Springer - Computational Differential Geometry Approach to Grid Generation - 2nd Edition - 2007 O[Z$~
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V.D. Liseikin _U}|Le@ e
A Computational 3+>R%TX6i<
Differential rE*yT(:w
Geometry Approach @IL@|Srs8
to Grid Generation !wAnsK
Second Edition azmeJpC
With 81 Figures OC5oxL2HTe
Including 3 Color Figures t_^cqEr
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Preface to the Second Edition +!@xH];
This second edition of A Computational Differential Geometry Approach to
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Grid Generation is significantly expanded by new material that centers on 1N),k5I
the recent advances in grid generation technology based on the numerical solution j &[lDlI_
of Beltrami and diffusion equations in monitor metrics. It gives a more UVXruH
detailed and practice-oriented description of the monitor metrics for providing K;/f?3q
the generation of adaptive, field-aligned, and balanced numerical grids. ,JH*l:7
New finite-difference codes are described for generating both structured and pYCMJK-H
unstructured surface and domain grids. Numerous applications of the codes CMC p7-v
for the generation of numerical grids with individual and balanced properties ~H''RzN
in surfaces and domains, in particular, in the tokamak-edge region are ="T}mc
demonstrated. The new edition also boasts examples of the implementations i.9}bw
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of the grid generation codes in the codes for the numerical investigations of ?o V.SG'
gas-dynamics and magnetized plasmas problems. <!dZ=9^^1
Grid technology, which has had a significant impact on the efficiency of o< b
numerical codes, remains a rapidly advancing field of computational physics Il/`#b@h
and applied mathematics. New achievements are being added by the creation oItC;T
of more sophisticated techniques, modification of the available methods, and R?:K\
implementation of more subtle tools as well as the results of the theories of 9on$0
differential equations, calculus of variations, and Riemannian geometry in the v2|zIZ
formulation of grid models and analysis of grid properties. 1q'_J?Xmd
The development of comprehensive differential and variational grid generation o
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techniques reviewed in the monographs of J.F. Thompson, Z.U.A.Warsi, '1!%yKc0
and C.W. Mastin, P. Knupp, and S. Steinberg, and V.D. Liseikin has been *)r_Y|vg
largely based on a popular concept in accordance with which a grid model Z+R-}<
realizing the required grid properties should be formulated through a linear Iv7BIK^0
combination of basic and control grid operators with weights. A typical, \.P'8As
basic grid operator is the operator responsible for the well-posedness of the d>M 0:
grid model and construction of unfolding grids, e.g., the Laplace equations :qXREF@h
(generalized Laplace equations referred also to as second-order Beltrami equations) f[zKA{R
or the function of grid smoothness, which produces fixed non-folding b0f6?s
grids while grid clustering is controlled by source terms in differential grid 0lt1/PEKx2
formulations or by an adaptation function in variational models. However, \ bNDeA&l
such a formulation does not obey the fundamental invariance laws with respect >Dv=lgPF
to parameterizations of physical geometries and frequently results in 5UL5C:3R9
VI Preface to the Second Edition *mWS+xcU(L
cumbersome governing grid equations. Besides this, the choice of the weight Gyu =}
and control functions for providing well-posedness, grid non-degeneracy, and fk^DkV^<
adaptation is largely based on unreliable theoretical assumptions borrowed #)D$\0ag
from one-dimensional models. L%7WHtU*#
The current book revises this popular concept and pursues a more updated @bkSA
and somewhat revolutionary one based on the general fact that an "`K73M,c?9
arbitrary one-to-one, smooth multidimensional coordinate transformation deriving l7ES*==&@0
a numerical grid in a domain or on a surface is realized by a solution of CNiJuj`
a system of the Beltrami equations in a suitable monitor metric specified in 5'Mw{`
the physical geometry. The system can be interpreted as the multidimensional 0Q%I[f8
equidistribution principle in which the monitor metric tensor is an extension e,vgD kI;
of a scalar-valued weight function. With this interpretation for a mathematical #;2mP6a[
model for generating grids in domains or on surfaces, one need only choose }8.$)&O$^
the Beltrami equations, without any complementary control operators that 9Lt3^MKa"
