[其它]Introduction to the Uniform Geometrical Theory of Diffraction (几何绕射)

---------本书从2楼到11楼,共9部分. 另推荐同类中文书  向大家推荐《几何绕射理论》 (附件在此贴4楼)-------------- Oe5rRQ$O  
【资料名称】：Introduction to the Uniform Geometrical Theory of Diffraction }3 xkA  
【作者】： YBt=8`r  
D.A. McNamara   J(]|
)?x2  
C.W.I. Pistorius <>HtXn/  
J.A.G. Malherbe _3Eo{^  
University of Pretoria w;'XqpP$*|  
【出版社】：Artech House Publishers +?J N_aR  
【页数】：488/PDF pGs?Y81  
【语言】： 英文 ]8A*uyi  
【发表时间】:1990-01-01 63l3WvoK  
【内容摘要】: $nt&'Xnv  
CONTENTS #9,8{ O"  
CONTENTS s= %3`3Fo  
Preface  xiii ]?6wU-a  
xiii q T6y&  
Preface :-?ZU4)  
1 D{(}&8a9  
Chapter 1  The Nature of High-Frequency Methods  1 nxZz{&  
1  The Nature of High-Frequency Methods &5W;E+Pub  
Chapter +ktv:d  
1 En\@d@j<u  
1.1  Introduction  1 DQ.
4b  
1.1  Introduction x,gk]
Cf  
2 u W]gBhO$O  
1.2  A Brief Historical Overview  2 Y 9$jJ1V  
1.2  A Brief Historical Overview DTO_IP  
1.3  High-Frequency Phenomena  5 KA2>[x2  
5 |Y3w6!$  
1.3  High-Frequency Phenomena a_b#hM/c;  
References  6 od=hCQ1>  
6 +[76_EXy  
References (L(7)WbH  
7 OAXA<  
Chapter 2  Geometrical Optics Fields  7 Yq ]sPE92  
Chapter QuR}6C  
2  Geometrical Optics Fields I=!kPuw  
7 TiD#t+g  
2.1  Introduction  7 Q.N!b7r7  
Introduction 5*44QV  
2.2  Ray Optical Construction of the High-Frequency Field  8
/a\i  
8 iT'doF  
Ray Optical Construction of the High-Frequency Field 1KZigeHXI  
2.2.1  Preliminary Remarks  8 ;W- A2g  
8 ;@Zuet  
2.2.1  Preliminary Remarks )LGVR3#  
8 S~/2Bw!2  
2.2.2  Some Conventional Electromagnetic Theory  8 z/\OtYz  
2.2.2  Some Conventional Electromagnetic Theory ;EBKzB  
10 Lm[,^k  
2.2.3  The Luneberg-Kline Anticipated Solution (Ansatz) Y(UK:LZ'  
10
e]~p:  
The Luneberg-Kline Anticipated Solution (Ansatz) G_+/ e]P  
2.2.3 48:xvTE?N  
11 O#D{:H_dD>  
2.2.4  The Eikonal Equation  11 pS$9mzY  
2.2.4  The Eikonal Equation MT!Y!*-5  
15 m7^f%<l  
2.2.5  Transport Equations  15 uWJJ\  
2.2.5  The Transport Equations J _rrc;F  
17 6{6hz8  
2.2.6  The Geometrical Optics Terms and Their Interpretation  17 JCcYFtW  
2.2.6    he Geometrical Optics Terms and Their Interpretation 4X^$"lM  
19 2"D4q(@  
2.2.7  Ray Paths, Amplitude Functions, and Phase Functions  19 L-9fo-  
Ray Paths, Amplitude Functions, and Phase Functions k'8tcXs  
2.2.7 }+@!c%TCx~  
2.2.8  Sign Conventions and Caustics of the Geometrical Optics y i$+rPF1  
2.2.8  Sign Conventions and Caustics of the Geometrical Optics rl}<&aPH  
Fields lC($@sC%  
28 Ar<5UnT  
28 0/v]YK.  
Fields %`i*SF(gV  
33 h*R@ d  
2.2.9  The Geometrical Optics Field and Fermat's Principle  33 0OO[@Ht  
The Geometrical Optics Field and Format's Principle [H*JFKpx  
2.2.9 ei-\t qY_  
2.3  Summary of the Properties of a High-Frequency Field and Some |%|
03}Q  
Summary of the Properties of a High-Frequency Field and Some  E0!d c  
Special Cases UF-&L:s[  
34 iqlb,8  
34 ,#2~<  
Special Cases 3)WfBvG  
37 G2|jS@L#  
2.4  Specific Examples of Geometrical Optics Fields  37 PhyIea  
Specific Examples of Geometrical Optics Fields O}i+1  
37 /ZyMD(_J  
2.4.1  Initial Comments and Some Definitions  37 }U8v ~wcd  
2.4.1  Initial Comments and Some Definitions -=
5~h
 
