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[书籍]Computational Differential Geometry Approach to Grid Generation [复制链接]

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只看楼主 倒序阅读 使用道具 楼主  发表于: 2009-09-07
Springer - Computational Differential Geometry Approach to Grid Generation - 2nd Edition - 2007 sHqs)@D  
KjrUTG0oA  
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  
L|y4u;-Q  
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 0WasE1t|  
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$<  
formulations or by an adaptation function in variational models. However, 2Xu?/yd  
such a formulation does not obey the fundamental invariance laws with respect 9uXuV$.  
to parameterizations of physical geometries and frequently results in a@|/D\C  
VI Preface to the Second Edition U>q&p}z0 H  
cumbersome governing grid equations. Besides this, the choice of the weight R^}}-Dv r  
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 dQoZh E  
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 +Za ew679  
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#$d@VG"  
for the solution of the challenging problem of the development of comprehensive c0J=gZiP  
grid generators. Consequently the efforts of research should be directed f8ap+][  
towards implementing this model into grid technology by developing /jR]sC)xs  
approaches for formulating metrics in physical geometries and establishing x=+R0ny  
necessary relations between them and the required grid properties for the ~s}0z&v^te  
purpose of setting up an adequate control of the grid quality by the choice a,o>E4#c  
of the suitable metric. b-/ztZ@u  
One natural approach for formulating metric tensors and corresponding IrAc&Ehul  
tensor-valued weight functions is based on the notion of a monitor surface A)5-w`1  
over the physical geometry that undergoes a gridding process. The monitor i\P?Y(-{  
surface is defined as the graph of some (in general vector-valued) function v&6=(k{E@R  
that takes into account the behavior of the physical solution. This monitor - nWs@\  
surface, having an inherent metric tensor that can be considered as the very :ZP4(}  
tensor-valued weight function, is suitable for generating adaptive grids with -hM nA)+  
the use of a smoothness functional (which is the functional of energy) whose  R^%uEP  
Euler–Lagrange equations are, in fact, equivalent to the Beltrami equations  #RE  
in the metric of the monitor surface. The resulting grid derived by this metric *cjH]MQ0Ak  
tends to cluster its nodes in the zones of the large gradient of the function. The V#j|_N1hm  
approach for formulating the adaptive metric is readily extended to define wzw`9^B  
more general monitor metrics in domains or on surfaces, thus turning them Gj[+{  
into Riemannian manifolds whose implementation in grid technology allows {K{&__Nk  
one to generate grids satisfying the most broad mesh quality requirements. 8q)wT0A~  
In order to control the required grid properties by the monitor metrics, )$V&Nf  
one needs a knowledge of geometric characteristics of the monitor geometries 4Xna}7  
and their relations to the resulting grid behavior. This knowledge can be attained vepZod}D  
with the aid of the theory of multidimensional differential geometry of rsbd DTy  
Riemannian manifolds adjusted to the features of grid technology. The theory }uI(D&?+h  
Preface to the Second Edition VII i|'M'^3r  
of multidimensional differential geometry is really one of the most promising A),nkw0X  
branches of the pure mathematical field of science, capable of pushing grid Qg)=4(<Hr  
technology to a more advanced level in its development. Indeed, many notions >28.^\?H4  
and characteristics of common surfaces, such as metric tensors, their invariants, (nhv#&Fd+  
first and second fundamental forms, curvatures and torsions of lines, the 4$~]t:n  
mean and Gauss curvatures, and Christoffel symbols, have already been used kzA%.bP|  
by many authors as natural elements in defining grid quality measures and RwH<JaL:  
formulating appropriate variational and differential grid techniques in a unified U'pm5Mc\q  
manner regardless of the geometry of the physical domains and surfaces. |{#=#3X  
A theory of more general geometric objects, such as regular multidimensional -29 Sw  
surfaces and Riemannian manifolds implemented for generating grids s\c*ibxM,  
with necessary properties, is expected to become a highly beneficial tool for @ljvTgZ(X  
boosting grid technology. The known relations and techniques of differential ;Nw.  
geometry also present an efficient means for transforming and modernizing $rB20!  
the physical and grid equations into a suitable form. It is presumable that oDyrf"dl  
the science of differential geometry will play in numerical grid technology |E\0Rv{H3  
the same role played by the science of matrices in the theory of difference 0nkon3H  
approximations of boundary value problems. aZ$$a+  
Therefore, there is a need for a monograph that is essentially aimed at -rU~  
providing deep and balanced insight into the fields of grid science, multidimensional 1B;-ea  
geometry adjusted to grid technology, and up-to-date achievements Rp~#zt9:  
of the applications of geometric tools to the creation of advanced grid techniques. *. H1m{V  
With this background the reader will be able to formulate and develop =1dU~B:Lm  
