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标题:
请问FindRoot外面套一个For循环的问题
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作者:
cxy623157929
时间:
2015-6-2 12:57
标题:
请问FindRoot外面套一个For循环的问题
lamda = 1.55 10^-6;
: I4 R% s3 \6 x2 j% A' R4 B
k0 = 2*Pi/lamda;
4 G) B2 `" l- U' \" I4 _
n1 = 1.4677;(*纤芯折射率*)
/ X( ~' O! G% ~4 q9 g; h
n2 = 1.4628;(*包层折射率*)
$ k; P$ y. b q) `3 @1 M* k
n3 = 0.469 + 9.32*I;(*银折射率*)
/ ]( l6 ~* j, |7 \- K* a
a1 = 4.1 10^-6;(*纤芯半径*)
' e4 I: k; e4 A2 m' A
a2 = 62.5 10^-6;(*包层半径*)
4 `5 P8 t" Y5 u, r4 S" r+ j Z4 u
d = 40 10^-9;(*金属厚度*)
# z. J$ h) z% a+ ~( g
a3 = a2 + d;
' d2 g4 c2 c2 o8 o( q
mu = Pi*4 10^-7;(*真空磁导率*)
& E* P m z& k/ ~1 L; h- U
epsi0 = 8.85 10^-12;(*介电常数*)
: n, k+ f6 k% w
$ R7 b7 m6 C0 k5 h u, a
n4 = 1.330;
$ C, v! p' _! r) B5 ?
2 t. Y D1 Z6 V6 K& x8 k, M: Y
neffcl = neffclre + neffclim*I;
. T0 O% e- T" X, w, p. ~
* m( I+ ~7 g; k0 D
betacl = k0*neffcl;
) f4 b# k2 k S4 g
omega = 2*Pi*299792458/lamda;
: a# a/ h; _+ s+ p
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epsi1 = n1^2*epsi0;
3 H" n& A: N: c4 T7 M
epsi2 = n2^2*epsi0;
7 ^" b% T: D2 W8 n5 E3 ~1 V
epsi3 = n3^2*epsi0;
5 d$ P" J4 A2 \% Z# c4 A; M9 i, o
epsi4 = n4^2*epsi0;
; x% T4 v- e4 t
}! m+ Y' c+ o
u1 = k0*Sqrt[neffcl^2 - n1^2];
' i+ S& J4 H8 z0 g" y& |+ b+ Y
u2 = k0*Sqrt[neffcl^2 - n2^2];
' D- ~6 @, ?& [, k9 p- b
u3 = k0*Sqrt[neffcl^2 - n3^2];
7 G" b+ W' { [
w4 = k0*Sqrt[neffcl^2 - n4^2];
9 w- l+ H9 Q/ R5 b, N4 {, Y
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Iua111 = BesselI[1, u1*a1];
& L, f& o' [. w
Iua121 = BesselI[1, u2*a1];
) u; L4 s, _6 O9 l/ ~
Iua122 = BesselI[1, u2*a2];
) C0 I' p* m) u6 |
Iua132 = BesselI[1, u3*a2];
1 N0 v3 K) u( ^: d' ~
Iua133 = BesselI[1, u3*a3];
: M, F3 G; Q2 u5 v4 K1 \( g
IIua111 = (BesselI[0, u1*a1] + BesselI [2, u1*a1])/2;
0 c" L( i9 Y O6 f6 `4 G
IIua121 = (BesselI [0, u2*a1] + BesselI [2, u2*a1])/2;
. T" F5 M; z' P5 w9 c) G
IIua122 = (BesselI[0, u2*a2] + BesselI[2, u2*a2])/2;
& E. o b2 A9 s3 Z1 z
IIua132 = (BesselI[0, u3*a2] + BesselI[2, u3*a2])/2;
& u: |0 g& X' ^5 B" ~3 Y+ Z
IIua133 = (BesselI[0, u3*a3] + BesselI[2, u3*a3])/2;