37 %,WH*")  
2.4.2  Uniform Plane Wave Fields  37 FO*Gc Z  
2.4.2  Uniform Plane Wave Fields ),yar9C  
40 YZ>L_$:q  
2.4.3  The Fields of Electric and Magnetic Line Sources  40 CHGa_  
2.4.3  The Fields of Electric and Magnetic Line Sources UOb`@
#  
42 ;t0q ?9  
2 .. \Y!#Y#c  
=\lw.59  

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Introduction to the Uniform Geometrical Theory of Diffraction.part09.rar W%+02_/
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共9部分, ;:=j{,&dl[  
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需要回复才能见下载地址 QqF<HCO  
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2.4.7
G T~rr*X  
Sources with Fields That Are Not Geometrical Optics or _zDS-e@  
Ray-Optic Fields RP2$(%  
2.4.8  Further Comment 1#N`elm  
Reduction of Results to Two-Dimensional Ray Tubes dlo`](5m  
2.5 p^Ey6,!8]D  
2.6  Rays in Lossy Media +}m`$B}mJ  
2.7  Concluding Remarks Oey Ph9^V  
A Taste of Things to Come <*J"
6x  
2.8 6H0kY/quL|  
Problems O h e^{:  
References er_6PV  
Chapter h.?<(I  
3  Geometrical Optics Reflected Fields  I / Ei:m@}g  
3.1  Introduction \Yj_U'2"i  
3.1.1  Initial Remarks  < X}'rPz\Lu  
3.1.2 p8 S~`fjV  
A Stroll in the Sun lai@,_<GV  
3.1.3 M%:\ry4:  
A Strategy for This Chapter ?xwi2<zz  
The Law of Reflection, Polarization Properties, and Phase P\dfxR;8%  
3.2 dXDyY  
Functions ^JxVs 7  
3.2.1  The Definition of Certain Geometrical Terms and B4un6-<i  
Coordinate Systems ED8
{  
3.2.2  The Law of Reflection ,$!fyi[;C  
3.2.3  Trajectories of Reflected Rays o%Q9]=%!  
3.2.4  Polarization of Reflected Rays )F hbN@3  
3.2.5 9%kO%j,3  
Phase Continuation along Reflected Rays A@~9r9Uf  
3.2.6 N=u( 3So  
Invocation of the Locality Principle ]A[}:E 5}  
3.2.7  More about Shadowing d1#lC*.Sg  
3.2.8  Geometrical Optics Surface Currents ^N7cXK*  
3.2.9 YN)qMI_`A  
An Alternative Interpretation of the Form of R and the +ase>'<N#  
Law of Reflection 9=}#.W3.  
3.2.10  What More Do We Need? F lVG,Z  
The Expressions for the Geometrical Optics Field Reflected from Gu{1%bb#kL  
3.3 hD#Mhy5h  
Smooth Conducting Surfaces: Two-Dimensional Problems T^eD
  