worsen the model, while the required grid properties are realized through the }2y"F@{T
specification of suitable metric tensors. ),;h
Thus the single Beltrami mathematical model provides a real foundation `5t~
Vlp
for the solution of the challenging problem of the development of comprehensive 1%.CtTi
grid generators. Consequently the efforts of research should be directed #r&yH^-
towards implementing this model into grid technology by developing !H^R_GC
approaches for formulating metrics in physical geometries and establishing ^-#:T
necessary relations between them and the required grid properties for the K(mzt[n(
purpose of setting up an adequate control of the grid quality by the choice p<a~L~xH6
of the suitable metric. gO~>*q &
One natural approach for formulating metric tensors and corresponding i/N6 8
tensor-valued weight functions is based on the notion of a monitor surface GB>h8yXH
over the physical geometry that undergoes a gridding process. The monitor AxJf\B8
surface is defined as the graph of some (in general vector-valued) function c1%ki%J#
that takes into account the behavior of the physical solution. This monitor a;7gy419<p
surface, having an inherent metric tensor that can be considered as the very ^YPw'cZZ&
tensor-valued weight function, is suitable for generating adaptive grids with #$t93EI
the use of a smoothness functional (which is the functional of energy) whose ^sZHy4-yK#
Euler–Lagrange equations are, in fact, equivalent to the Beltrami equations tV.96P;)/9
in the metric of the monitor surface. The resulting grid derived by this metric 0J )VEMC
tends to cluster its nodes in the zones of the large gradient of the function. The IOUzj{G#
approach for formulating the adaptive metric is readily extended to define #"-w;T%b
more general monitor metrics in domains or on surfaces, thus turning them ]N'4q}<5o
into Riemannian manifolds whose implementation in grid technology allows p'SY 2xq-,
one to generate grids satisfying the most broad mesh quality requirements. YWhS< }^
In order to control the required grid properties by the monitor metrics, (B+zh
one needs a knowledge of geometric characteristics of the monitor geometries 9&c *%mm
and their relations to the resulting grid behavior. This knowledge can be attained $<wU>X
with the aid of the theory of multidimensional differential geometry of 6l?KX
Riemannian manifolds adjusted to the features of grid technology. The theory t;%MSedn
Preface to the Second Edition VII ~xZ)btf
of multidimensional differential geometry is really one of the most promising ?IG+U TI
branches of the pure mathematical field of science, capable of pushing grid xI=[=;L
technology to a more advanced level in its development. Indeed, many notions ctC!b{S"@
and characteristics of common surfaces, such as metric tensors, their invariants, ,J-YfL^x6*
first and second fundamental forms, curvatures and torsions of lines, the 9NC6q-2
mean and Gauss curvatures, and Christoffel symbols, have already been used $_Lcw"xO
by many authors as natural elements in defining grid quality measures and () HIcu*i
formulating appropriate variational and differential grid techniques in a unified iV%tn{fc
manner regardless of the geometry of the physical domains and surfaces. l$p"%5]_
A theory of more general geometric objects, such as regular multidimensional a67NWH
surfaces and Riemannian manifolds implemented for generating grids 2L2)``*
with necessary properties, is expected to become a highly beneficial tool for IW|1)8d
boosting grid technology. The known relations and techniques of differential vw
q Y;7
geometry also present an efficient means for transforming and modernizing 1K$8F ~%Z
the physical and grid equations into a suitable form. It is presumable that Vzrp9&loY
the science of differential geometry will play in numerical grid technology .=b)Ae c
the same role played by the science of matrices in the theory of difference ]\R%@FCYc
approximations of boundary value problems. W$Z""
Therefore, there is a need for a monograph that is essentially aimed at g|3FJA/
providing deep and balanced insight into the fields of grid science, multidimensional V,9UOC,Gn
geometry adjusted to grid technology, and up-to-date achievements DOo34l6#
of the applications of geometric tools to the creation of advanced grid techniques. .!Q[kn0a
With this background the reader will be able to formulate and develop pzBd(d^*
well-posed grid models and algorithms and analyze grid properties with geometry ^nL_*+V`f
related tools, thus taking part in the solution of the very challenging 9%uJ:c?