' j# ?2 s2 ~3 J1 u1 a5 Q3 {; w
0 z, T2 a! o5 k9 S% a6 B* @
Kua121 = BesselK [1, u2*a1];
_9 S7 t# [% q6 @: b) W
Kua122 = BesselK [1, u2*a2];
5 n% S$ c7 S8 H
Kua132 = BesselK [1, u3*a2];
; ]3 Q& V9 h, J& P+ L* u* P
Kua133 = BesselK [1, u3*a3];
2 t1 M3 d+ G& O- B. d! Q
Kwa143 = BesselK [1, w4*a3];
. _+ W- J9 J: N0 I9 G% J! J' }
KKua121 = -(BesselK [0, u2*a1] + BesselK [2, u2*a1])/2;
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KKua122 = -(BesselK [0, u2*a2] + BesselK [2, u2*a2])/2;
a+ }) r4 h) r: A
KKua132 = -(BesselK [0, u3*a2] + BesselK [2, u3*a2])/2;
; w8 n+ N" N! b9 }4 F9 B
KKua133 = -(BesselK [0, u3*a3] + BesselK [2, u3*a3])/2;
7 j. o4 M" g3 {1 I
KKwa143 = -(BesselK [0, w4*a3] + BesselK [2, w4*a3])/2;
) Z/ _" J/ |9 I# c
" l' _5 x! Q' W* V1 K$ ?
H1 = (betacl*Kwa143*
I0 l! S% p9 O# B( n
Kua133*(w4^2/u3^2 - 1)/omega/epsi4/u3/a3)*(u3/u2*IIua132*
! O# ?% s R% v& Q9 n$ C4 J0 K
Kua122 - u3^2/u2^2*Iua132*KKua122) - (betacl*Kwa143*
n, a. e7 w7 l
Iua133*(w4^2/u3^2 - 1)/omega/epsi4/u3/a3)*(u3/u2*KKua132*
1 H# x/ Q2 n2 Y
Kua122 - u3^2/u2^2*Kua132*KKua122) + (betacl*Iua132*
2 O* e d- @ o. o+ J% ~( s2 N/ e
Kua122*(u3^2/u2^2 - 1)/omega/epsi3/u2/a2)*(w4/u3*KKwa143*
J2 w# C4 g1 |: n. R
Kua133 - w4^2*epsi3/u3^2/epsi4*Kwa143*KKua133) - (betacl*
8 w7 A' }; O+ ~
Kua132*Kua122*(u3^2/u2^2 - 1)/omega/epsi3/u2/a2)*(w4/u3*KKwa143*
; |( E. h% o& W( v( T. w ^3 y& z2 ]
Iua133 - w4^2*epsi3/u3^2/epsi4*Kwa143*IIua133);
4 A5 [! M. J. I3 K. s
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H2 = (betacl*Kwa143*
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Kua133*(w4^2/u3^2 - 1)/omega/epsi4/u3/a3)*(u3/u2*IIua132*
0 x/ a, a0 x) I: J4 U
Iua122 - u3^2/u2^2*Iua132*IIua122) - (betacl*Kwa143*
2 o0 e, J2 R6 ~; T3 a6 d) v- d
Iua133*(w4^2/u3^2 - 1)/omega/epsi4/u3/a3)*(u3/u2*KKua132*
! E# U& q0 T' I# F! G
Iua122 - u3^2/u2^2*Kua132*IIua122) + (betacl*Iua132*
: i. W6 W; ^' N0 {; \
Iua122*(u3^2/u2^2 - 1)/omega/epsi3/u2/a2)*(w4/u3*KKwa143*
4 O$ E9 T. @* }. p1 i
Kua133 - w4^2*epsi3/u3^2/epsi4*Kwa143*KKua133) - (betacl*
+ r1 q D& D" J9 P) C0 _: `
Kua132*Iua122*(u3^2/u2^2 - 1)/omega/epsi3/u2/a2)*(w4/u3*KKwa143*