3.3.1 gIweL{Pc  
When Is a Problem of a Two-Dimensional Nature? =,*/Ph&  
3.3.2 Pjq9BK9p  
Description of the Two-Dimensional Reflecting Surface F$i50s  
Geometry )PR`irw  
3.3.3  Simplifications for Two-Dimensional Problems vV"YgN:  
3.3.4 ,8DC9yM,  
Simplification of the Polarization Description of ~Q"qz<WO  
Reflected GO Fields for Two-Dimensional Problems b:9"nALgC  
3.3.5  Amplitude Continuation along Two-Dimensional G-D}J2r=F  
Reflected Ray Tubes BT(eU*m-  
3.3.6 0<uL0FOT  
The Classical Geometrical Optics Interpretation Y|mtQE?c  
3.3.7 I[A<e]uK  
Summary of Reflected Field Expressions for Two- GF@`~im  
Dimensional Problems 9/8+R%  
3.3.8 ih("`//nP  
On the Specular Point Qr and Its Location UHV"<9tk  
3.3.9  Initial Two-Dimensional Problem Examples lrPIXIM  
3.3.10  Interpretation in Terms of Fundamental Electromagnetic 4NRj>
y  
Theory }qGd*k0F0  
3.3.11  Relationship to Physical Optics UK'8cz9  
3.3.12  Comments on GO Reflected Fields about Shadow '~yxu$aK  
Boundaries X%I@4 B7Ts  
3.4 `!X8Cn  
Further Examples of Two-Dimensional Reflected Field Problems qCVb-f  
3.5  General Expressions for the Reflected Fields from Three- Jm=3%H  
Dimensional Smooth Conducting Surfaces WTD86A  
3.5.1  Introduction -AL^  
3.5.2 r+Sv(KS4i^  
Principal Radii of Curvature of Reflected Ray Tube at VSO(DCr"L  
Q,-First  Format SIM>Lz  
3.5.3  Principal Radii of Curvature of Reflected Ray Tube at maSVqG  
Qr-Second  Format Bs3&yEq(  
3.5.4  Important Special Cases }x6)}sz7  
3.5.5 2 .Xx)(>  
Principal Directions of the Reflected Wavefront 86KK Y2  
3.5.6 v#9i|  
Alternative Form for the Reflected GO Field at the \*5z0A9)5)  
Qr k{!9f=^   
Specular Point [#aJ- Uu  
3.5.7 E}zGY2Xx  
Comments on the Expressions for the Reflected GO \1?'JdN  
Field B{`K?e0  
Alternative Determination of Principal Radii of L8E4|F}  
3.5.8 y:zNf?6&  
Curvature of the Reflected Wavefront j7Zv"Vq@  
3.6 _TdH6[9  
Examples of Three-Dimensional Reflected Field Problems wtL=^  
3.7  Concluding Remarks  f^}n#  
Problems ?1|\(W#  
References sOz {spA  
Chapter |pknaz  
4  Two-Dimensional Wedge Diffraction 1e9~):C~W  
4.1  Introduction Ta3* G  
4.2  Diffraction by Huygens' Principle ',+Zqog92  
4.3  Keller's Original GTD /^K-tz-R  
4.4 kg(}%Ih  
The Uniform Theory of Diffraction #3>jgluM'  
4.4.1  Shadow Boundaries z2R?GQ5 A  
4.4.2  Two-Dimensional UTD Diffraction Coefficients "\lOOp^-  
4.4.3 ',Z]w;D!G
 
