IEEE MTT-V033-I02 (1985-02)


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~IEEE

TRAN SACTI 0 NS

ON

MICROWAVE THEORY AND TECHNIQUES FEBRUARY 1985

VOLUME MTT-33

NUMBER

2

(ISSN 0018-9480)

A PUBLICATION OF THE IEEE MICROWAVE THEORY AND TECHNIQUES SOCIETY

PAPERS

Power-Handling Capabilities of Circular Dielectric Waveguide at Millimeter Wavelengths ................ D. G. Jablonski 85-115-GHz Receivers for Radio Astronomy ............................ D. P. Woody, R. E. Miller, and M. J. Wengler Field Theory Design of Rectangular Waveguide Broad-Wall Metal-Insert Slot Couplers for Millimeter-Wave Applications .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . F. Arndt, B. Koch, H..-J. Orlok, and N. Schroder 12-GHz-Band GaAs Dual-Gate MESFET Monolithic Mixers ....................... T. Sugiura, K. Honjo, and T. Tsuji Variational Analysis of Ridged Waveguide Modes ..................................................... Y. Utsumi The Electric-Field Problem of an lnterdigital Transducer in a Multilayered Structure ................................ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . P. M. van den Berg, W. J. Ghijsen, and A. Venema Computer Calculation of Large-Signal GaAs FET Amplifier Characteristics ................ A. Materka and T. Kacprzak Short Millimeter Wavelength Mixer with Low Local Oscillator Power ....................................... W. Hant

85 90 95 105 111 121 129 135

SHORT PAPERS

Exact Wave Resistanc(f.of Coaxial Regular Polygonal Conductors ...................................... R. Terakado Analysis of the Transmission Characteristics of Inhomogeneous Grounded Finlines ............................ . A. Beyer Phase-Matched Waveguide Using the Artificial Anisotropic Structure and its Application to a Mode Converter ........... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . T. Mizumoto, H. Yamazaki, and Y. Naito A Design Method of Bandpass Filters Using Dielectric-Filled Coaxial Resonators .................................... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . M. Sagawa, M. Makimoto, and S. Yamashita Conservation Laws for Distributed Four-Ports .......................................... 0. Schwelb and R. Antepyan A Broad-Band Directional Coupler for Both Dielectric and Image Guides .................. R. J. Collier and G. Hjipieris An Iterative Moment Method for Analyzing the Electromagnetic Field Distribution inside Inhomogeneous Lossy Dielectric Objects .......................................................................... M. F. Sultan and R. Mittra On the Graceful Degradation Performance of Multiple-Device Oscillators .................. S. Sarkar and M. C. Agrawal

143 145 149 152 157 161 163 168

LETTERS

Comments on "EM Local Heating with HF Electric Fields" ........................... M. J. Hagmann and K-M. Chen Comments about "On the Definition of Parameters in Ferrite-Electromagnetic Wave Interactions" ..................... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . E. M. A. Eid and L. Lewin

171

N. R. Dietrich

174

PATENT ABSTRACTS ..................., .............•...........................................

172

. and u ill recel}-e this TR.\XS +c~Io\s upon pa} merrt of the annual Society membership fee of $8.00. Affdiate membership is avadable upon payment of the annu~l affdiate fee of S24 (N). ~1..j the Society fee of S8.00. For information on joining write to the IEEE at the address below.

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N. W’. COX J. E. DEGENFORD,

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V.G GELNOVATCH P. T. GREILING R. B. HICKS * E.Y offic[o (past pre ~ldents ) A. C BECK S. B COHN

w.

w“

S. L. MARCH 1). N. MCQUIDDY, JR.

C.T

R. S. KAGIWADA R. H. KiNERR Honorary Lij> Members

E. C. NIEHENKE J M. ROE

B. E SPIELWtAN

A

OLIh ER T S SAAD

TRANSACTIONS@

ON

Chapter

S ADA,M

MICROWAVE

ELECTRICAL

AND

fhed Lecturers P. T. GREILING S. WEINREB

Princeton: A, K. SHARMA San Diego: D T GAVIN Santa Clara Valley/San Francisco

L. A. STARK Schenectady: J, BORREGO Seattle: D G. DOW Southeastern Michig~n: D. P. NYQUMT St. Louis: C. E. LARSON Sweden: E. L, KOLLBERG Switzerland: F. E. GARDIOL Syracuse. J. C. RAU~ to Tokyo: T OKOSH1 Tucson: E, P. PIERCF. Twin Cities: C. R. SEASHORE Utah/Salt Lake City M F. ISKANDER Washington/Northern Virginia: M. ZISSORSON West Germany: N, J, KEEN

THEORY

,4ND

TECHNIQUES

Editors M. AKAIKE (Abstracts Editor—Asia]

F [VkNEK

OF

RUCKER*

Chairmen

Associate

INSTITUTE

ROSENBAUM*

R. A. SPARKS*

K TOM IYASU L Y’OLYG

B. BHAT

N R. DIETRICH (Patent Ab~iracrs)

THE

F,J

IJist{ngu!

A

Editor ITOH

KUNO

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Secretary-Treasurer

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STAi3CKER,

H.J

S-MTT

T

P, ~,

T. ITOH

MU MFORD

Albuquerque: J. P CASTILLO Atlanta: B. J. CowN Baltimore: J. A. FAULKNER, JR,

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TRANSACTIONS

ON

IEEE

TRANSACTIONS

ON MICROWAVE

THEORY

AND

TECHNIQUES,

85

MTT-33, NO. 2, FEBRUARY 1985

VOL.