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Iua133 - w4^2*epsi3/u3^2/epsi4*Kwa143*IIua133);
% h. f7 d; I- e$ y2 z
k: t% {# U" `! u& d( f5 Q
H3 = (betacl*Iua132*Kua122*(u3^2/u2^2 - 1)/omega/mu/u2/a2)*(betacl*
* E5 a, Y- u. l
Kwa143*Kua133*(w4^2/u3^2 - 1)/omega/epsi4/u3/a3) - (betacl*
# j5 k W5 B. d
Kua132*Kua122*(u3^2/u2^2 - 1)/omega/mu/u2/a2)*(betacl*Kwa143*
4 W. A0 v1 ~0 I! h
Iua133*(w4^2/u3^2 - 1)/omega/epsi4/u3/a3) + (u3/u2*IIua132*
8 i, X6 V8 w9 K) }1 u6 H! l0 m
Kua122 -
# I7 Y; h5 b! T( u4 p3 W
u3^2*epsi2/u2^2/epsi3*Iua132*KKua122)*(w4/u3*KKwa143*Kua133 -
~, C4 F% Z, X
w4^2*epsi3/u3^2/epsi4*Kwa143*KKua133) - (u3/u2*KKua132*Kua122 -
' b4 x! R3 N/ I
u3^2*epsi2/u2^2/epsi3*Kua132*KKua122)*(w4/u3*KKwa143*Iua133 -
' D( O3 I( O4 {9 s' ]0 n# V
w4^2*epsi3/u3^2/epsi4*Kwa143*IIua133);
4 A! o7 l( R, B1 t& d
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H4 = (betacl*Iua132*Iua122*(u3^2/u2^2 - 1)/omega/mu/u2/a2)*(betacl*
, [0 i% B, q" Z+ x. k
Kwa143*Kua133*(w4^2/u3^2 - 1)/omega/epsi4/u3/a3) - (betacl*
( @- m# x$ c+ T8 i( _
Kua132*Iua122*(u3^2/u2^2 - 1)/omega/mu/u2/a2)*(betacl*Kwa143*
' E+ Q# L; t, D6 f
Iua133*(w4^2/u3^2 - 1)/omega/epsi4/u3/a3) + (u3/u2*IIua132*
! d' M: K! a& W. B e( M
Iua122 -
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u3^2*epsi2/u2^2/epsi3*Iua132*IIua122)*(w4/u3*KKwa143*Kua133 -
% D' [. Y9 V2 D2 g- l
w4^2*epsi3/u3^2/epsi4*Kwa143*KKua133) - (u3/u2*KKua132*Iua122 -
7 f8 {' g* U _. [( ~ o
u3^2*epsi2/u2^2/epsi3*Kua132*IIua122)*(w4/u3*KKwa143*Iua133 -
# {2 k$ z. ]6 b; `
w4^2*epsi3/u3^2/epsi4*Kwa143*IIua133);
& C3 c1 N- ?9 e! p3 E
( A* e0 T# ~6 ~$ P* W
M1 = (betacl*Iua132*Kua122*(u3^2/u2^2 - 1)/omega/epsi3/u2/a2)*(betacl*
3 W# @4 J+ B+ E$ }
Kwa143*Kua133*(w4^2/u3^2 - 1)/omega/mu/u3/a3) - (betacl*Kua132*
. B, f9 ]6 ?# ~
Kua122*(u3^2/u2^2 - 1)/omega/epsi3/u2/a2)*(betacl*Kwa143*
( R& H* _( c# r
Iua133*(w4^2/u3^2 - 1)/omega/mu/u3/a3) + (u3/u2*IIua132*Kua122 -
0 U( D4 u$ i8 e- \" N* E1 r
u3^2/u2^2*Iua132*KKua122)*(w4/u3*KKwa143*Kua133 -
% V% n0 P! x) R: y' T
w4^2/u3^2*Kwa143*KKua133) - (u3/u2*KKua132*Kua122 -
" q4 {; i4 P. k