Enforcing Continuity across the Shadow Boundaries (uHyWEHt  
4.4.4  Transition Regions U$@}!X  
4.4.5  Grazing Incidence <D& Ep  
4.4.6  Half-Plane and Curved Screen >C{8}Lg-.  
4.4.7  Continuity across the Shadow Boundary: Grazing 6*1f -IbV  
Incidence %IIFLl
D  
4.4.8  Full-Plane $<VH~Q<  
4.5  Slope Diffraction m+dQBsz\  
4.5  Slope Diffraction )`<&~>qp  
220 K{Nj-Rqd  
4.6  General Two-Dimensional Edge Diffracted Fields ifWQwS/,a  
4.6  General Two-Dimensional Edge Diffracted Fields lwG)&qyVd  
225 ,9KnC=_y  
4.7  Dielectric and Impedance Wedges Fv(FRZ)  
4.7  Dielectric and Impedance Wedges Jzp|#*~$E  
227 hBz>E 4mEv  
Problems 2.{zfr  
Problems I(3YXv VN  
228 ]T40VGJ:h  
References L;Ynq<x  
References y9T5  
231 [@pumH
>  
Chapter 5  Applications of Two-Dimensional Wedge Diffraction h0x'QiCc  
5  Applications of Two-Dimensional Wedge Diffraction <}xgp[O  
Chapter i6FJG\d  
235 zk@s#_3ct  
5.1  Radiation from a Parallel Plate Waveguide with TEM Mode vEE\{1  
Radiation from a Parallel Plate Waveguide with TEM Mode dBM{]@bZ  
5.1 x'G_z_<V  
Propagation, Terminated in an Infinite Ground Plane 6c>:h)?  
Propagation, Terminated L*rCUv`  
in an Infinite Ground Plane P=P']\`p+  
235 r|z B?9Q  
5.2  Antenna Gain lkp$rJ#6  
5.2  Antenna Gain ^IvQdVB  
238 I~HA ad,k  
Radiation from ah E-Plane Horn Antenna Wj)v,v2&  
5.3  Radiation from ah E-Plane hVz]',  
Hom Antenna >CcDG  
240 y(a>Y! dgU  
5.3 j:8Pcx  
/ `PLax@]2  
I L[5U(`q[  
, vwAhNw2-  
5.4  Radiation from an H-Plane k:mW ,s|a  
5.4  Radiation from an H-Plane Horn Antenna  r F *U.cJ%  
Hom Antenna Aj/EaIq  
244 44k8IYC*o  
Radar Width of a Two-Dimensional Structure IW}Wt{'m  
5.5  Radar Width of a Two-Dimensional Structure [tC=P&<  
5.5 S
g
N?[r)  
248 ))X"bFP!3  
1' FUL'=Xo  
Problems  { 3
l j^I  
Problems EKuLt*a/  
257 ZBH^
0  
References 1(i%nX<U  
References M
4 }))  
260 ;Ob^@OM  
Chapter 6  Three-Dimensional Wedge Diffraction and Comer Diffraction ~XXNzz]?  
263 0a!|*Z  
6  Three-Dimensional Wedge Diffraction and Corner Diffraction FLG{1dS  
Chapter 4B[uF/[  
6.1  Introduction J_<6;#  
263 6Xn9$C)  
6.1  Introduction O"X7 DgbC  
6.2  Edge-Fixed Coordinate System |~v2~   
265 y\9#"=+  
6.2  Edge-Fixed Coordinate System UsCaO<A  
6.3  Three-Dimensional "2tKh!?Q  
UID Diffraction Coefficients [_
KOU2  
268 Hkf]=kPy*  
6.3  Three-Dimensional UTD Diffraction Coefficients pOB<Bx5t  
Examples of Three-Dimensional Wedge Diffraction ,CBE&g  
6.4  Examples of Three-Dimensional Wedge Diffraction &tiJ=;R1  
274 p&2d&;Qo0  
6.4 p9MJa[}V  
6.5  Comer Diffraction }:s.m8LC5n  
288 A^|~>9  
6.5  Corner Diffraction ZBQ@S  
6.5.1  Comer Diffraction from a Flat Plate <&((vrfa  
Corner Diffraction from a Flat plate qjg Z

