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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 a 2 IgC25  
br-]fE.be  
V.D. Liseikin 2i;7{7  
A Computational /!h;c$  
Differential 21hv%CF\9  
Geometry Approach zk-.u}RBFG  
to Grid Generation kF(n!2"W  
Second Edition 5GA C`}}  
With 81 Figures eET&pP3Rp  
Including 3 Color Figures I/Jb!R ~  
1W7% 1FA  
Preface to the Second Edition I9h ?;(  
This second edition of A Computational Differential Geometry Approach to oND@:>QBF  
Grid Generation is significantly expanded by new material that centers on 4}+/F}TbJ5  
the recent advances in grid generation technology based on the numerical solution b 5yW_Ozdh  
of Beltrami and diffusion equations in monitor metrics. It gives a more hj'(*ND7z  
detailed and practice-oriented description of the monitor metrics for providing xvl3vAN9  
the generation of adaptive, field-aligned, and balanced numerical grids. yY?b.ty  
New finite-difference codes are described for generating both structured and %\]* OZ7  
unstructured surface and domain grids. Numerous applications of the codes ) e5 @  
for the generation of numerical grids with individual and balanced properties wO?{?+I`q  
in surfaces and domains, in particular, in the tokamak-edge region are J'$>Gk]  
demonstrated. The new edition also boasts examples of the implementations #(An6itl  
of the grid generation codes in the codes for the numerical investigations of {9UEq0  
gas-dynamics and magnetized plasmas problems. 8YC_3Yi%  
Grid technology, which has had a significant impact on the efficiency of 8J$|NYv_b  
numerical codes, remains a rapidly advancing field of computational physics [ ol9|sdu  
and applied mathematics. New achievements are being added by the creation I:K"'R^  
of more sophisticated techniques, modification of the available methods, and V"c 6Kdtd  
implementation of more subtle tools as well as the results of the theories of WSuww  
differential equations, calculus of variations, and Riemannian geometry in the Po%LE]v,  
formulation of grid models and analysis of grid properties. ;rc`OZyE  
The development of comprehensive differential and variational grid generation !*R qCS,  
techniques reviewed in the monographs of J.F. Thompson, Z.U.A.Warsi, UMAgA!s  
and C.W. Mastin, P. Knupp, and S. Steinberg, and V.D. Liseikin has been okbQ<{9  
largely based on a popular concept in accordance with which a grid model |$?bc3  
realizing the required grid properties should be formulated through a linear AbZKYF P  
combination of basic and control grid operators with weights. A typical, O T.*pk+<)  
basic grid operator is the operator responsible for the well-posedness of the $Y69@s%f  
grid model and construction of unfolding grids, e.g., the Laplace equations lXcx@#~  
(generalized Laplace equations referred also to as second-order Beltrami equations) h1'\:N`  
or the function of grid smoothness, which produces fixed non-folding }zhGS!fO  
grids while grid clustering is controlled by source terms in differential grid i3rH'B -I.  
formulations or by an adaptation function in variational models. However, lOtDqb&  
such a formulation does not obey the fundamental invariance laws with respect hjZKUM G(k  
to parameterizations of physical geometries and frequently results in ;4Y%PV z~D  
VI Preface to the Second Edition 89r DyRJ;  
cumbersome governing grid equations. Besides this, the choice of the weight : q#Xq;Wp  
and control functions for providing well-posedness, grid non-degeneracy, and ^R:cd8+?%  
adaptation is largely based on unreliable theoretical assumptions borrowed <HbcNE~  
from one-dimensional models. nBk)WX&[K  
The current book revises this popular concept and pursues a more updated ep)>X@t  
and somewhat revolutionary one based on the general fact that an 5[c^TJ3  
arbitrary one-to-one, smooth multidimensional coordinate transformation deriving L 4!{h|  
a numerical grid in a domain or on a surface is realized by a solution of E? _Z`*h  
a system of the Beltrami equations in a suitable monitor metric specified in '7XIhN9  
the physical geometry. The system can be interpreted as the multidimensional dCRyOid$  
equidistribution principle in which the monitor metric tensor is an extension d_IAs  
of a scalar-valued weight function. With this interpretation for a mathematical Djg,Lvhm  
model for generating grids in domains or on surfaces, one need only choose w.[ "p9tc  
the Beltrami equations, without any complementary control operators that IiG6<|d8H  
worsen the model, while the required grid properties are realized through the }GeSu|m(  
specification of suitable metric tensors. #O+),,WS  
Thus the single Beltrami mathematical model provides a real foundation T}8Y6N<\m  
for the solution of the challenging problem of the development of comprehensive +E{|63~q  
grid generators. Consequently the efforts of research should be directed l1f\=G?tmU  
towards implementing this model into grid technology by developing h5(4*$%  
approaches for formulating metrics in physical geometries and establishing J+`VujWT  
necessary relations between them and the required grid properties for the \B,(k<  
purpose of setting up an adequate control of the grid quality by the choice zux{S; :?  
