Springer - Computational Differential Geometry Approach to Grid Generation - 2nd Edition - 2007 sHqs)@D
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V.D. Liseikin N=>6PLie
A Computational 0{ZYYB&"~J
Differential x>>#<hOz[
Geometry Approach uhyw?#f
to Grid Generation B! `Dj,_
Second Edition h,Y!d]2w
With 81 Figures P87!+pB(
Including 3 Color Figures Quc,,#u
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Preface to the Second Edition yGNZw7^(
This second edition of A Computational Differential Geometry Approach to F{:ZHCm
Grid Generation is significantly expanded by new material that centers on A@8Ot-t:\2
the recent advances in grid generation technology based on the numerical solution )HrFWI'Y
of Beltrami and diffusion equations in monitor metrics. It gives a more c+6/@y
detailed and practice-oriented description of the monitor metrics for providing *V\z]Dy-[
the generation of adaptive, field-aligned, and balanced numerical grids. 1]yOC)u"i
New finite-difference codes are described for generating both structured and /Hox]r]'e
unstructured surface and domain grids. Numerous applications of the codes >-2eZ(n)"
for the generation of numerical grids with individual and balanced properties Dq#/Uw#
in surfaces and domains, in particular, in the tokamak-edge region are 61Z#;2]
demonstrated. The new edition also boasts examples of the implementations |H:JwxH
of the grid generation codes in the codes for the numerical investigations of (M1HNIM;(
gas-dynamics and magnetized plasmas problems. @}#" o
Grid technology, which has had a significant impact on the efficiency of 4%8}vCs
numerical codes, remains a rapidly advancing field of computational physics Q*S|SH-cZ0
and applied mathematics. New achievements are being added by the creation LvWl*:z
of more sophisticated techniques, modification of the available methods, and 0W asE1t|
implementation of more subtle tools as well as the results of the theories of >m}U|#;W
differential equations, calculus of variations, and Riemannian geometry in the jV(\]g"/=
formulation of grid models and analysis of grid properties. ]Qo.X~]
The development of comprehensive differential and variational grid generation >&@hm4
techniques reviewed in the monographs of J.F. Thompson, Z.U.A.Warsi, nkKiYr
and C.W. Mastin, P. Knupp, and S. Steinberg, and V.D. Liseikin has been *]ROUk@K=
largely based on a popular concept in accordance with which a grid model 56;(mbW
realizing the required grid properties should be formulated through a linear bv.DW,l%'
combination of basic and control grid operators with weights. A typical, ?_\t7f
basic grid operator is the operator responsible for the well-posedness of the Q?f%]uGFQ
grid model and construction of unfolding grids, e.g., the Laplace equations >^1|Mg/!>
(generalized Laplace equations referred also to as second-order Beltrami equations) U~~Y'R\NU
or the function of grid smoothness, which produces fixed non-folding hSxlj7Eo^T
grids while grid clustering is controlled by source terms in differential grid )KZ1Z$<
formulations or by an adaptation function in variational models. However, 2Xu?/yd
such a formulation does not obey the fundamental invariance laws with respect 9uXu V$.
to parameterizations of physical geometries and frequently results in a@|/D\C
VI Preface to the Second Edition U>q&p}z0H
cumbersome governing grid equations. Besides this, the choice of the weight R^}}-Dvr
and control functions for providing well-posedness, grid non-degeneracy, and |-WoR u
adaptation is largely based on unreliable theoretical assumptions borrowed G}o?lo\#h
from one-dimensional models. dDuT,zP
The current book revises this popular concept and pursues a more updated S?X2MX
and somewhat revolutionary one based on the general fact that an M18H1e@Al
arbitrary one-to-one, smooth multidimensional coordinate transformation deriving dQoZhE
a numerical grid in a domain or on a surface is realized by a solution of s6#@S4^=\
a system of the Beltrami equations in a suitable monitor metric specified in +Zaew679
the physical geometry. The system can be interpreted as the multidimensional 4H7
3a5f
equidistribution principle in which the monitor metric tensor is an extension ]!u12^A{
of a scalar-valued weight function. With this interpretation for a mathematical W\(u1>lj
model for generating grids in domains or on surfaces, one need only choose =h?Q.vad
the Beltrami equations, without any complementary control operators that 59?@55
worsen the model, while the required grid properties are realized through the ;(a\F
specification of suitable metric tensors. -#=y
Thus the single Beltrami mathematical model provides a real foundation ;j#$d@VG"
for the solution of the challenging problem of the development of comprehensive c0J=gZiP
grid generators. Consequently the efforts of research should be directed f8ap+][
towards implementing this model into grid technology by developing /jR]sC)xs
approaches for formulating metrics in physical geometries and establishing x=+R0ny
necessary relations between them and the required grid properties for the ~s}0z&v^te
purpose of setting up an adequate control of the grid quality by the choice a,o>E4#c
of the suitable metric. b-/zt Z@u
One natural approach for formulating metric tensors and corresponding IrAc&Eh