 
288 k O.iJcZg  
6.5.1 &:}WfY!hX  
6.5.2  Corner Diffraction from a Vertex ?5%o-hB|  
in Which Wedges with M`* BS  
Corner Diffraction from a Vertex in Which Wedges with ssH[\i  
6.5.2 |v#rSVx  
Arbitrary Wedge Angles Are Terminated s?Gv/&  
Arbitrary Wedge Angles Are Terminated Da)_OJYE  
298 B oiS  
6.6  Alternative Forms of the Diffraction Coefficients G~4G$YL*  
Alternative Forms of the Diffraction Coefficients I,Jb_)H&t  
300 wq8&2(|Fc  
6.6 F0kAQgUv  
Problems 4)XB3$<  
Problems \nTV;@F  
301 Zx: h)I  
References 2P=~6(  
References "F Etl(  
304 fgA-+y  
Chapter 7  Equivalent Currents +KTHZpp!c2  
305 Bq-}BN?pz  
Chapter [4yw? U  
7  Equivalent Currents 0q]0+o*%  
7.1  Introduction HRCnjem/v\  
7.1  Introduction 4`o<e)c3  
305 /*"pylm  
Equivalent Currents for Edge Diffraction u2[L^]|  
7.2  Equivalent Currents for Edge Diffraction Vkf{dHjW  
306 ~g@}A  
7.2 I;UT;/E2  
7.3  Radiation From Equivalent Currents PH^Gj
m  
7.3  Radiation From Equivalent Currents 0xeY0!ux  
312 N>)Db  
Reflected Fields Using Equivalent Currents e;|$nw-  
7.4  Reflected Fields Using Equivalent Currents ^/}&z  
322 #\K"FE0PGz  
7.4 <LJb,l"  
Problems R`Hy0;X  
Problems +A$>F@u  
327 2^rJ|Ni  
References .F$cR^i5u  
References ^HE@ [b  
328 Czy}~;_Ay  
Chapter 8  Diffraction at a Smooth Convex Conducting Surface >V\^oh)t]t  
Chapter I_R6 M1  
8  Diffraction at a Smooth Convex Conducting Surface f)r6F JLU  
331 b9v<Jk  
8.1  The Phenomenon of Creeping Waves, or Curved Surface tCwB7c-  
8.1  The Phenomenon of Creeping Waves, or Curved Surface  &Du S*  
Diffraction
Cm"S=gV  
Diffraction Otf{)f  
331 V&Rwj_Y  
8.1.1  Introduction Nz;\PS  
331 l<7SB5  
8.1.1  Introduction rP!GS _RG  
8.1.2  Asymptotic Evaluation of Eigenfunction Solutions for ID{XZ  
Asymptotic Evaluation of Eigenfunction Solutions for B;piO-hH  
8.1.2 @a 7U0$,O#  
Line Source Illumination of a Conducting Circular g^\!> i  
Line Source Illumination of a Conducting Circular .2ZFJ.Z"  
Cylinder W|s";EAM  
Cylinder U: )Gc  
332 eYu0")  
8.1.3  Interpretation of the Asymptotic Solution in Terms of NnU`u.$D  
8.1.3  Interpretation of the Asymptotic Solution in Terms of ekmWYQ ~  
Surface Rays 5/CF_v  
Surface Rays )ac!@slb^7  
335 K7nyQGS  
8.1.4  Invocation of Locality and the Generalized Fermat xZ>j Q_}  
8.1.4 J`{o`>  
Invocation of Locality and the Generalized Fermat $>+g)  
Principle O,NVhU7,  
336 hp2$[p6O  
Principle S a
}P |qI  
8.1.5  The Significance of the UTD Results for Diffraction by d..JW{  
8.1.5  The Significance of the UTD Results for Diffraction by uW!saT5o  
Smooth Convex Surfaces  341 {9^p3Q+:P  
Smooth Convex Surfaces v?%vB#A^  
8.1.6  Problem Classes for Curved-Surface Diffraction  343 #ZP;] W  
8.1.6  Problem Classes for Curved-Surface Diffraction 3 4&xh1=3  
8.1.7  Differential Geometry for 2D Curved-Surface Diffraction  344 Jz P0D'  
8.1.7  Differential Geometry for 2D Curved-Surface Diffraction Ea-U+7JC  
8.2  The Two-Dimensional Scattering Formulation  344 aEVy20wd  
The Two-Dimensional Scattering Formulation {.y_{yWo  
8.2.1  The Scattering Problem Geometry  344 +!$`0v
  
8.2.1  The Scattering Problem Geometry {l
giH+:  
8.2.2  UID Scattering Solution in the Lit Region  345 :l?mNm5  
8.2.2  UTD Scattering Solution in the Lit Region >6)|>#Wi  
8.2.3  UTD Scattering Solution in the Shadow Region  350 deTD|R  
8.2.3  UTD Scattering Solution in the Shadow Region OkCAvRg  
8.2.4  Field Continuity at the SSB  356 #5{BxX&\  
Field Continuity at the SSB <~
:2~r  
8.2.4 lXzm)  
8.2.5  UID Scattering Solution in the Surface-Based Ray K{B|  
8.2.5  UTD Scattering Solution in the Surface-Based Ray  =+q\Jh  
370 <vD(,||  
Coordinate System d9%P[(yM^
 