of the suitable metric. ~]QHk?[wc  
One natural approach for formulating metric tensors and corresponding U&?v:&c#&n  
tensor-valued weight functions is based on the notion of a monitor surface y&V@^ "`  
over the physical geometry that undergoes a gridding process. The monitor j KoG7HH  
surface is defined as the graph of some (in general vector-valued) function yU9DSY\m{  
that takes into account the behavior of the physical solution. This monitor v%q0OX>9X"  
surface, having an inherent metric tensor that can be considered as the very @)fd}tV  
tensor-valued weight function, is suitable for generating adaptive grids with Mnscb  
the use of a smoothness functional (which is the functional of energy) whose V,%=AR5  
Euler–Lagrange equations are, in fact, equivalent to the Beltrami equations Y'8?.a]'  
in the metric of the monitor surface. The resulting grid derived by this metric 9jw\s P@  
tends to cluster its nodes in the zones of the large gradient of the function. The H '  
approach for formulating the adaptive metric is readily extended to define DAXX;4  
more general monitor metrics in domains or on surfaces, thus turning them /Njd[= B  
into Riemannian manifolds whose implementation in grid technology allows 97}OL`y  
one to generate grids satisfying the most broad mesh quality requirements. 3.*8)NW  
In order to control the required grid properties by the monitor metrics, lhqg$lb  
one needs a knowledge of geometric characteristics of the monitor geometries #3gp6*R  
and their relations to the resulting grid behavior. This knowledge can be attained 9Gnc9_]I;W  
with the aid of the theory of multidimensional differential geometry of ME*LH r,  
Riemannian manifolds adjusted to the features of grid technology. The theory , GP?amh  
Preface to the Second Edition VII T\D}kQM  
of multidimensional differential geometry is really one of the most promising NxsBX :XDn  
branches of the pure mathematical field of science, capable of pushing grid 7eAX*Kgt<_  
technology to a more advanced level in its development. Indeed, many notions d~i+ I5  
and characteristics of common surfaces, such as metric tensors, their invariants, ]"?)Z  
first and second fundamental forms, curvatures and torsions of lines, the JU)dr4S?  
mean and Gauss curvatures, and Christoffel symbols, have already been used ]@phF _  
by many authors as natural elements in defining grid quality measures and R^Y <RI  
formulating appropriate variational and differential grid techniques in a unified (jAg_$6  
manner regardless of the geometry of the physical domains and surfaces. B!?%O  
A theory of more general geometric objects, such as regular multidimensional 'h,VR=e<  
surfaces and Riemannian manifolds implemented for generating grids 8|\8O@  
with necessary properties, is expected to become a highly beneficial tool for ;IZwTXu!S  
boosting grid technology. The known relations and techniques of differential V6@o]*  
geometry also present an efficient means for transforming and modernizing m)'=G%y  
the physical and grid equations into a suitable form. It is presumable that ~5}* d  
the science of differential geometry will play in numerical grid technology 5:KQg  
the same role played by the science of matrices in the theory of difference G;l_|8<t#\  
approximations of boundary value problems. pe 1R(|H  
Therefore, there is a need for a monograph that is essentially aimed at Pu"P9  
providing deep and balanced insight into the fields of grid science, multidimensional % ~H=sjg  
geometry adjusted to grid technology, and up-to-date achievements 9-fLz?J  
of the applications of geometric tools to the creation of advanced grid techniques. 4bYK}o S  
With this background the reader will be able to formulate and develop T7hcnF$  
well-posed grid models and algorithms and analyze grid properties with geometry ~ v|>xqWV  
related tools, thus taking part in the solution of the very challenging v@ lM3_rbO  
problem of the development of advanced comprehensive grid generators. oYm[V<nIl  
This monograph gives an account of the geometrization of popular comprehensive G$F<$  
grid methods and presents an important extension to the methods Wa{`VS  
related to the application of the technique of Riemannian manifolds to the V<T9&8l+:  
formulation of grid equations by developing some procedures for the construction ;z$(nhJ  
of monitor metric tensors. Contrary to classical geometric studies, k@k&}N0{  
which center on geometric features and characteristics of specified Riemannian <+?7H\b  
manifolds, the problem of finding appropriate monitor metrics for producing "W955?4m  
grid systems with the required properties is somewhat an inverse 8|l\E VV6  
problem of the creation of Riemannian manifolds with desirable geometric ]H+8rY%+  
characteristics. In accordance with the concept of the inverse problem, the ,)Znb=  
