3.18)) that the property
                        of positive definiteness of a αβ is preserved under co-ordinate transformations provided
                        the Jacobian of the transformation is non-zero.
                          Vectors in the tangent plane to S at a point P of the surface are linear combinations
                        of the tangent vectors a 1 and a 2 , and may be called surface vectors. The vectors a α
                        thus serve as covariant base vectors for the tangent plane, and a surface vector A with
                                                              α
                               α
                        A = A a α has contravariant components A ,α = 1, 2. An equation analogous to
                        eqn (1.55) now gives the length of a surface vector A :

                                                                   β
                                                                α
                                                    |A|=    a αβ A A .                     (3.26)
                                                                         α
                          We can also define surface contravariant base vectors a ,α = 1, 2, such that
                                                        α
                                                                α
                                                       a · a β = δ ,                       (3.27)
                                                                β
                        and the surface contravariant metric tensor
                                                             α
                                                                 β
                                                      a αβ  = a · a .                      (3.28)
                          The symmetric 2 × 2 matrix array corresponding to (3.28) is the inverse of that
                        corresponding to eqn (3.17), that is,
                                                                γ
                                                       a αβ a αγ  = δ .                    (3.29)
                                                                β
                          Thus we have, explicitly,
                                       11            12   21             22
                                      a  = a 22 /a,  a  = a  =−a 12 /a,  a  = a 11 /a.     (3.30)
                                                  αβ
                                             α
                        Exercise 4. Show that a = a a β with
                                          1                        1
                                      1                        2
                                     a =   (a 22 a 1 − a 12 a 2 )  and a =  (−a 12 a 1 + a 11 a 2 ).  (3.31)
                                          a                        a
                                                                           3
                        Exercise 5. A surface of revolution may be generated in E by rotating the curve in
                        the cartesian plane Oxz given in parametric form by x = f(u), z = g(u) about the
                        axis Oz. This gives the parametric form
                                         x = f(u) cos v,  y = f(u) sin v,  z = g(u),       (3.32)
                        where u and v may be used as surface co-ordinates. Show that the covariant surface
                                             1
                                                       2
                        base vectors, with u = u and v = u ,are



                              a 1 = (f (u) cos v, f (u) sin v, g (u)),  a 2 = (−f(u) sin v, f (u) cos v, 0)
                        in background cartesian co-ordinates and that the covariant metric tensor has
                        components
                                                           2    2
                                                         f  + g    0
                                                 a αβ =             2  ,                   (3.33)
                                                            0     f
                        which are functions of u but not v, while the contravariant metric tensor is
                                                          2    2 −1
                                               αβ     (f  + g )      0
                                              a   =                  −2   .                (3.34)
                                                            0       f
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