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Variational methods and adaptive grid generation  167

                        and
                                        1        1                1      1
                                                                           
                                          ϕ ξ x ξ +  ψ η x η        x ξ    x η
                                       ϕ 2      ψ 2               ϕ 2   ψ 2
                                                                             ϕ ξ
                              S =−                       =−                            (6.50)
                                     1          1             1       1     ψ η
                                          ϕ ξ y ξ +  ψ η y η        y ξ    y η
                                       ϕ 2      ψ 2               ϕ 2   ψ 2
                        and partial differentiation (including that of the vector r) is denoted by suffixes.
                        6.4.3 The weighted area-functional

                        The area-functional generally provides a more satisfactory grid than the length-functional.
                        The objective here is to generate a grid such that the area of grid-cells is proportional to
                        some given positive weight function ϕ(ξ, η) in computational space. Given that the area
                        of grid-cells in the physical domain corresponding to uniform grid-cells of fixed area in
                                                             √
                        the computational domain is proportional to  g, a natural way to define a functional by
                        analogy with the length functionals above would be to put
                                            1        g          1       J  2
                                       I A =            dξ dη =             dξ dη,         (6.51)
                                            2   R ϕ(ξ, η)       2   R ϕ(ξ, η)


                        where the Jacobian J = (x ξ y η − x η y ξ ).
                        Exercise 2. Show that the Euler-Lagrange equations in this case can be written as

                                                   Jr η      Jr ξ
                                                         −         = 0.
                                                    ϕ   ξ     ϕ   η
                          It may be seen that on further differentiation these equations reduce to

                                                 (J/ϕ) ξ r η − (J/ϕ) η r ξ = 0.            (6.52)
                        Exercise 3. Show that this is equivalent to
                                             A 11 r ξξ + A 12 r ξη + A 22 r ηη + S = 0

                        as in (6.48), with
                                   	      2
                                      (y η )  −x η y η             −2y ξ y η  x ξ y η + x η y ξ
                             A 11 =                  ,   A 12 =                           ,
                                              (x η ) 2
                                      −x η y η                   x ξ y η + x η y ξ  −2x ξ x η
                                   	      2
                                      (y ξ )  −x ξ y ξ        J    y η  −y ξ     ϕ ξ
                              A 22 =             2   ,   S =−                         .    (6.53)
                                      −x ξ y ξ  (x ξ )        ϕ    −x η  x ξ     ϕ η

                        6.4.4 Orthogonality-functional


                        An orthogonality (O)-functional without weight function is
                                                       1         2
                                                  I O =     (g 12 ) dξ dη,                 (6.54)
                                                       2   R
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