Page 60 - Basic Structured Grid Generation
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Differential geometry of surfaces in E 3  49

                          A surface vector A has covariant and contravariant components with respect to the
                        surface base vectors given, respectively, by

                                                               α
                                                                       α
                                                A α = A · a α ,  A = A · a .               (3.35)
                          Since eqn (3.16) can be written
                                                              α
                                                            du du β
                                                     1 = a αβ      ,                       (3.36)
                                                             ds ds
                                                                        α
                                                                α
                        it follows by comparison with eqn (3.26) that du /ds = λ represents the contravariant
                                                                       3
                        components of a unit surface vector. Viewed from E this vector λ has cartesian
                        components
                                                    dy i  ∂y i du α  ∂y i  α
                                               λ i =   =          =    λ                   (3.37)
                                                    ds    ∂u α  ds  ∂u α
                        (which may be regarded as a set of direction cosines) and background contravariant
                        curvilinear components
                                                            i
                                                   dx i   ∂x du α   ∂x i
                                                i                       α
                                               λ =     =         =     λ .                 (3.38)
                                                    ds    ∂u α  ds  ∂u α
                          The angle θ between directions specified by unit surface vectors λ and µ each
                                                     α
                                     α β
                                                       β
                        satisfying a αβ λ λ = 1and a αβ µ µ = 1isgiven by
                                                    cos θ = λ · µ = λ i µ i
                        in cartesian components, or, by eqn (3.37),
                                                     ∂y i ∂y i  α  β    α  β
                                              cos θ =       λ µ = a αβ λ µ                 (3.39)
                                                       α
                                                     ∂u ∂u β
                        using eqn (3.17). This result may be compared with the general equations for a scalar
                        product in eqn (1.54).
                                                                1
                                                                      2
                          Unit surface vectors λ, µ tangential to the u and u co-ordinate curves at a point
                        must have contravariant components given by, respectively,
                                             1                                 1
                                        1           2           1        2
                                       λ = √    ,  λ = 0   and µ = 0,   µ = √     .        (3.40)
                                             a 11                              a 22
                          According to eqn (3.39) the angle θ between the co-ordinate curves is given by

                                                           1 2     a 12
                                                cos θ = a 12 λ µ = √    .                  (3.41)
                                                                   a 11 a 22
                          The co-ordinate curves form an orthogonal network if a 12 = F = 0 everywhere.
                          The element of surface area dσ given by the parallelogram with sides formed by
                                                  2
                                            1
                        the line-segments a 1 du , a 2 du tangential to the co-ordinate curves at a point is
                                                          √    1  2
                                                     dσ =  a du du ,                       (3.42)
                        analogously to eqn (1.44).
                          It is sometimes convenient to have at our disposal the two-dimensional alternating
                        symbol e αβ  = e αβ satisfying
                                11         22            12             21
                               e  = e 11 = e  = e 22 = 0,  e  = e 12 = 1,  e  = e 21 =−1.  (3.43)
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