Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of...

33
1 Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie I (NFT I) / 8th Lecture / 8. Vorlesung Universität Kassel Fachbereich Elektrotechnik / Informatik (FB 16) Fachgebiet Theoretische Elektrotechnik (FG TET) Wilhelmshöher Allee 71 Büro: Raum 2113 / 2115 D-34121 Kassel Dr.-Ing. René Marklein [email protected] http://www.tet.e-technik.uni-kassel.de http://www.uni-kassel.de/fb16/tet/marklein/index.html University of Kassel Dept. Electrical Engineering / Computer Science (FB 16) Electromagnetic Field Theory (FG TET) Wilhelmshöher Allee 71 Office: Room 2113 / 2115 D-34121 Kassel

Transcript of Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of...

Page 1: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

1

Num

eric

al M

etho

ds o

f El

ectr

omag

netic

Fie

ld T

heor

y I (

NFT

I)N

umer

isch

e M

etho

den

der

Elek

trom

agne

tisch

en F

eldt

heor

ie I

(NFT

I) /

8th

Lect

ure

/ 8.

Vorle

sung

Univ

ersi

tät K

asse

lFa

chbe

reic

h El

ektr

otec

hnik

/ In

form

atik

(F

B 16

)Fa

chge

biet

The

oret

isch

e El

ektr

otec

hnik

(F

G T

ET)

Wilh

elm

shöh

er A

llee

71Bü

ro: R

aum

211

3 /

2115

D-3

4121

Kas

selDr.

-Ing

. Ren

éM

arkl

ein

mar

klei

n@un

i-ka

ssel

.de

http

://w

ww

.tet.e

-tec

hnik

.uni

-kas

sel.d

eht

tp:/

/ww

w.u

ni-k

asse

l.de/

fb16

/tet

/mar

klei

n/in

dex.

htm

l

Univ

ersi

ty o

f Kas

sel

Dep

t. El

ectr

ical

Eng

inee

ring

/ Co

mpu

ter

Scie

nce

(FB

16)

Elec

trom

agne

tic F

ield

The

ory

(FG

TET

)W

ilhel

msh

öher

Alle

e 71

Off

ice:

Roo

m 2

113

/ 21

15D

-341

21 K

asse

l

Page 2: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

2

3-D

FD

TD –

Der

ivat

ion

of th

e D

iscr

ete

Equa

tions

/

3D-F

DTD

–Ab

leitu

ng d

er d

iskr

eten

Gle

ichu

ngen

The

first

two

Max

wel

l’s E

quat

ions

are

in d

iffer

entia

l for

m /

D

ie e

rste

n be

iden

Max

wel

lsch

en G

leic

hung

en la

uten

in D

iffer

entia

lform

:

m e

(,)

(,)

(

,)

(,)

(,

) (

,)

tt

tt

tt

tt∂

=−∇

−∂ ∂

=∇

−∂

BR

×ER

JR

DR

×HR

JR

In C

arte

sian

Coo

rdin

ates

we

find

for

the

Curl

oper

ator

app

lied

to E

and

H /

Im

Kar

tesi

sche

n Ko

ordi

nate

nsys

tem

find

en w

ir fü

r de

n Ro

tatio

nsop

erat

or a

ngew

ende

t auf

E u

nd H

:

(,)

(,

)(

,)(

,)

(,)

(,

)(

,)(

,)

(,)

(,)

(,)

(,

)(

,)

(,

)

(,)

(,

)

xy

y

xy

z

yy

xx

zz

xy

z

xy

y

xy

z

yz

tx

yz

Et

Et

Et

Et

Et

Et

Et

Et

Et

yz

zx

xy

tx

yz

Ht

Ht

Ht

Ht

Ht

y

∂∂

∂∇

=∂

∂∂

∂∂

∂∂

∂∂

=−

+−

+−

∂∂

∂∂

∂∂

∂∂

∂∇

=∂

∂∂

∂∂

=−

∂ee

e

×ER

RR

R

RR

RR

RR

ee

e

ee

e

×HR

RR

R

RR

(,)

(,)

(,)

(,)

yx

xz

xy

zH

tH

tH

tH

tz

zx

xy

∂∂

+−

+−

∂∂

∂∂

RR

RR

ee

e

Page 3: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

3

3-D

FD

TD –

Der

ivat

ion

of th

e D

iscr

ete

Equa

tions

/

3D-F

DTD

–Ab

leitu

ng d

er d

iskr

eten

Gle

ichu

ngen

If w

e in

sert

the

last

exp

ress

ions

into

the

first

two

Max

wel

l’s e

quat

ions

are

in d

iffer

entia

l for

m r

ead

/ W

enn

wir

die

letz

ten

Ausd

rück

e in

the

erst

en b

eide

n M

axw

ells

chen

Gle

ichu

ngen

in D

iffer

entia

lform

ein

setz

en,

erha

lten

wir:

m(

,)