problem of the development of advanced comprehensive grid generators. I'uRXvEr7
This monograph gives an account of the geometrization of popular comprehensive
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grid methods and presents an important extension to the methods .7zdA IKW
related to the application of the technique of Riemannian manifolds to the h "r)z6Q/
formulation of grid equations by developing some procedures for the construction ZYW=#df R
of monitor metric tensors. Contrary to classical geometric studies, b~;+E#[*
which center on geometric features and characteristics of specified Riemannian ~_L_un.R
manifolds, the problem of finding appropriate monitor metrics for producing _q\w9gN
grid systems with the required properties is somewhat an inverse ,e>N9\*
problem of the creation of Riemannian manifolds with desirable geometric ?<$DQ%bf
characteristics. In accordance with the concept of the inverse problem, the *j=
whdw%J
author of the monograph discusses rather thoroughly some new techniques zTt6L6:u
aimed at the construction of special monitor metrics in physical geometries. *$7c||J7
The techniques are designed by generalizing the projection approach in which 2}R)0][W
the monitor metric in an n-dimensional physical geometry is borrowed from ;lo!o9`<
a natural metric of the n-dimensional surface derived by a height monitor au1(.(
function over the geometry. This technology allows the required metric to ;,]Wtmu)7
be defined through the original metric of the physical geometry and certain 6cOm 8#
vector-valued functions. {Uu|NA87Cd
VIII Preface to the Second Edition #$>m`r
The book establishes and reviews some of the relations of the Riemannian A0Hs d
geometry for the purpose of obtaining new equations with implemented metric G&*2h2,]
characteristics aimed at facilitating the control of the generation of grids Z4Qq#iHZR
with the required properties. Taking advantage of the relations established, xBcE>^{1.
the author has converted the equations into a compact form convenient for U,u\o@3A
numerical treatment via the available algorithms. AUAJMS!m
The technique of multidimensional differential geometry is also applied l<nL8/5{<
to study the qualitative effect of a general class of monitor metrics on the bc|DC,n?
resulting mesh. For this purpose a new characteristic of grid clustering is HTCn=MZm
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formulated. Certain relations between this measurement and some geometric *e05{C:kS
characteristics of grid hypersurfaces and the monitor functions forming the nz]+G2h
monitor metrics are established. The well-known results for grids generated P\H$*6v(
by inverted Laplace equations about node-clustering near concave boundary a2un[$Jq`
segments of domains and node-rarefaction near convex boundary segments S(*SUH
are, using these relations, extended to arbitrary boundary segments and to X8b= z9
more general Beltrami equations in monitor metrics. On the basis of the y|%rW
established formulas, the monitor functions are readily estimated in the inverted MY}B)`yx=
diffusion and Beltrami grid equations to provide grid clustering or, if it .),m7"u|
is reasonable, grid rarefaction near arbitrary segments of physical geometries. MkG*6A
Some relations of the mean curvature of the monitor surfaces to the Beltrami @(A[H^E
equations for grid generation are exhibited. The book also includes Dos`lh
a chapter devoted to the implementation of the comprehensive grid equations O9W|&LAL
and the energy functional into numerical codes and to the application ',p`B-dw
of the codes to the numerical solution of some gas-dynamics and plasmarelated h{cJ S9e}
problems. oos7x6
Since grid technology has widespread applications to nearly all field problems, $McVK>=
this monograph will be useful for a broad range of readers, including ZjXpMx,
teachers, students, and researchers as well as practitioners in applied mathematics, sk_Q\0a
mechanics, biology, medicine, and physics interested in the numerical t/aT
analysis of multidimensional field problems with complicated geometries and e'z[JG=
complex solutions. It@.U|
The book is divided into two parts. Part I of the book gives a geometric $/Q*@4t
background needed for the development of grid generators. The grid equations, (-(sBQ a+
codes, and applications are described in Part II. B@Q Ate7
Part I of the monograph includes Chaps. 1–4. Chapter 1 gives a general introduction "V;M,/Q|
to the subject of numerical grids and methods of their generation. H?>R#Ds-
Chapters 2–4 introduce the reader to multidimensional differential geometry C2<