Page 116 - Basic Structured Grid Generation
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Structured grid generation – algebraic methods  105

                        η which can be used to give an interpolation formula r(ξ, η) between inner and outer
                        curves, with
                                             r(ξ, η i ) = r i (ξ),  i = 1, 2, 3,...,n.    (4.106)

                          Piecewise-linear curves from inner curve r 1 (ξ) to outer curve r n (ξ) may be con-
                        structed by linking together points on all n curves corresponding to the same value
                        of ξ. We assume that these piecewise-linear curves do not intersect each other. A
                        segment of such a curve between the curves r i (ξ) and r i+1 (ξ) must be the vector
                        r i+1 (ξ) − r i (ξ). The multisurface method produces smooth co-ordinate curves r(ξ, η)
                        with ξ fixed and η varying from η 1 to η n by matching tangent vectors ∂r/∂η at each sur-
                        face r i (ξ), i = 1, 2, 3,. ..,n−1, to the directions of the line segment r i+1 (ξ)−r i (ξ).
                        Thus we take
                                                   n−1
                                              ∂r
                                                =     ψ i (η)T i {r i+1 (ξ) − r i (ξ)},   (4.107)
                                             ∂η
                                                   i=1
                        where the T i s are positive scalars associated with the surfaces r 1 , r 2 ,.. . , r n−1 ,and the
                        ψ i s satisfy
                                                       ψ i (η k ) = δ ik .

                        These could be Lagrange polynomials, given by eqn (4.13).
                          Integration then yields

                                                n−1  !  η


                                 r(ξ, η) = r 1 (ξ) +    ψ i (η ) dη    T i {r i+1 (ξ) − r i (ξ)}.  (4.108)
                                                i=1  η 1
                          Note that if we put
                                                                     −1
                                                       !
                                                         η n

                                                 T i =     ψ i (η ) dη    ,               (4.109)
                                                        η 1
                        we obtain an equation which is consistent at η = η n , since the right-hand side of
                        eqn (4.108) reduces to
                                                       n−1

                                                r 1 (ξ) +  {r i+1 (ξ) − r i (ξ)},
                                                       i=1
                        which clearly telescopes down to the left-hand side r(ξ, η n ) = r n (ξ). Equation (4.108)
                        is, of course, also consistent at η = η 1 .
                          Thus the multisurface equation is taken to be
                                                     !  η

                                                         ψ i (η ) dη
                                                n−1

                                                      η 1
                                 r(ξ, η) = r 1 (ξ) +              {r i+1 (ξ) − r i (ξ)}.  (4.110)
                                                     !
                                                       η n

                                                i=1      ψ i (η ) dη
                                                      η 1
                          In the case n = 3, where there is one intermediate surface r 2 (ξ), the approach we
                        take here is to choose parameter values η 1 = 0, η 2 = 1, and η 3 initially unspecified,
                        with value greater than one. We can then use the linear Lagrange polynomials
                                                   ψ 1 = 1 − η,  ψ 2 = η.
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