Power-Handling Capabilities of Circular Dielectric Waveguide at Millimeter Wavelengths DANIEL

Abstract’-The

power-handling

gnide propagating illustrate guides

imposed

are presented

at 70 GHz.

circular

dielectric

orders

of a circular

dielectric

the single HE ~, mode are discussed. Simple

the limits

Examples

capabilities

G. JABLONSKI,

by dielectric

for polystyrene

The

results

waveguide

heating that

and dielectric

maximum

in the millimeter-wave

of 10 to 100 W and that dielectric

(PTFE) levels

for

will be of the

is the fimiting

phenome-

non.

1.

T

HERE

HAS

magnetic

considerable

properties

ever, there has been little, handling

capabilities

study of the electro-

of a dielectric

waveguide.

if any, mention

How-

of the power-

of such a guide. This is not surprising,

as dielectric waveguide is primarily of interest at millimeter wavelengths, where levels of available power are rather low. Given the current amount of activity aimed at developing high-power millimeter wavelength sources, though, it seems useful to perform at least a simple study of the power

limitations

There in

this

of a typical

are three physical regard.

The

known

in conjunction

voltage

insulators.

results from principle, Raman

power

dielectric

first,

is well

the use of dielectrics

as high-

The second is dielectric

cause the waveguide and

Brillouin

heating,

which

in the dielectric

and can, in

to melt. Finally,

stimulated

scattering

are of great

concern

to

designers of optical-fiber systems. This is because the wavelength of a guided mode is sufficiently small for the optical signal

to interact

purities

in

importance

with

lattice

the dielectric. at millimeter

vibrations,

However,

defects,

scattering

wavelengths,

only because of the extremely

and im-

is of little

and is mentioned

close connection

between

the

circular dielectric waveguide and an optical fiber. Dielectric breakdown and dielectric heating are disussed in turn. Examples of dielectric breakdown and dielectric heating are given for various materials utilized as circular dielectric however,

waveguide at 70 GHz. The discussion begins, with a brief review of the properties of the HE1l

mode in a dielectric

The HE1l

mode has received much attention,

of polytetrafluoroethylene

surrounded

by air. Hence,

the free-space

and only a

usually

or polyst yrene be equal to c ~,

permittivity.

The field components are given by Stratton cylinder

(PTFE)

c1 will

of the allowed

[1]. Provided

is less than a critical

can propagate.

This critical

propagation

modes

that the radius

a of the

radius

ao, only a single mode

radius is shown by Cullen

[2] to

occur when (la)

Jo(x)=o where x = 27raO(61/eO)l’2(6r

breakdown,

attenuation

DIELECTRIC-ROD

–1)1’2/X0.

(lb)

that are of interest

dielectric

with

OF THE

few important points will be discussed here. A section of dielectric guide is sketched in Fig. 1. The guide consists of a cylinder of dielectric constant c ~ imbedded in a medium of dielectric constant cl. Typically, the guide consists of a

waveguide.

phenomena

PROPERTIES

WAVEGUIDE

cylinder

INTRODUCTION

BEEN

II.

IEEE

breakdown.

power

spectnrm

heating

wave-

MEMBER,

calculations

and prdytetrafluoroethylene

suggest

SENIOR

cylinder.

Manuscript received April 16, 1984; revised August 16, 1984. This work was supported by the Navaf Surface Weapons Center under an Independent Research Grant. The author is with the Navaf Surface Weapons Center, White Oak, Silver Spring, MD 20910.

U.S. Government

JO is the ordinary Bessel function of the first kind. The relative dielectric constant c,, is defined as c~/cl, and A ~ is the free-space

wavelength

As an example, 70 GHz,

A.=

4.3 mm.

x = 2.405. Hence, mm. The single brid

longitudinal

which

the HE1l

the radius

size is decreased,

wave.

first

zero

of

a. is found

propagates

when

as the HE1l

at

to be 1.58

a

surface

I

@el=@e2

a+e, = o 6%



where n = inn, the normal shown in Fig. 2.

on magnetic

wall

(3b)

vector on each surface or wall as

n(Y)=o,

=71(Y)>

for the trial

eigenfunction

on 12, lb, 1~, and 16

(5b)

on

13

(5C)

on

15.

The relation between q(y) and $(y) is described later for the TM modes. The integral (A)sl for the cross-sectional area S, and the contour integral (A)=, for the contour pass

UTSUMI

: VARIATIONAL

ANALYSIS

OF RIDGED

WAVEGUIDE

113

MODES

as

The left-hand

(A)~l=~s~.dx.dy

IV.

C, are defined

side of (9) is also stationary

for ~.,.

STATIONARY FORMULA FOR RIDGED WAVEGUIDE

(A).,

= ~b~aA.

dx.dy

Applying

(A)c, =~’Alx.o”dy +~lY.s. o +

OAIX=,. dy +

/

dx

/1‘A

=J~”d’+l:”d’:JA”d’+ 1

the TE constraint

conditions

on 12 and Id that

dOhl/ dn = O and the TE boundary condition on 11 that ;Yt;~~ we find the trial eigenfunction in region I (O< x <

~=o.dx

where

lA”d’ 4

3

m: integer (A)c2=

~b4x=, ”dy

f&=,”dy+

s

o

+ j=AIY=~.dx+~OAIX=..dy

+ ~’AIY=o”dx

=-i:”d’-l;”:-i: In

Appendix

minimize

”dl

I, we have

(4a) and (5a) with

proved

(6)

a

that

if

the constraint

Eigenfunction

Equation

Including

the TE constraint

= O, we

also

(t<

x l)=6n(n>l)

we should

function

$(y)

select the appropriate

which is proportional

for

=2. trial

cq. coskqy.

~ ‘$(Y)=

/

C~, &(y)

formulas

and

(A16)

into

(19)

of (21a) Ph = left-hand

side of (21a) (21b)

for

TM modes

is given by

(s’-y’)-(1’3),

Iyl

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