well-posed grid models and algorithms and analyze grid properties with geometry 'Ii%/ Ob!  
related tools, thus taking part in the solution of the very challenging O"otzla  
problem of the development of advanced comprehensive grid generators. (Bta vE  
This monograph gives an account of the geometrization of popular comprehensive 5zebH  
grid methods and presents an important extension to the methods oo{5 :  
related to the application of the technique of Riemannian manifolds to the %5X}4k!p  
formulation of grid equations by developing some procedures for the construction \z}/=Qgc  
of monitor metric tensors. Contrary to classical geometric studies, go, Hfb  
which center on geometric features and characteristics of specified Riemannian ]!>ThBMa  
manifolds, the problem of finding appropriate monitor metrics for producing u3!aKXnv<  
grid systems with the required properties is somewhat an inverse ~|j:xM(i  
problem of the creation of Riemannian manifolds with desirable geometric ^y.e Fz  
characteristics. In accordance with the concept of the inverse problem, the us&!%`  
author of the monograph discusses rather thoroughly some new techniques t@GPB]3[  
aimed at the construction of special monitor metrics in physical geometries. _9Pxtf  
The techniques are designed by generalizing the projection approach in which A#s`!SNv  
the monitor metric in an n-dimensional physical geometry is borrowed from #!Iez vWf  
a natural metric of the n-dimensional surface derived by a height monitor x\=2D<@az  
function over the geometry. This technology allows the required metric to _Qy3A T~  
be defined through the original metric of the physical geometry and certain yOn +Y  
vector-valued functions. Sz\"*W;>  
VIII Preface to the Second Edition jL$&]sQ`O)  
The book establishes and reviews some of the relations of the Riemannian ~Rzn =>a  
geometry for the purpose of obtaining new equations with implemented metric U] 2fV|Hn  
characteristics aimed at facilitating the control of the generation of grids *>Z|!{bI  
with the required properties. Taking advantage of the relations established, +k!Y]_&(:f  
the author has converted the equations into a compact form convenient for P!?Je/ Tz]  
numerical treatment via the available algorithms. UWdPB2x[  
The technique of multidimensional differential geometry is also applied RB5fn+FiZ  
to study the qualitative effect of a general class of monitor metrics on the @PXb^x#k  
resulting mesh. For this purpose a new characteristic of grid clustering is uV]4C^k;`[  
formulated. Certain relations between this measurement and some geometric p_!;N^y.  
characteristics of grid hypersurfaces and the monitor functions forming the ,hj5.;M  
monitor metrics are established. The well-known results for grids generated O<3i6   
by inverted Laplace equations about node-clustering near concave boundary >U~B"'!xV  
segments of domains and node-rarefaction near convex boundary segments PZ/gD  
are, using these relations, extended to arbitrary boundary segments and to >*xa\ve  
more general Beltrami equations in monitor metrics. On the basis of the %G%##wv:  
established formulas, the monitor functions are readily estimated in the inverted }*!7 Vrep  
diffusion and Beltrami grid equations to provide grid clustering or, if it f%LzWXA  
is reasonable, grid rarefaction near arbitrary segments of physical geometries. Tct[0B  
Some relations of the mean curvature of the monitor surfaces to the Beltrami FHNK%Ko  
equations for grid generation are exhibited. The book also includes u$%>/cv  
a chapter devoted to the implementation of the comprehensive grid equations zw{cli&S  
and the energy functional into numerical codes and to the application ,`7;S,f  
of the codes to the numerical solution of some gas-dynamics and plasmarelated #1MEmt  
problems. `aFy2x`3  
Since grid technology has widespread applications to nearly all field problems, =-M)2&~L~  
this monograph will be useful for a broad range of readers, including RP]hW{:U  
teachers, students, and researchers as well as practitioners in applied mathematics, S~"1q 0  
mechanics, biology, medicine, and physics interested in the numerical U D9&k^  
analysis of multidimensional field problems with complicated geometries and 32_{nLV$[  
complex solutions. NO4V{}?a  
The book is divided into two parts. Part I of the book gives a geometric \NYtxGV[Z  
background needed for the development of grid generators. The grid equations, {VC4rA  
codes, and applications are described in Part II. c#q OK  
Part I of the monograph includes Chaps. 1–4. Chapter 1 gives a general introduction B/IPG~aMEZ  
to the subject of numerical grids and methods of their generation. |aiP7C  
Chapters 2–4 introduce the reader to multidimensional differential geometry !P7##ho0  
for the purpose of better understanding those of its techniques that are suitable >wK ^W{  
for the implementation into advanced grid generation technologies. The *}9i@DP1,  
geometric implementation in grid technology pursued in the book assumes the r7tN(2;5  
development of robust techniques for producing appropriate monitor metrics q&IO9/[dk  
over both physical domains and surfaces thus converting them into Riemannian ?^z!yD\  
manifolds. The metrics should guarantee generation of grids with the Te%'9-jk  
necessary properties through popular mathematical models. o E+s8Q  
Preface to the Second Edition IX R jO9E.nm  
