U.S. patent number 3,786,372 [Application Number 05/314,835] was granted by the patent office on 1974-01-15 for broadband high frequency balun.
This patent grant is currently assigned to GTE Sylvania Incorporated. Invention is credited to James J. Epis, Samuel Chung-shu Kuo.
United States Patent |
3,786,372 |
Epis , et al. |
January 15, 1974 |
BROADBAND HIGH FREQUENCY BALUN
Abstract
A broadband high frequency balun is connectable between balanced
and unbalanced transmission lines so that these lines are
essentially colinear. The balun comprises a coaxial cable and a
shorted stub in approximately a half-loop configuration, the
balanced line being connected to the cable and stub within a
conductive housing or shield. The cable-stub spacing is
substantially greater than the effective length of the stub,
thereby decreasing the lower frequency operating limit of the
balun. The addition of a lossy layer to the inner surface of the
housing permits a substantial increase in the operating bandwidth
of the balun by suppressing adverse resonance effects within the
housing.
Inventors: |
Epis; James J. (Sunnyvale,
CA), Kuo; Samuel Chung-shu (Cupertino, CA) |
Assignee: |
GTE Sylvania Incorporated
(Mountain View, CA)
|
Family
ID: |
23221655 |
Appl.
No.: |
05/314,835 |
Filed: |
December 13, 1972 |
Current U.S.
Class: |
333/26;
333/33 |
Current CPC
Class: |
H01P
5/10 (20130101) |
Current International
Class: |
H01P
5/10 (20060101); H03h 007/38 (); H03h 007/42 () |
Field of
Search: |
;333/25,26,32,33
;343/859,814,816,821 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
Other References
Fubini et al.-"A Wide-Band Transformer from an Unbalanced to a
Balanced Line" in Proceedings of the IRE-Waves and Electrons
Section October, 1947; pages 1,153-1,155. .
MacKenzie-"Some Recent Advances in Coaxial Components for Sweep
Frequency Instrumentation" in the Microwave Journal June 1969;
pages 73-74..
|
Primary Examiner: Rolinec; Rudolph V.
Assistant Examiner: Nussbaum; Marvin
Attorney, Agent or Firm: Lawler; John F.
Claims
What is claimed is:
1. A device for transforming an unbalanced transmission line to a
balanced transmission line comprising
an electrically conductive casing having a side wall and parallel
end walls connected to opposite ends of the side wall and defining
a cavity therewithin,
one of said end walls having an opening through which the balanced
line extends into the cavity transversely of and insulated from
said one end wall,
said unbalanced line comprising a coaxial cable projecting into the
cavity from the other end wall and having an outer conductor
connected at opposite ends to said other end wall and to one
conductor of said balanced transmission line, respectively, said
cable also having an inner conductor connected within the cavity to
the other conductor of said balanced line,
a conductive stub electrically connecting the other conductor of
said balanced line to said other end wall,
said stub and said cable having substantially equal outer diameters
and substantially equal lengths, and having first parallel
portions, respectively, projecting into the cavity from said other
end wall and being spaced apart by a distance substantially greater
than the length of each of said first portions.
2. The device according to claim 1 with a thin layer of lossy
material on the interior of said side wall.
3. A balun for interconnecting an unbalanced transmission line with
a balanced transmission line comprising
a cylindrical conductive housing having an axis and axially spaced
end walls,
one of said end walls having a central opening therein through
which said balanced line extends axially into and insulated from
said housing,
an L-shaped coaxial cable having a first leg extending into the
housing from the other end wall parallel to and offset from said
axis and having a second leg extending radially inwardly from the
first leg toward said balanced line,
said cable having an inner conductor and an outer conductor, said
outer conductor being electrically connected to said housing,
means for electrically connecting said unbalanced line on the
outside of said housing to said first leg of the cable whereby the
unbalanced and balanced lines extend substantially parallel to one
another,
an L-shaped conductive stub in said housing having a first leg
connected to said other end wall and extending parallel to and
offset from said axis, said stub also having a second leg connected
to and extending radially inwardly toward said balanced line
colinearly with the second leg of the coaxial cable,
said balanced line having first and second conductors connected to
the outer and inner conductors, respectively, of said cable, said
second conductor also being connected to said second leg of said
stub,
the spacing between the first legs of said cable and said stub
being substantially greater than the length of said first leg of
the stub.
4. The balun according to claim 3 in which said housing has a side
wall, and a resistive coating on the inner surface of said side
wall.
Description
BACKGROUND OF THE INVENTION
This invention relates to baluns and more particularly to an
improved balun capable of operating at high frequencies.
A balun is a device which effectually transforms a TEM-mode wave
propagating on a balanced two-conductor transmission line into
another TEM-mode wave propagating inside an unbalanced-type
transmission line, the latter typically being a coaxial line. The
TEM-mode transformation is reciprocal.