Coordinate System  Wu8^Z Z{  
8.3  The Radiation Problem for a Source Mounted on a Smooth qL[SwEc  
The Radiation Problem for a Source Mounted on a Smooth AD@ {7  
Convex Conducting Surface 'G>9iw  
374 6GqC]rd*:  
Convex Conducting Surface a(ml#-M  
8.3.1  The Radiation Problem Geometry  374 >vO+k^'Y  
8.3.1  The Radiation Problem Geometry %}XyzGq{
  
8.3.2  Sources of the Radiated Fields  375 :-$8u;!M  
8.3.2  Sources of the Radiated Fields B<a` o&?  
8.3.3  UTD Solution for the Radiation Problem: Observation k_Y7<z0G  
8.3.3  UTD Solution for the Radiation Problem: Observation @g]EY&Uzl  
Point Ed2A\S6tl  
in the Lit Zone  377
-*Th=B-  
Point in the Lit Zone J(wFJg\/  
8.3.4  UTD Solution for the Radiation Problem: Observation Ps[#z@5{x  
UTD Solution for the Radiation Problem: Observation k1s5cg=n(  
8.3.4 )+w1nw|m  
in the Shadow Zone  381 4%I[.dBnM  
Point fc[_~I'  
Point in the Shadow Zone aUA)p}/:  
8.3.5  Noninfinitesimal Sources  385 ZE~zs~z|  
8.3.5  Noninfinitesimal Sources k,f/9e+#  
8.3.6  Deep Shadow Zone Field Expressions and Their ,H^!G\  
Deep Shadow Zone Field Expressions and Their x($Djx  
8.3.6 S2nX{=  
387 =q`T|9v  
Interpretation Fmz+ Xb  
Interpretation ]]3rSXs2}J  
8.4  The Two-Dimensional Convex Conducting Surface Coupling /H3w7QU  
The Two-Dimensional Convex Conducting Surface Coupling (mKH,r  
Problem f*9O39&|  
401 ;K%/sIIke  
Problem S kB*w'k  
8.4.1  Detailed Geometry for the Coupling Problem  401  _+(@?  
8.4.1  Detailed Geometry for the Coupling Problem P|]r*1^5  
8.4.2  Preliminaries  401 y~VI,82*  
8.4.2  Preliminaries NK(_ &.F
 
8.4.3  UID Coupling Solution for Magnetic Current Sources  402 /SQ/$`1{  
8.4.3  UTD Coupling Solution for Magnetic Current Sources ;oDr8a<A  
8.4.4  UTD Coupling Solution for Electric Current Sources  403 e0otr_)3F  
8.4.4  UTD Coupling Solution for Electric Current Sources 8F@Sy,D  
8.4.5  Special Geometries  403 \k{[HfVvn  
8.4.5  Special Geometries ZmNNR 1%/  
8.4.6  A Form of the Coupling Solution in the Deep Shadow 3dolrW  
8.4.6  A Form of the Coupling Solution in the Deep Shadow siT`O z|,  
Regiop. and Its Interpretation  405 G#^0Bh&  
Region and Its Interpretation .`V$j.a  
8.5  Bibliographic Remarks  408 %H2ios[UO  
Bibliographic Remarks JY^i  
Problems  409 ~131|e`C  
Problems nAAv42j[  
References  410 k}NM]9EAE  
References 5Dz$_2oM3  
Appendix A  Unit Vectors  413 het<#3Bo  
Appendix A Unit Vectors 6 .)Xeb"  
A.1  Cartesian Coordinate System  413 sf# px|~9  
I  Cartesian Coordinate System K}^#VlY9  
A. GG +
T-  
A.2  Spherical Coordinate System  413 AQT_s9"0  
A.2  Spherical Coordinate System %~gI+0HK  
A.3  Cylindrical Coordinate System  414 |r36iUHZS  
A.3  Cylindrical Coordinate System

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