u3^2/u2^2*Kua132*KKua122)*(w4/u3*KKwa143*Iua133 -
3 U. a( X% o" e' t) B
w4^2/u3^2*Kwa143*IIua133);
- T4 |# s2 l0 j
% e. D, j" ?1 @7 n
M2 = (betacl*Iua132*Iua122*(u3^2/u2^2 - 1)/omega/epsi3/u2/a2)*(betacl*
/ ~, S7 {% Y, d, [- i7 Z
Kwa143*Kua133*(w4^2/u3^2 - 1)/omega/mu/u3/a3) - (betacl*Kua132*
& i$ K* ]: W$ w, e
Iua122*(u3^2/u2^2 - 1)/omega/epsi3/u2/a2)*(betacl*Kwa143*
. R5 f+ B0 D* Y2 @
Iua133*(w4^2/u3^2 - 1)/omega/mu/u3/a3) + (u3/u2*IIua132*Iua122 -
9 M+ @0 k3 v! q$ i& N* a
u3^2/u2^2*Iua132*IIua122)*(w4/u3*KKwa143*Kua133 -
+ a% G/ [2 l. U6 l; v$ y- c" e7 q
w4^2/u3^2*Kwa143*KKua133) - (u3/u2*KKua132*Iua122 -
* ]1 D; Y8 s9 n
u3^2/u2^2*Kua132*IIua122)*(w4/u3*KKwa143*Iua133 -
& Z- f& C' G' v, f) p3 V
w4^2/u3^2*Kwa143*IIua133);
. a: z! n; C9 F* M. c8 w4 V) D
0 G2 S5 b/ H/ G# Y5 B
M3 = (betacl*Kwa143*
5 X7 z' F: S6 Q( F6 X
Kua133*(w4^2/u3^2 - 1)/omega/mu/u3/a3)*(u3/u2*IIua132*Kua122 -
6 W- ~7 F: X0 g. o* d, c$ A
u3^2*epsi2/u2^2/epsi3*Iua132*KKua122) - (betacl*Kwa143*
Y/ y, s+ L2 c, P. J4 T" K8 U! d
Iua133*(w4^2/u3^2 - 1)/omega/mu/u3/a3)*(u3/u2*KKua132*Kua122 -
, [9 P; Q+ _. W
u3^2*epsi2/u2^2/epsi3*Kua132*KKua122) + (betacl*Iua132*
8 o$ Q& V, z. {! a" b. Z
Kua122*(u3^2/u2^2 - 1)/omega/mu/u2/a2)*(w4/u3*KKwa143*Kua133 -
! F5 O! A9 B9 X" g4 `+ c0 S
w4^2/u3^2*Kwa143*KKua133) - (betacl*Kua132*
4 S2 w# @ b* n" O6 D7 D
Kua122*(u3^2/u2^2 - 1)/omega/mu/u2/a2)*(w4/u3*KKwa143*Iua133 -
& ] C" K1 n" r
w4^2/u3^2*Kwa143*IIua133);
; b: \1 c7 e( k
6 ^1 Y- h+ q# P8 @: m
M4 = (betacl*Kwa143*
?& [6 W7 M% v' g# b
Kua133*(w4^2/u3^2 - 1)/omega/mu/u3/a3)*(u3/u2*IIua132*Iua122 -
# @" h! d: ^0 e
u3^2*epsi2/u2^2/epsi3*Iua132*IIua122) - (betacl*Kwa143*
7 R# {/ s' L5 \' b3 c, m; g' A
Iua133*(w4^2/u3^2 - 1)/omega/mu/u3/a3)*(u3/u2*KKua132*Iua122 -
7 r5 }- o d% j8 k+ N) ^
u3^2*epsi2/u2^2/epsi3*Kua132*IIua122) + (betacl*Iua132*
- U! B, n, f, B
Kua122*(u3^2/u2^2 - 1)/omega/mu/u2/a2)*(w4/u3*KKwa143*Kua133 -
! F6 X( a' O6 s
w4^2/u3^2*Kwa143*KKua133) - (betacl*Kua132*
. Y5 J4 K% `2 ]% D+ q& }0 N. w5 y
Iua122*(u3^2/u2^2 - 1)/omega/mu/u2/a2)*(w4/u3*KKwa143*Iua133 -
1 ~) ?- {( Q) r5 p+ e" s
w4^2/u3^2*Kwa143*IIua133);