There are many applications for such a device. An important
application is the connection of a coaxial-line output or input of
a transmitter or a receiver to any type of antenna that can be
excited properly only by means of a balanced two-conductor
transmission line. In many instances it is desired if not required
that the balun interconnecting the two different types of
transmission lines be capable of operating effectively and
efficiently over broad frequency bands, often over very broad
bands. An everincreasing demand for very broadband conical and
cavity-backed spiral antennas for operation up to 30 to 40 GHz
exist at the present time. Utilization of a broadband balun
provides the most economical convenient means to achieve proper
excitation of these antennas. The provision of a satisfactory
reasonably efficient very broadband balun for these important newly
developing applications for spiral antennas is a principal
objective of this invention.
A prior art balun useful at high microwave frequencies is described
in an article entitled "A Wide-Band Balun" by McLaughlin et al. in
IRE Transaction on Microwave Theory and Techniques, July 1958, at
pages 314-316. The upper limit of useful frequency range for this
balun is about 18 GHz and furthermore the input and output lines to
this balun are spatially orthogonal. Accordingly, this balun cannot
be used over the full range of a spiral antenna, for example,
operating over a band of 1.3 to 40 HHz. Furthermore, colinear feed
arrangements cannot be accommodated by this balun.
OBJECTS AND SUMMARY OF INVENTION
An object of this invention is the provision of a balun having
insertion loss and input VSWR performances comparable to
state-of-the-art baluns but having extremely broadband widths,
i.e., 36:1.
A further object is to provide a balun of this type for use at
frequencies up to 40 GHz.
Another object is to provide a balun in which the unbalanced
coaxial input transmission line is colinear or nearly colinear with
the balanced line.
These and other objects of the invention are achieved with a balun
featuring a cable and shorted stub spaced apart by a distance
greater than the length of the stub and housed in a conductive
shield. The cable and stub are configured to form approximately a
half loop and the balanced line connected to the cable and stub
extends in a direction parallel to the cable. The bandwidth of the
balun is greatly increased with a slight increase in insertion loss
through suppression of resonances of the TEM-wave, TE-wave and
TM-wave modes within the cavity by disposition of a lossy material
in the housing.
DESCRIPTION OF THE DRAWINGS
FIG. 1 is a top plan view of a balun embodying the invention;
FIG. 2 is a section taken on line 2--2 of FIG. 1;
FIG. 3 is a greatly enlarged sectional view of the junction of the
balanced line with the coaxial line and shorted stub;
FIG. 4 is a view taken on line 4--4 of FIG. 3; and
FIG. 5 is a section taken on line 5--5 of FIG. 4.
DESCRIPTION OF PREFERRED EMBODIMENTS
Referring now to the drawings, a balun embodying the invention is
shown at 10 and comprises a cylindrical housing 11 having an axis
A, a side wall 12 and end walls 13 and 14 at opposite ends of the
side wall. The housing is preferably made of conductive material
such as copper or brass and defines a cavity 16 within which energy
from a balanced line 18 is transformed to an unbalanced line 19 (or
vice versa). A central opening 21 in end wall 13 permits the
balanced line to extend into the cavity without making electrical
contact with the housing. A standard connector 22 attached to end
wall 14 permits connection to the balun of the external unbalanced
line 19, shown as a coaxial line.
Extending into the housing from end wall 14 at connector 22 is an
inverted L-shaped coaxial cable 24 having a first leg 25 extending
parallel to housing axis A and a second leg 26 extending radially
inwardly from and substantially at right angles to leg 25 for
connection to balanced line 18. Cable 24 has an inner conductor 24a
and an outer conductor 24b, the latter being connected to end wall
14. On the diametrically opposite side of the cavity from cable 24
is a similarly inverted L-shaped conductive stub 28 having a first
leg 29 electrically connected to and extending inwardly from the
end wall 14 and a second leg 30 extending radially inwardly and
substantially at right angles to first leg 29. Cable 24 and stub 28
lie in a plane containing the axis A of the housing and are
symmetrically disposed about the axis in the shape of a half
rectangular loop as shown in FIG. 2.
Balanced line 18 comprises a pair of conductors 32 and 33 which, in
the embodiment shown, are formed or deposited as thin films on a
low loss dielectric strip 35. This balanced line extends from its
connection to cable 24 and stub 28 within housing 11 to utilization
apparatus, not shown, such as a spiral antenna.
The connection of the balanced line 18 to the cable and stub is
shown in FIG. 3. Cable outer conductor 24b at the inner end of
radial leg 26 is electrically connected to conductor 32 of balanced
line 18. Inner conductor 24a extends through an opening 37 in and
therefore is electrically insulated from conductor 32 and passes
through insulator strip 35 for electrical contact with conductor 33
and stub leg 30. In practice, stub 28 preferably is tubular in
shape and may then have an apertured plug 39 press-fitted into the
inner end of leg 30 for receiving the extension of the inner
conductor as shown. The plug, inner conductor, and stub leg 30 are
electrically connected to conductor 33 of the balanced line by
solder 40 or the like. Optimum operation of the balun is achieved
by forming the outer surfaces of coaxial cable 24 and stub 28 such
that those surfaces are virtually identical.