author of the monograph discusses rather thoroughly some new techniques j}.\]$J  
aimed at the construction of special monitor metrics in physical geometries. `xqr{lhL  
The techniques are designed by generalizing the projection approach in which H[U!%Z  
the monitor metric in an n-dimensional physical geometry is borrowed from ',JinE95  
a natural metric of the n-dimensional surface derived by a height monitor ~d|A!S`  
function over the geometry. This technology allows the required metric to  +|n*b  
be defined through the original metric of the physical geometry and certain pL/DZ|S3  
vector-valued functions. 1SCR.@ k<  
VIII Preface to the Second Edition KUlp"{a`,K  
The book establishes and reviews some of the relations of the Riemannian  Ac2n  
geometry for the purpose of obtaining new equations with implemented metric *Doa* wQ  
characteristics aimed at facilitating the control of the generation of grids Lr~=^{  
with the required properties. Taking advantage of the relations established, ix)M`F%P3  
the author has converted the equations into a compact form convenient for RC7]'4o  
numerical treatment via the available algorithms. 42$VhdG  
The technique of multidimensional differential geometry is also applied Ch <[l8;K  
to study the qualitative effect of a general class of monitor metrics on the \o*5  
resulting mesh. For this purpose a new characteristic of grid clustering is }HFN3cq;C  
formulated. Certain relations between this measurement and some geometric b*c*r dTx  
characteristics of grid hypersurfaces and the monitor functions forming the [\v}Ul  
monitor metrics are established. The well-known results for grids generated "Q@ronP(~  
by inverted Laplace equations about node-clustering near concave boundary KBx6NU?;PO  
segments of domains and node-rarefaction near convex boundary segments M_/7D|xl/T  
are, using these relations, extended to arbitrary boundary segments and to q_A!'sm@)  
more general Beltrami equations in monitor metrics. On the basis of the 3TeY%5iVt  
established formulas, the monitor functions are readily estimated in the inverted $5aV:Z3P  
diffusion and Beltrami grid equations to provide grid clustering or, if it YIQ 4t  
is reasonable, grid rarefaction near arbitrary segments of physical geometries. e> e}vZlX  
Some relations of the mean curvature of the monitor surfaces to the Beltrami k@RDvn  
equations for grid generation are exhibited. The book also includes jaII r06  
a chapter devoted to the implementation of the comprehensive grid equations OEA&~4&{7  
and the energy functional into numerical codes and to the application '7hu 2i5  
of the codes to the numerical solution of some gas-dynamics and plasmarelated chM%]|gey  
problems. yerg=,$_i  
Since grid technology has widespread applications to nearly all field problems, ,Z&xNBX  
this monograph will be useful for a broad range of readers, including N8F~8lTi  
teachers, students, and researchers as well as practitioners in applied mathematics, v&DI`xn~  
mechanics, biology, medicine, and physics interested in the numerical Ezc?#<+7  
analysis of multidimensional field problems with complicated geometries and e>+i>/Fn{h  
complex solutions. qr"3y  
The book is divided into two parts. Part I of the book gives a geometric 8lvV4yb  
background needed for the development of grid generators. The grid equations, 7)`nD<j 5  
codes, and applications are described in Part II. S9]'?|  
Part I of the monograph includes Chaps. 1–4. Chapter 1 gives a general introduction vWz m @  
to the subject of numerical grids and methods of their generation. {Aw#?#GPW  
Chapters 2–4 introduce the reader to multidimensional differential geometry [9evz}X  
for the purpose of better understanding those of its techniques that are suitable %[Wh [zZy  
for the implementation into advanced grid generation technologies. The 2_HNhW  
geometric implementation in grid technology pursued in the book assumes the B~MU^ |v  
development of robust techniques for producing appropriate monitor metrics M?Y;a5{  
over both physical domains and surfaces thus converting them into Riemannian n' n/Tu   
manifolds. The metrics should guarantee generation of grids with the [1g8*j~L  
necessary properties through popular mathematical models. AG`L64B  
Preface to the Second Edition IX t5\-v_mG=&  
Part II of the book is devoted to the implementation of geometric tools #rMlI3;  
into the development of grid techniques and codes. It contains Chaps. 5–7. 46_xyz3+  
Chapter 5 deals with fundamental elliptic grid models formulated through gc_:%ki  
the operators of Beltrami and diffusion and establishes compact formulas of Gp?a(-K5  
monitor metrics. Two-dimensional Beltrami equations in the natural metric of X( \ AB  
a physical surface were originally proposed byWarsi for generating fixed grids %g{X?  