Part II of the book is devoted to the implementation of geometric tools 1'5I]D ec  
into the development of grid techniques and codes. It contains Chaps. 5–7. I0 y+,~\  
Chapter 5 deals with fundamental elliptic grid models formulated through <B]\&  
the operators of Beltrami and diffusion and establishes compact formulas of [3a-1,  
monitor metrics. Two-dimensional Beltrami equations in the natural metric of )oOcV%  
a physical surface were originally proposed byWarsi for generating fixed grids o0-7#2  
on the surface. The ordinary Laplace equations that are the Beltrami equations @MfuV4*  
in the Euclidean metric were applied to generate fixed grids in domains ?Gq'r2V  
by Crowley and Winslow. One justification of the Beltramian operator is O_*(:Z  
demonstrated in Chap. 5 by the proof of the statement that an arbitrary nondegenerate &"dT/5}6  
smooth transformation of a physical domain or surface is realized !B==cNq  
as a solution of the Dirichlet boundary value problem for the system of Beltrami KKm0@Y   
grid equations in some appropriate metric. The chapter also discusses tuA,t  
some variational and harmonic interpretations of the Beltrami equations, in CroI,=a&,  
particular, a variational approach for generating harmonic maps through the *_<P% J  
minimization of energy functionals, which was suggested by Dvinsky. ETP}mo  
With the help of the geometric relations, established in Chap. 4, the grid ({3hX"C@Q  
equations introduced in Chap. 5 are transformed in Chap. 6 to equations in ;!<WL@C~  
invariant forms with respect to independent logical variables. Special monitor "7R"(.~>  
metrics over two-dimensional surfaces are designed that result in simpler Wt +, 6Cq  
transformed equations, even in comparison with the equations that have xCH,d:n=  
been used for generating fixed grids. The chapter also establishes relations G Q&9b_  
between the monitor functions and geometric characteristics of the Riemannian S~1>q+<Q  
manifolds produced and the coordinate lines and surfaces generated by G"CV S@  
a corresponding mathematical model, for the purpose of realization of grid k^q}F%UV  
control through a suitable specification of the monitor functions. Sd;/yC8  
Chapter 7 gives a description of some computational codes for generating I)~&6@J n  
grids with the numerical solution in the logical domain of the elliptic KlgPDV9mg  
equations obtained in Chap. 6 by changing mutually dependent and independent 0\t k/<w2  
variables in the original Beltrami and diffusion equations. Some *|n::9  
numerical aspects related to the development of grid generation codes are X!5  
reviewed, in particular, the application of layer-type functions to formulating { 7y.0_Y  
monitor metrics and description of two techniques for generating smooth $!c)%qDq  
block-structured grids. Numerical results related to the application of the 0_Hdj K  
grid technology advocated in the book to some gas-dynamics and plasma I At;?4  
problems are also exhibited in this chapter. 2e}${NZN  
The book ends with a list of references. !F0MLvdX7^  
Acknowledgement 9I>+Q&   
The author is very grateful for helpful suggestions in geometry, algebra, and wj>mk  
numerical techniques made by his colleagues, Professors Borisov, Churkin, Q]_3 #_'  
Glasser, Kuzminov, Sharafutdinov, and Shvedov. a a<9%j  
The author is also much obliged to the researchers who responded to his V:h-K`~ /  
requests and sent files of their papers and of pictures for figures, namely ~Mv@Bl  
X Preface to the Second Edition R9SJ;TsE  
B.S. Azarenok (Figs. 7.10–7.14), A.A. Charakhch’yan (Figs. 7.8–7.9), and ^/ K\a ,  
A.H. Glasser (Figs. 5.11–5.12). Figures 7.10–7.14 were published in Azarenok ,63hO.4M  
(2000, 2002), 7.8 in Charakhch’yan and Ivanenko (1997), 7.9 in Lomonosov, j(|G) F  
Frolova and Charakhch’yan (1997), and 5.10–5.11 in Glasser et al. (2005). t&UPU&tY  
The work over the book was partly supported by the US Civilian Research )u7*YlU\I  
& Development Foundation (CRDF): Award NO RU-M1-2579-NO-04. /#Y)nyE  
In particular, the efforts related to the development of grid generation codes, Wxl^f?I`:  
computing figures of grids, and preparing the text of the book in Latex code, ; Xy\7tx  
made by I. Kitaeva, Yu. Likhanova, and D. Patrakhin, whom the author _A*5BAB:h(  
thanks very much, were remunerated by payments from the CRDF grant. NiU}A$U  
Figures 5.6, 7.29 and 7.37 were published in Glasser, Liseikin and Kitaeva !g /&ws&  
(2005), 5.4, 5.8, 7.32 and 7.34 in Glasser et al. (2005). _S:6;_bz  
Novosibirsk, March 2006 Vladimir D. Liseikin
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离线sjzdh01

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只看该作者 1楼 发表于: 2009-09-08
下载先学习学习了
离线ymcheng

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只看该作者 2楼 发表于: 2009-09-08
thanks a lot
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只看该作者 3楼 发表于: 2009-09-08
thanks!   
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离线wwhite

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只看该作者 5楼 发表于: 2009-09-13
OIRTSH[PDTUK[I8K\-IO\R6809\=0P\=8P=8P-9-=0\=Y78976R9Y8II
离线wwhite

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PORSTY=UO6R7IO-\PI\=PI\-YU==O-=\Y\=RTY=0U0=YT0OU-0RIY0I-YRY6URYU
离线hnzzncwu

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只看该作者 7楼 发表于: 2013-05-25
数学方法是基础。
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