# B" m1 r' T# q; e
$ ^+ l! @' d; N
R1 = u2^2/u1^2*Iua121*IIua111 - u2/u1*IIua121*Iua111;
& J% I; p* j+ f; X) c
T1 = u2^2/u1^2*Kua121*IIua111 - u2/u1*KKua121*Iua111;
7 H; m0 R4 s: r8 d- w: @4 t
U1 = betacl*Iua121*Iua111*(u2^2/u1^2 - 1)/omega/epsi2/u1/a1;
5 Y: b5 Y6 X# x& P) Z$ M0 I
V1 = betacl*Kua121*Iua111*(u2^2/u1^2 - 1)/omega/epsi2/u1/a1;
) Q! K! J1 d* H9 x6 B
' i: q, _& i' l: t
R2 = u2^2/u1^2*epsi1/epsi2*Iua121*IIua111 - u2/u1*IIua121*Iua111;
x [2 t' ]( S7 u+ d5 J, b
T2 = u2^2/u1^2*epsi1/epsi2*Kua121*IIua111 - u2/u1*KKua121*Iua111;
; x/ q$ P$ v; ]( u* d7 o
U2 = betacl*Iua121*Iua111*(u2^2/u1^2 - 1)/omega/mu/u1/a1;
2 L+ b g4 k7 R' x" s- g6 t$ q9 L6 j
V2 = betacl*Kua121*Iua111*(u2^2/u1^2 - 1)/omega/mu/u1/a1;
" R& f3 o3 b. o# F" h
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xicl1 = (-R1*H1 + T1*H2 + U1*H3 - V1*H4)/(R1*M1 - T1*M2 - U1*M3 +
8 j2 S6 W. y7 B* F- _
V1*M4);
! }4 U5 h u' c- M% j& j% Q
xicl2 = (-R2*H3 + T2*H4 + U2*H1 - V2*H2)/(R2*M3 - T2*M4 - U2*M1 +
/ o* {0 ?8 L/ u8 n& ]8 K: F
V2*M2);
3 g) [( V: F$ s: k% L3 x: D& R
7 S. ?8 l- p! ]
x = xicl1 - xicl2;
2 A+ a2 e0 A+ R7 z1 S" u) Z8 g
x1 = Re[x];
0 i/ N1 I1 j% R
x2 = Im[x];
/ d+ a6 M3 K1 U h4 g
) R3 G0 [; v, g
FindRoot[{x1,x2},{{neffclre,1.333},{neffclim,0.00001}}];
$ k* E; t% p( N; k t/ R
]
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复制代码
代码如上,结果是{neffclre -> 1.33017, neffclim -> 0.0000172055}
5 V) _' k, w0 W3 `' f
但我把
FindRoot[{x1,x2},{{neffclre,1.333},{neffclim,0.00001}}];
) C5 d; A1 _- `4 W3 P6 d/ S
换成
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For[i = 1, i < 133, i++, neffclbase = 1.330 + 0.001*i;
h8 N4 P3 {! M; j6 W) d! T
FindRoot[{x1, x2}, {{neffclre, neffclbase}, {neffclim, 0.00001}}];
% w: D. _5 w: v, a" Q& N$ i
]
, ^% t$ _) s: U+ G2 `, g% r
就会出现
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FindRoot::lstol: 线搜索把步长降低到由 AccuracyGoal 和 PrecisionGoal 指定的容差范围内,但是无法找到 merit 函数的充足的降低. 您可能需要多于 MachinePrecision 位工作精度以满足这些容差.
2 |. K, G) E& a4 q% Y4 {0 ?; r
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请问是怎么回事?
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