on the surface. The ordinary Laplace equations that are the Beltrami equations \A 2r]  
in the Euclidean metric were applied to generate fixed grids in domains qeVfE_<  
by Crowley and Winslow. One justification of the Beltramian operator is e^6)Zz1\  
demonstrated in Chap. 5 by the proof of the statement that an arbitrary nondegenerate 6m* QX+  
smooth transformation of a physical domain or surface is realized 3]}D`Qs6  
as a solution of the Dirichlet boundary value problem for the system of Beltrami LG{,c.Qj*  
grid equations in some appropriate metric. The chapter also discusses 81? hY4  
some variational and harmonic interpretations of the Beltrami equations, in +h|`/ &,  
particular, a variational approach for generating harmonic maps through the `i3NG1 v0  
minimization of energy functionals, which was suggested by Dvinsky. t3 8m'J :>  
With the help of the geometric relations, established in Chap. 4, the grid 1H? u Qy  
equations introduced in Chap. 5 are transformed in Chap. 6 to equations in D=j-!{zB  
invariant forms with respect to independent logical variables. Special monitor 6Zm# bFQ  
metrics over two-dimensional surfaces are designed that result in simpler ElcjtYu4  
transformed equations, even in comparison with the equations that have kbX8$xTM  
been used for generating fixed grids. The chapter also establishes relations _hAcJ{Y  
between the monitor functions and geometric characteristics of the Riemannian CGW.I$u  
manifolds produced and the coordinate lines and surfaces generated by T*Y~\~Jhu  
a corresponding mathematical model, for the purpose of realization of grid 'N (:@]4N  
control through a suitable specification of the monitor functions. V#2+"(7h  
Chapter 7 gives a description of some computational codes for generating ?pW`cFLDHF  
grids with the numerical solution in the logical domain of the elliptic |mxDjgq  
equations obtained in Chap. 6 by changing mutually dependent and independent o[Q MTP  
variables in the original Beltrami and diffusion equations. Some \ub7`01  
numerical aspects related to the development of grid generation codes are V\ZGd+?  
reviewed, in particular, the application of layer-type functions to formulating W9 GxXPA  
monitor metrics and description of two techniques for generating smooth u^@f&BIG]:  
block-structured grids. Numerical results related to the application of the vYwYQG  
grid technology advocated in the book to some gas-dynamics and plasma $v4.sl:x  
problems are also exhibited in this chapter. ysQ_[ ]/  
The book ends with a list of references. "jeb%k  
Acknowledgement Qp)v?k ]  
The author is very grateful for helpful suggestions in geometry, algebra, and &N2N6&Ta/  
numerical techniques made by his colleagues, Professors Borisov, Churkin, EizKoHI-z  
Glasser, Kuzminov, Sharafutdinov, and Shvedov. M8kPj8}{  
The author is also much obliged to the researchers who responded to his ` 06;   
requests and sent files of their papers and of pictures for figures, namely DU0zez I9  
X Preface to the Second Edition M8MR oA6F  
B.S. Azarenok (Figs. 7.10–7.14), A.A. Charakhch’yan (Figs. 7.8–7.9), and Si2k"<5 U  
A.H. Glasser (Figs. 5.11–5.12). Figures 7.10–7.14 were published in Azarenok 2V- 16Q'%  
(2000, 2002), 7.8 in Charakhch’yan and Ivanenko (1997), 7.9 in Lomonosov, d[@X%  
Frolova and Charakhch’yan (1997), and 5.10–5.11 in Glasser et al. (2005). .F4>p=r  
The work over the book was partly supported by the US Civilian Research 1F5XvQl  
& Development Foundation (CRDF): Award NO RU-M1-2579-NO-04. [_R~%Yh+'E  
In particular, the efforts related to the development of grid generation codes, |GdUL%1hnC  
computing figures of grids, and preparing the text of the book in Latex code, l: HTk4$0  
made by I. Kitaeva, Yu. Likhanova, and D. Patrakhin, whom the author CM/H9Kz.  
thanks very much, were remunerated by payments from the CRDF grant. ? &o2st  
Figures 5.6, 7.29 and 7.37 were published in Glasser, Liseikin and Kitaeva 8g@<d ^8@  
(2005), 5.4, 5.8, 7.32 and 7.34 in Glasser et al. (2005). ~Z\8UsVN  
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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thanks!   
离线frank1975

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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
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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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