In prior art baluns of the general type described above, the
distance d between component parts corresponding to legs 25 and 29
of the cable and stub, respectively, generally determine the
highest usable frequency of the devices. More particularly, as the
distance d approaches 0.2 .lambda. where .lambda. is the operating
wavelength, currents on the exterior of legs 25 and 29 begin to
radiate.
Without the housing 11 functioning as an electromagnetic shield
around those legs, such radiation would render the balun of the
present invention useless for its intended purpose. More
specifically, the shielding effect of housing 11 prevents such
radiation, thereby extending the frequency range of the device. As
the operating frequency is increased, however, resonant cavity
effects of housing 11 come into play. With such increase in
frequency, the cavity in the housing becomes electrically large
enough in diameter to support waveguide-type modes. These
waveguide-type modes are TE- and TM-modes as distinguished from
TEM-modes. The currents on the legs of the stub and coaxial cable
within the cavity excite such modes. The effect of the
waveguide-type modes in the cavity is to cause insertion loss
spikes periodically across the operating band. In order to
eliminate these spikes, and thereby greatly increase the operating
bandwidth, a layer or cylinder 42 of dissipative or lossy material
is disposed adjacent to the side wall of the cavity, as shown in
FIGS. 1 and 2. This material suppresses these waveguide-type modes
and eliminates the insertion loss spikes caused by them while at
the same time producing an acceptably small increase in the average
insertion loss of the device across the band.
It should be noted that the balun described above without the lossy
material 42 and in which the distance d is greater than the height
h of the stub and cable provided satisfactory performance as a
balun over a 15:1 bandwidth, the insertion loss being less than 1.3
db. Thus, for applications having this or a smaller bandwidth
requirement, the lossy material may be omitted, with the advantage
of a decrease in insertion loss. Details are described below.
A shielded half-loop balun of the type described above without
lossy liner 42 was constructed and successfully operated and had
the following dimensions and operating characteristics:
Cavity Inner diameter 2.75 inches Length (axial) 1.25 inches Loop
Distance d 1.5 inches Height h 0.697 inches Diameter of cable/stub
0.085 inches Balanced line Thickness t (gap) 0.031 inches
Characteristic impedance 62 ohms Bandwidth 0.256 GHz to 3.84 GHz
(15.0:1) Maximum insertion loss 1.2 db
The addition to the above-described tested balun of a complete
cylinder 42 of 0.375 inch thick lossy maerial made of carbonized
foam by Emerson Cummings, Inc. and designated as AN-73, adjacent to
the cylindrical side wall 12 increased the useful bandwidth from
the 0.256 GHZ -3.84 GHz (15:1) range to 0.269 GHz to 9.71 GHz
(36:1) while maintaining the insertion loss less than 1.5 db across
that band. In addition to suppressing TE- and TM-mode resonances,
the lossy material also suppressed TEM-mode resonances which
occurred in the cavity as a consequence of the effective electrical
length of stub leg 29 approaching .lambda.2 and 1.0 .lambda..
The higher frequency versions of baluns which embody this invention
are achieved by scaling the dimensions of the balun components in
accordance with the frequency desired or required. Such scaling is
demonstrated in Table I for baluns without lossy cylinder 42,
beginning with the tested model described earlier.
TABLE I
Semi-Rigid Coaxial Line Frequency Band Comment UT 85 0.256 to 3.84
GHz Tested Model (15:1 Bandwidth) UT 70 0.311 to 4.663 GHz 70/85
Scale Model UT 47 0.462 to 6.945 GHz 47/85 Scale Model UT 35 0.622
to 9.326 GHz 35/85 Scale Model UT 20 1.088 to 16.32 GHz 20/85 Scale
Model
All of the coaxial cables referenced in the table and satisfactory
connectors for them are commercially available items. Dimensioning
of the balanced line is readily and accurately controlled by
photo-etching the lines on a dielectric strip of properly scaled
dimensions. Finally, the housing 11 is machined so that it is
readily constructed accurately to the precise scaled dimensions.
While Table I demonstrates how the preferred embodiment of the
invention without lossy cylinder 42 is scaled for use at higher
frequencies, it does not necessarily follow that directly scaled
models are optimum designs.
Table II illustrates the effect of scaling the dimensions of the
foregoing tested embodiment of the invention which included the
lossy layer 42 within the cavity to greatly expand the operating
bandwidth of the balun.
TABLE II
Semi-Rigid Coaxial Line Frequency Range Comment UT 85 0.269 to 9.71
GHz Tested Model (36:1 Bandwidth) UT 70 0.3266 to 11.79 GHz UT 47
0.4865 to 17.57 GHz UT 35 0.6533 to 23.58 GHz UT 20 1.143 to 41.26
GHz
The last version of the balun listed in this table has an upper
operating frequency limit in excess of 40 GHz.
* * * * *