(,

) (

,)

(,

)(

,)

(,

)

(,

)(

,)

(,

)(

,)

(,

)(

,)

xy

zx

yz

yy

xx

zz

xy

z

tt

tt

Bt

Bt

Bt

tE

tE

tE

tE

tE

tE

ty

zz

xx

y

∂=−∇

−∂ ∂

+

+

∂∂

∂∂

=−

−+

−+

∂∂

∂∂

BR

×ER

JR

Re

Re

Re

RR

RR

RR

ee

e

mm

m

e

(

,)

(,

)(

,)

(,

)

(

,)

(,

)

(,

)(

,)

(,

)

(,

)(

,)

(,

)

xy

zx

yz

xy

zx

yz

yx

zx

Jt

Jt

Jt

tt

tt

Dt

Dt

Dt

tH

tH

tH

ty

zz

−+

+

∂=

∇−

∂ ∂

+

+

∂=

−+

∂∂

Re

Re

Re

DR

×HR

JR

Re

Re

Re

RR

Re

ee

e

(,

)(

,)

(,

)

(,

)(

,)

(,

)

yx

zy

z

xy

zx

yz

Ht

Ht

Ht

xx

y

Jt

Jt

Jt

∂∂

−+

∂∂

−+

+

RR

Re

e

Re

Re

Re

Six

deco

uple

d sc

alar

equ

atio

ns! /

Se

chs

entk

oppe

lte s

kala

re G

leic

hung

en!

Page 4: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

4

3-D

FD

TD –

Der

ivat

ion

of th

e D

iscr

ete

Equa

tions

/

3D-F

DTD

–Ab

leitu

ng d

er d

iskr

eten

Gle

ichu

ngen

If w

e in

sert

the

last

exp

ress

ions

into

the

first

two

Max

wel

l’s e

quat

ions

are

in d

iffer

entia

l for

m w

e re

ad /

W

enn

wir

die

letz

ten

Ausd

rück

e in

die

ers

ten

beid

en M

axw

ells

chen

Gle

ichu

ngen

in D

iffer

entia

lform

ei

nset

zen,

erh

alte

n w

ir:

m m m e

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)

(,

)

(

yz

xx

xz

yy

yx

zz

yz

xx

y

Et

Et

Bt

Jt

ty

z

Et

Et

Bt

Jt

tz

xE

tE

tB

tJ

tt

xy

Ht

Ht

Dt

Jt

ty

z

D t

∂=−

−−

∂∂

∂∂

=−

−−

∂∂

∂=−

−−

∂∂

∂=

−−

∂∂

∂ ∂

RR

RR

RR

RR

RR

RR

RR

RR

Re e

(,

)(

,)

,)

(

,)

(,

)(

,)

(,

)

(,

)

xz

y

yx

zz

Ht

Ht

tJ

tz

xH

tH

tD

tJ

tt

xy

∂∂

=−

∂=

−−

∂∂

RR

R

RR

RR

Page 5: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

5

3-D

FD

TD –

Der

ivat

ion

of th

e D

iscr

ete

Equa

tions

/

3D-F

DTD

–Ab

leitu

ng d

er d

iskr

eten

Gle

ichu

ngen

m m m e

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)(

,)

(,

)

(,

)

yz

xx

xz

yy

yx

zz

yz

xx

Et

Et

Ht

Jt

ty

z

Et

Et

Ht

Jt

tz

xE

tE

tH

tJ

tt

xy

Ht

Ht

Et

Jt

ty

z

tµ µ µ ε

∂=−

−−

∂∂

∂∂

=−

−−

∂∂

∂=−

−−

∂∂

∂=

−−

∂∂

∂ ∂

RR

RR

RR

RR

RR

RR

RR

RR

e e

(,

)(

,)

(,

)

(,

)

(,

)(

,)

(,

)

(,

)

xz

yy

yx

zz

Ht

Ht

Et

Jt

zx

Ht

Ht

Et

Jt

tx

y

ε ε

∂∂

=−

∂=

−−

∂∂

RR

RR

RR

RR

xEyE

zE

xH

zH

yH

m e

,1,

2,3

,1,

2,3

ii

ii

xx

xx

HJ

i

EJ

i

==

==

(,

)(

,)

(,

)(

,)

(,

)(

,)

xx

yy

zz

Bt

Ht

Bt

Ht

Bt

Ht

µ µ µ

= = =

RR

RR

RR

(,

)(

,)

(,

)(

,)

(,

)(

,)

xx

yy

zz

Dt

Et

Dt

Et

Dt

Et

ε ε ε

= = =

RR

RR

RR

Cons

titut

ive

equa

tion

for

hom

ogen

eous

isot

ropi

c m

ater

ials

/

Kons

titui

eren

de G

leic

hung

en fü

r ho

mog

ene

isot

rope

Mat

eria

lien:

Page 6: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

6

3-D

FD

TD –

Der

ivat

ion

of th

e D

iscr

ete

Equa

tions

/

3D-F

DTD

–Ab

leitu

ng d

er d

iskr

eten

Gle

ichu

ngen

m(

,)

(,

)(

,)

(,

)y

zx

xE

tE

tH

tJ

ty

=−

−−

∂∂

RR

RR

(,

)(

,)

xx

Ht

Ht

t∂=

∂R

R

()d yE

()b zE

()m x

H

()f zE

()u yE

()

()

()

()

mm (

)(

)2

()

()

2

(,

)()

(,

)()

(,

)()

()

(,

)()

()

mx

x mx

x fb

zz

z

du

yy

y

Ht

Ht

Jt

Jt

Et

Et

Et

yy

y

Et

Et

Et

zz

z

µ= =

∂−

=+

∂−

=+

R R R R

○ ○

()d yE

()b zE

()m x

H(

)f zE

()u yE

()

()

()

()

()

()

m()

()()

()()

()d

uf

by

ym

mz

zx

xE

tE

tE

tE

tH

tJ

ty

−−

=−

+−

∆∆

A pa

rt o

f the

dis

cret

e cu

rl op

erat

or /

Ei

n Te

il de

s di

skre

ten

Rota

tions

oper

ator

s

Page 7: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

7

2-D

EM

Wav

e Pr

opag

atio

n–

2-D

FD

TD –

TM a

nd T

E Ca

se /

2D E

M W

elle

naus

brei

tung

–2D

-FD

TD –

TM-

und

TE-F

all (

)ng

G∈

()n

gG

1xx

= 3zx

=

2-D

TE

Case

/ 2

D-T

E-Fa

ll

Gnn

=

Gn(

)n xE

()n zE

()n y

H

2yx

=(

)ng

G∈

()n

gG

1xx

= 3zx

=

2-D

TM

Cas

e /

2D-T

M-F

all

Gnn

=

Gn

()n x

H

()n z

H(

)n yE

2yx

=

m m

e

(,

)(

,)

(

,)

(,

)(

,)

(,

)

(,

)(

,)

(,

)

(,

)

yx

x

yz

z

xz

yy

xz

Et

Ht

Jt

tz

Et

Ht

Jt

tx

Ht

Ht

Et

Jt

tz

xx

z

µ µ ε

∂∂

=−

∂∂

∂∂

=−

−∂

∂∂

=

−−

∂∂

=

+

RR

R

RR

R

RR

RR

Re

e

m

e e

(,

)(

,)

(,

)(

,)

(,

)(

,)

(

,)

(,

)(

,)

(,

)

xz

yy

yx

x

yz

z

xz

Et

Et

Ht

Jt

tz

x

Ht

Et

Jt

tz

Ht

Et

Jt

tx

xz

µ ε ε

∂∂

=−

−−

∂∂

∂∂

=−

−∂

∂∂

∂=

−∂

∂=

+

RR

RR

RR

R

RR

R

Re

e

GG

Dua

l ort

hogo

nal

grid

sys

tem

in s

pace

/

Dua

l-or

thog

onal

esG

itter

syst

em im

Rau

m

Page 8: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

8

2-D

EM

Wav

e Pr

opag

atio

n–

2-D

FD

TD –

TM C

ase/

2D E

M W

elle

naus

brei

tung

–2D

-FD

TD –

TM-F

all

()n

gG

()n

gG

1xx

= 3zx

=

2-D

TM

Cas

e /

2D-T

M-F

all

Gnn

=

Gn

()n x

H

()n z

H(

)n yE

2yx

=

m

m

e

(,

)(

,)

(,

)

(,

)(

,)

(,

)

(,

)(

,)

(,

)

(,

)

yx

x

yz

z

xz

yy

xz

Et

Ht

Jt

tzE

tH

tJ

tt

x

Ht

Ht

Et

Jt

tz

xx

z

µ µ ε

∂∂

=−

∂∂

∂∂

=−

−∂

∂∂

=

−−

∂∂

=

+RR

R

RR

R

RR

RR

Re

e

Two-

dim

ensi

onal

sta

gger

ed g

rid s

yste

m in

the

2-D

TM

cas

e /

Zwei

dim

ensi

onal

esve

rset

ztes

Gitt

ersy

stem

im2D

-TM

-Fal

l

Page 9: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

9

Impl

emen

tatio

n of

Bou

ndar

y Co

nditi

ons

/ Im

plem

entie

rung

von

Ran

dbed

ingu

ngen

Boun

dary

con

ditio

n fo

r a

perf

ectly

ele

ctric

ally

con

duct

ing

(PEC

)mat

eria

l /

Rand

bedi

ngun

g fü

r ei

n id

eal e

lekt

risch

leite

ndes

Mat

eria

l

(,,

)

(,,

)

01

0

t tny

tt

nyE

nN

E

=

=

ii ii

Plan

e w

ave

boun

dary

con

ditio

n fo

r a

vert

ical

inci

dent

pla

ne w

ave

/ Eb

ene-

Wel

len-

Rand

bedi

ngun

g fü

r ei

ne v

ertik

al e

infa

llend

e eb

ene

Wel

le

(2,

,)

(3,

,)

(1,

,)

(2,

,2)

1 1

zt

zt

xz

tx

zt

nn

nn

yy

zz

Nnn

Nnn

tt

yy

EE

nN

nN

EE

−−

=

≤≤

≤=

PW B

C /

EW-R

BPW

BC

/ EW

-RB

PEC

BC /

IE

L-RB

PEC

BC /

IE

L-RB

Slit

/ Sc

hlitz

PEC

BC /

IE

L-RB

Plan

e w

ave

exci

tatio

n /

Eben

e-W

elle

n-An

regu

ng

Page 10: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

10

2-D

EM

Wav

e Pr

opag

atio

n–

2-D

FD

TD –

TM C

ase/

2D E

M W

elle

naus

brei

tung

–2D

-FD

TD –

TM-F

all

()

0n x

H=

()

0n z

H=

()

0n yE=

Gho

st c

ompo

nent

s w

hich

are

al

loca

ted

outs

ide

the

sim

ulat

ion

area

/

Gei

ster

kom

pone

nten

, wel

che

auße

rhal

b de

s Si

mul

atio

nsge

biet

es

liege

n

Gho

st g

rid c

ells

/

Gei

ster

gitt

erze

llen

Sim

ulat

ion

area

/

Sim

ulat

ions

gebi

et

Page 11: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

11

2-D

EM

Wav

e Pr

opag

atio

n–

2-D

FD

TD –

TM C

ase/

2D E

M W

elle

naus

brei

tung

–2D

-FD

TD –

TM-F

all

Gho

st g

rid c

ells

/

Gei

ster

gitt

erze

llen

Sim

ulat

ion

area

/

Sim

ulat

ions

gebi

et

(2,

,,)

(3,

,,)

zt

zt

nn

nn

yy

EE

=

0yE=

0yE=

0yE=

0yE=

Plan

e w

ave

exci

tatio

n /

Eben

e-W

elle

n-An

regu

ngSl

it /

Schl

itz

Page 12: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

12

2-D

TM

FD

TD –

Diff

ract

ion

on a

Sin

gle

Slit

/2D

-TM

-FD

TD –

Beug

ung

an e

inem

Spa

lt

Page 13: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

13

2-D

TM

FD

TD –

Diff

ract

ion

on a

Sin

gle

Slit

/2D

-TM

-FD

TD –

Beug

ung

am S

palt

Wav

e fie

ld m

ovie

of t

he H

xfie

ld c

ompo

nent

/

Wel

lenf

eldf

ilmde

rH x

-Fel

dkom

pone

nte

Wav

e fie

ld m

ovie

of t

heH z

field

com

pone

nt /

W

elle

nfel

dfilm

der

H z-F

eldk

ompo

nent

e

Wav

e fie

ld m

ovie

of t

heE y

field

com

pone

nt /

W

elle

nfel

dfilm

der

E y-F

eldk

ompo

nent

e

Page 14: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

14

2-D

TM

FD

TD –

Diff

ract

ion

on a

Dou

ble

Slit

/2D

-TM

-FD

TD –

Beug

ung

am D

oppe

lspa

lt

Page 15: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

15

2-D

TM

FD

TD –

Diff

ract

ion

on a

Dou

ble

Slit

/2D

-TM

-FD

TD –

Beug

ung

am D

oppe

lspa

lt

Wav

e fie

ld m

ovie

of t

he H

xfie

ld c

ompo

nent

/

Wel

lenf

eldf

ilmde

rHx-

Feld

kom

pone

nte

Wav

e fie

ld m

ovie

of t

heH z

field

com

pone

nt /

W

elle

nfel

dfilm

der

H z-F

eldk

ompo

nent

e

Wav

e fie

ld m

ovie

of t

heE y

field

com

pone

nt /

W

elle

nfel

dfilm

der

E y-F

eldk

ompo

nent

e

Page 16: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

16

Phot

onic

Cry

stal

s /

Phot

onis

che

Kris

talle

Joan

nopo

ulos

, J. D

., R.

D. M

eade

, J.

N. W

inn:

Phot

onic

Cry

stal

s –

Mol

ding

the

Flow

of

Ligh

t. Pr

ince

ton

Univ

ersi

ty

Pres

s, P

rince

ton,

199

5.

John

son,

S. G

.: Ph

oton

ic C

ryst

als:

The

Ro

ad fr

om T

heor

y to

Pr

actic

e .

Kluw

er A

cade

mic

Pr

ess,

200

1.

Link

s:

Phot

onic

Cry

stal

s Re

sear

ch a

t MIT

Hom

epag

e of

Pro

f. Sa

jeev

John

, Uni

vers

ity o

f Tor

onto

, Can

ada

Page 17: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

17

2-D

TM

FD

TD –

Phot

onic

Cry

stal

s /

2D-T

M-F

DTD

–Ph

oton

isch

e Kr

ista

lle

()

r ()

r

Rela

tive

perm

ittiv

ity o

f the

bac

kgro

und

1

Rela

tive

Perm

ittiv

ität d

es H

inte

rgru

ndes

Rela

tive

perm

ittiv

ity o

f the

rods

11

.4Re

lativ

e Pe

rmitt

ivitä

t der

Stä

be

b r

ε ε

= =

Page 18: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

18

2-D

TM

FD

TD –

Phot

onic

Cry

stal

s /

2D-T

M-F

DTD

–Ph

oton

isch

e Kr

ista

lle

Wav

e fie

ld m

ovie

of t

he H

xfie

ld c

ompo

nent

/

Wel

lenf

eldf

ilmde

rH x

-Fel

dkom

pone

nte

Wav

e fie

ld m

ovie

of t

heH z

field

com

pone

nt /

W

elle

nfel

dfilm

der

H z-F

eldk

ompo

nent

e

Wav

e fie

ld m

ovie

of t

heE y

field

com

pone

nt /

W

elle

nfel

dfilm

der

E y-F

eldk

ompo

nent

e

Page 19: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

19

2-D

TM

FD

TD –

Phot

onic

Cry

stal

s /

2D-T

M-F

DTD

–Ph

oton

isch

e Kr

ista

lle

Wav

e fie

ld m

ovie

of t

he H

xfie

ld c

ompo

nent

/

Wel

lenf

eldf

ilmde

rH x

-Fel

dkom

pone

nte

Wav

e fie

ld m

ovie

of t

heH z

field

com

pone

nt /

W

elle

nfel

dfilm

der

H z-F

eldk

ompo

nent

e

Wav

e fie

ld m

ovie

of t

heE y

field

com

pone

nt /

W

elle

nfel

dfilm

der

E y-F

eldk

ompo

nent

e

Page 20: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

20

2-D

TM

FD

TD –

Phot

onic

Cry

stal

s /

2D-T

M-F

DTD

–Ph

oton

isch

e Kr

ista

lle

Page 21: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

21

2-D

TM

FD

TD –

Phot

onic

Cry

stal

s /

2D-T

M-F

DTD

–Ph

oton

isch

e Kr

ista

lle

Page 22: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

22

FDTD

and

FIT

/ F

DTD

und

FIT

FDTD

:

Fi

nite

Diff

eren

ce T

ime

Dom

ain

/ Fi

nite

Diff

eren

zen

im

Zeitb

erei

chFI

T

:

Fi

nite

Inte

grat

ion

Tech

niqu

e/

Fini

te In

tegr

atio

nste

chni

k

m e

e m

(,

)(

,)

(,

)

(,

)

(,

)(

,)

(,

)(

,)

(,

)(

,)

tt

tt

tt

tt

tt

tt

ρ ρ

∂=−∇

−∂ ∂

=∇

−∂ ∇

=

∇=

BR

×ER

JR

DR

×HR

JR

DR

R

BR

R

i i

m e

e m

d(

,)

(,

)(

,)

d d(

,)

(,

)(

,)

d

(,

)

(,

)

(,

)

(,

)

SC

SS

SC

SS

SV

V

SV

V

tt

tt

tt

tt

ttdV

ttdV

ρ ρ=∂ =∂

=∂ =∂

=−

=−

= =

∫∫∫

∫∫

∫∫∫

∫∫

∫∫∫∫∫

∫∫∫∫∫

BR

dSER

dRJ

RdS

DR

dSHR

dRJR

dS

DR

dSR

BR

dSR

ii

i

ii

i

i i

FDTD

Max

wel

l’s e

quat

ions

in d

iffer

entia

l for

m /

M

axw

ells

che

Gle

ichu

ngen

in D

iffer

entia

lform

FIT

Max

wel

l’s e

quat

ions

in in

tegr

al fo

rm /

M

axw

ells

che

Gle

ichu

ngen

in In

tegr

alfo

rm

0

00

,,

22

(,

) zz

zz

fz

tfz

tfzt

zz

=

∆∆

+−

≈∂

0

00

(,

)d,

2z

z

zz

zfztz

fz

tz

+∆

=

+∆

FD a

ppro

xim

atio

n of

spa

tial a

nd

tem

pora

l der

ivat

ives

/ F

D-

Appr

oxim

atio

n vo

n rä

umlic

hen

und

zeitl

iche

n Ab

leitu

ngen

FIT

appr

oxim

atio

n of

spa

tial a

nd

tem

pora

l int

egra

ls /

FIT

-App

roxi

mat

ion

von

räum

liche

n un

d ze

itlic

hen

Inte

gral

enCe

ntra

l diff

eren

ce a

ppro

xim

atio

n /

Zent

rale

Diff

eren

zen

Appr

oxim

atio

n

Mid

poi

nt r

ule

appr

oxim

atio

n of

a 1

-D in

tegr

al /

M

ittel

punk

tsre

gel-

Appr

oxim

atio

n ei

nes

1D-

Inte

gral

s

Page 23: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

23

Def

initi

on o

f Mat

eria

l Cel

ls /

D

efin

ition

der

Mat

eria

lzel

len

1xx

= 3zx

=2

yx

=1

xx

=

3zx

=

2yx

=

1xn=

xx

nN

=1

yn=

yy

nN

=

zz

nN

=1zn=

()n

mM

ater

ial c

ell /

M

ater

ialz

elle (

)

1

Nn

nM

m=

=∑

()

()

()

()

()

()

nn

N

nn

N

mn

mn

→∈

→∈

εR

ε

νR

ν

()

()

()

11

11

1,2,

,

1

xx

yy

zz

xyz

x yx

zx

y

nM

nM

nM

n

nN

NNN

M MN

MNN

=+

−+

−+

==

= = =

Page 24: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

24

3-D

FIT

–D

eriv

atio

n of

the

Dis

cret

e G

rid E

quat

ions

/

3D-F

IT –

Able

itung

der

dis

kret

en G

itter

glei

chun

gen

dd

dx

SS

R=

=

=

dSn

edR

s

()d yE

()b zE

()m xB

()f zE

()u yE

()d yE

()b zE

()m xB

()f zE

()u yE

md

(,

)(

,)

(,

)d

SC

SS

tt

tt

=∂=−

−∫∫

∫∫∫

BR

dSER

dRJ

RdS

ii

i

()

()

()

()

33

()

33

()

(,

)(

,)d

(,

)d

()d

()xS

S

xS m x

S yz

m x

tdS

tS

BtS

Bt

Sy

zyz

Btyz

yz

yz

=∆∆

= =

=+Ο

∆∆

+∆

=∆∆

∆∆

+∆

∫∫∫∫ ∫∫

∫∫

nBR

eBR

R

ii

1xx

= 3zx

=2

yx

=

1xx

=3

zx

=

2yx

=

inte

grat

ion

cell

/

-In

tegr

atio

nsze

lle(

)m xBI

()m xBI

()

()

()

()

33

()

33

()

(,

)d()

dd

()

mS

Syz

m

ftS

ft

yz

yz

yz

ftyz

yz

yz

=∆∆

=+Ο

∆∆

+∆

=∆∆

∆∆

+∆

∫∫∫∫

R

x∆

z∆

Fiel

d co

mpo

nent

in th

e m

iddl

e /

Feld

kom

pone

nte

in d

er M

itte

Appr

oxim

atio

n er

ror

/ Ap

prox

imat

ions

fehl

er

z∆

y∆

y∆

Page 25: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

25

3-D

FIT

–D

eriv

atio

n of

the

Dis

cret

e G

rid E

quat

ions

/

3D-F

IT –

Able

itung

der

dis

kret

en G

itter

glei

chun

gen

dd

dd

d

dd

x

yy

zz

Syz

Ry

Rz

==

==

==

dSn

edR

se

dRs

e

()d yE

()b zE

()m xB

()f zE

()u yE

md

(,

)(

,)

(,

)d

SC

SS

tt

tt

=∂=−

−∫∫

∫∫∫

BR

dSER

dRJ

RdS

ii

i

1xx

=3

zx

=

2yx

=

inte

grat

ion

cell

/

-In

tegr

atio

nsze

lle(

)m xBI

()m xBI

y∆

z∆

()

()

()

()

()

()

()

()

()

()

()

(,)

(,)

(,)

(

,)(

,)

(,)

d(

,)d

(,)

d(

,)d

(,)

d(

,)d

(

,)d

(,)

d

uf

db

uf

db

uf

d

CS

CC

CC

yz

CC

yz

CC

yz

CC

yz

C

tt

t

tt

ty

tz

ty

tz

Ety

Etz

Ety

Et

=∂=

+

++

=+

−−

=+

−−

∫∫

∫∫

∫∫

∫∫

∫∫

ER

dRER

dRER

dR

ER

dRER

dR

ER

eER

e

ER

eER

e

RR

RR

ii

i

ii

ii

ii

()b

Cz

()u

C

()f

C(

)dC

()b

C

(,

)?

CS

t=∂

=∫

ER

dRi

Page 26: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

26

3-D

FIT

–D

eriv

atio

n of

the

Dis

cret

e G

rid E

quat

ions

/

3D-F

IT –

Able

itung

der

dis

kret

en G

itter

glei

chun

gen

()

()

()

()

(,

)(

,)d

(,

)d(

,)d

(,

)du

fd

by

zy

zC

SC

CC

Ct

Ety

Etz

Ety

Etz

=∂=

+−

−∫

∫∫

∫∫

ER

dRR

RR

Ri

()

() (

)

() (

)

()

()

()

()

()

()

3(

)

3(

)

3(

)

3(

)

3(

)

()

(,

)d()

d

()

(,

)d()

d

()

(

,)d

()d

(

uu

ff

dd

uy

yC

Cy

u y fz

zC

Cz

f z dy

yC

Cy

d y

EtyE

ty

y

Ety

y

EtzE

tz

z

Etz

z

EtyE

ty

y

Et

=∆ =∆ =∆

=+

=∆

+∆

=

+∆

=∆

+∆

=

+∆

=

∫∫

∫∫

∫∫

R R R

() (

)

()

()

()

3

3(

)

3(

)

)

(,

)d()

d

()

bb

bz

zC

Cz

b z

yy

EtzE

tz

z

Etz

z

=∆

∆+

=+

=∆

+∆

∫∫

R

()

()

()

()

3(

)

3(

)

(,

)d()

d

()

uu

mC

Cy

m

ftR

ft

yy

fty

y

=∆

=+

=∆

+∆

∫∫

R○

Fiel

d co

mpo

nent

in th

e m

iddl

e /

Feld

kom

pone

nte

in d

er M

itte

Appr

oxim

atio

n er

ror

/ Ap

prox

imat

ions

fehl

er

()mf

1xx

=3

zx

=

2yx

=

y∆

()u

C

yα=

Page 27: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

27

3-D

FIT

–D

eriv

atio

n of

the

Dis

cret

e G

rid E

quat

ions

/

3D-F

IT –

Able

itung

der

dis

kret

en G

itter

glei

chun

gen

()

()

()

()

()

()

()

()

()

()

()

()

()

()

33

(,

)(

,)d

(,

)d

(,

)d(

,)d

()d

()d

()d

()d

uf

db

uf

db

yz

yz

CS

CC

CC

uf

db

yz

yz

CC

CC

yz

yz

tE

ty

Etz

Ety

Etz

Et

yE

tzE

tyE

tz

yz

=∂

=∆=∆

=∆=∆

=+

−−

=+

−−

+∆

+∆

∫∫

∫∫

∫∫

∫∫

ER

dRR

RR

Ri

○○

()

()

33

()

()

()

()

(,

)()

()

()()

u

fd

by

zy

zC

St

EtyE

tz

EtyE

tz

yz

=∂

=

∆+

∆−

∆−

∆+

∆+

ER

dRi○

()d yE

()b zE

()m xB

()f zE

()u yE

1xx

=3

zx

=

2yx

=in

tegr

atio

n ce

ll /

-

Inte

grat

ions

zelle

()m xBI

()m xBI

y∆

z∆

()u

C

()f

C(

)dC

()b

C

Page 28: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

28

3-D

FIT

–D

eriv

atio

n of

the

Dis

cret

e G

rid E

quat

ions

/

3D-F

IT –

Able

itung

der

dis

kret

en G

itter

glei

chun

gen

md

(,

)(

,)

(,

)d

SC

SS

tt

tt

=∂=−

−∫∫

∫∫∫

BR

dSER

dRJ

RdS

ii

i

()

()

()

()

mm

m

33

()

m

33

()

m

(,

)(

,)d

(,

)d

()d

()xS

S

xS m x

S yz

m x

tdS

tS

JtS

Jt

Sy

zyz

Jtyz

yz

yz

=∆∆

= =

=+Ο

∆∆

+∆

=∆∆

∆∆

+∆

∫∫∫∫ ∫∫

∫∫

nJ

ReJ

R

R

ii

()

()

()

()

()

()

md

()()

()()

()()

dm

uf

db

mx

yz

yz

xB

tyz

EtyE

tzE

tyE

tz

Jtyz

t

∆∆

=−

∆+

∆−

∆−

∆−

∆∆

inte

grat

ion

cell

/

-In

tegr

atio

nsze

lle(

)m xBI

()m xBI

()

()

()

()

()

()

33

(,

)()

()()

()

uf

db

yz

yz

CS

tE

tyE

tzE

tyE

tz

yz

=∂=

∆+

∆−

∆−

+∆

+∆

∫ER

dRi

○○

inte

grat

ion

cell

/

-In

tegr

atio

nsze

lle(

)m xBI

()m xBI

inte

grat

ion

cell

/

-In

tegr

atio

nsze

lle(

)m xBI

()m xBI

Page 29: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

29

3-D

FIT

–D

eriv

atio

n of

the

Dis

cret

e G

rid E

quat

ions

/

3D-F

IT –

Able

itung

der

dis

kret

en G

itter

glei

chun

gen

()r zE

()d xE

()r zE

()m yB

()l zE

()u xE

1xx

= 3zx

=2

yx

=

1xx

=

3zx

=2

yx

=

inte

grat

ion

cell

/

-In

tegr

atio

nsze

lle(

)m yBI

()m yBI

x∆

z∆

()m yB

()l zE

()d xE

()u xE

()

()

()

()

()

()

m

d()

d

()()

()()

()

m y

ul

dr

xz

xz

m y

Btyz

t

EtxE

tzE

txE

tz

Jtyz

∆∆

=−−

∆+

∆+

∆−

−∆∆

md

(,

)(

,)

(,

)d

SC

SS

tt

tt

=∂=−

−∫∫

∫∫∫

BR

dSER

dRJ

RdS

ii

i

inte

grat

ion

cell

/

-In

tegr

atio

nsze

lle(

)m yBI

()m yBI

Page 30: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

30

3-D

FIT

–D

eriv

atio

n of

the

Dis

cret

e G

rid E

quat

ions

/

3D-F

IT –

Able

itung

der

dis

kret

en G

itter

glei

chun

gen

1xx

= 3zx

=2

yx

=

1xx

=

3zx

=2

yx

=

inte

grat

ion

cell

/

-In

tegr

atio

nsze

lle(

)m zBI

()m zBI

y∆

()f xE(

)m zB

()b xE

()r yE

()l yE

()f xE

()m zB

()b xE

()r yE

()l yE

x∆

()

()

()

()

()

()

m

d()

d

()()

()()

()

m z

br

fl

xy

xy

m z

Btxy

t

EtxE

tyE

txE

ty

Jtxy

∆∆

=−

∆+

∆−

∆−

−∆∆

md

(,

)(

,)

(,

)d

SC

SS

tt

tt

=∂=−

−∫∫

∫∫∫

BR

dSER

dRJ

RdS

ii

i

inte

grat

ion

cell

/

-In

tegr

atio

nsze

lle(

)m zBI

()m zBI

Page 31: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

31

3-D

FIT

–D

eriv

atio

n of

the

Dis

cret

e G

rid E

quat

ions

/

3D-F

IT –

Able

itung

der

dis

kret

en G

itter

glei

chun

gen

md

(,

)(

,)

(,

)d

SC

SS

tt

tt

=∂=−

−∫∫

∫∫∫

BR

dSER

dRJ

RdS

ii

i

()

()

()

()

()

()

m

()

()

()

()

()

()

m

()

()

()

(

d()

()()

()()

()d d

()()

()()

()()

d d()

()()

d

mu

fd

bm

xy

zy

zx

mu

ld

rm

yx

zx

zy

mu

fd

zy

zy

Btyz

EtyE

tzE

tyE

tz

Jtyz

t Btyz

EtxE

tzE

txE

tz

Jtyz

t Btyz

EtyE

tzE

t

∆∆

=−

∆+

∆−

∆−

∆−

∆∆

∆∆

=−−

∆+

∆+

∆−

∆−

∆∆

∆∆

=−

∆+

∆−

)(

)(

)m

()()

()b

mz

ztyE

tz

Jtyz

∆+

∆−

∆∆

Page 32: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

32

Dua

l-O

rtho

gona

l Grid

Sys

tem

in S

pace

/D

ual-

orth

ogon

ales

Gitt

ersy

stem

im R

aum

1xx

= 3zx

=2

yx

=

3-D

/

3D

()

()n n

gG

mM

∈ ∈ ()n

gG

G

G⊥

Prim

ary

grid

/Se

cond

ary

(dua

l) gr

idPr

imär

es G

itter

Seku

ndär

es (d

uale

s) G

itter

Gnn

=

Gn

()n xE

()n yE

()n zB

()n yB

()y

nM

zE−

() z

nM

yE−

() z

nM

xE−

() x

nM

zE−

() x

nM

yE−

()y

nM

xE−

()

()

()

11

11

1,2,

,

1

xx

yy

zz

xyz

x yx

zx

y

nM

nM

nM

n

nN

NNN

M MN

MNN

=+

−+

−+

==

= = =

GM

=Pr

imar

y gr

id /

Mat

eria

l grid

Prim

äres

Gitt

erM

ater

ialg

itter

Glo

bal n

ode

num

berin

g /

Glo

bale

Gitt

ernu

mm

erie

rung

()n zE

()n xB

Page 33: Numerical Methods of Electromagnetic Field Theory I (NFT I ... · Numerical Methods of Electromagnetic Field Theory I (NFT I) Numerische Methoden der Elektromagnetischen Feldtheorie

33

End

of L

ectu

re 8

/En

de d

er 8

. Vor

lesu

ng