U.S. patent number 3,587,009 [Application Number 04/787,479] was granted by the patent office on 1971-06-22 for electromagnetic filters wherein waveguide walls comprise alternate conductivity sections.
This patent grant is currently assigned to Bell Telephone Labratories, Incorporated. Invention is credited to Lynden U. Kibler.
United States Patent |
3,587,009 |
Kibler |
June 22, 1971 |
ELECTROMAGNETIC FILTERS WHEREIN WAVEGUIDE WALLS COMPRISE ALTERNATE
CONDUCTIVITY SECTIONS
Abstract
A high pass filter comprising a section of waveguide having
alternate sections of different wall conductivity to produce a
sharper cutoff and more linear phase propagation near cutoff.
Low-pass, band-pass and band-reject filters are also described.
Inventors: |
Kibler; Lynden U. (Middletown,
NJ) |
Assignee: |
Bell Telephone Labratories,
Incorporated (Murray Hill, NJ)
|
Family
ID: |
25141614 |
Appl.
No.: |
04/787,479 |
Filed: |
December 27, 1968 |
Current U.S.
Class: |
333/210; 333/248;
333/208; 333/251 |
Current CPC
Class: |
H01P
1/207 (20130101); H01P 3/127 (20130101) |
Current International
Class: |
H01P
1/207 (20060101); H01P 3/127 (20060101); H01P
3/00 (20060101); H01P 1/20 (20060101); H01p
001/20 () |
Field of
Search: |
;333/7S,73W,95,98 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
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|
|
|
|
|
|
1,036,341 |
|
Aug 1958 |
|
DT |
|
1,130,487 |
|
May 1962 |
|
DT |
|
Primary Examiner: Saalbach; Herman Karl
Assistant Examiner: Gensler; Paul L.
Claims
What I claim is:
1. An electromagnetic wave filter comprising a waveguide of
essentially uniform diameter having conductively bounded walls,
said walls comprising alternate sections of conductive material
having different conductivities, the ratio of the conductivities
being between two and fifteen.
2. A device according to claim 1 wherein there are between 10 and
50 sections of each conductivity.
3. A device according to claim 2 wherein said waveguide has a
cutoff frequency and the length of two of said alternate sections
lies between 0.25 and 5 wavelengths at the cutoff frequency.
4. A device according to claim 3 wherein the length of a section of
the lower conductivity is greater than that of a section of the
higher conductivity.
5. An electromagnetic filter comprising a filter in accordance with
claim 1 and means for selectively extracting the transmitted and
the reflected portions of an input signal.
6. An electromagnetic wave low-pass filter comprising a three-port
circulator including an input, a filter according to claim 1
terminating the second port and an output port.
7. A band-pass filter including a pair of filters according to
claim 1 having different frequency characteristics.
8. A band-reject filter including a pair of filters according to
claim 1 having different frequency characteristics.
Description
This invention relates to improved electromagnetic wave
filters.
BACKGROUND OF THE INVENTION
Electromagnetic wave filters are used in a wide variety of
communications systems. For example, in radio systems using several
different transmit and receive frequencies, filters are typically
required to separate the transmit and receive frequencies.
A typical prior art high pass filter for microwave frequency
operation is simply a section of uniform waveguide having a cutoff
frequency at the desired minimum pass frequency. When a signal is
applied to the section, those portions of the signal having
frequencies above cutoff pass through the section essentially
unattenuated while those portions having frequencies below cutoff
are reflected back. One difficulty with such filters, however, is
the nonlinearity of the phase and attenuation propagation constants
for frequencies near the waveguide cutoff frequency. Because of
this nonlinearity, a significant bandwidth, on the order of 150
megahertz for a 3 gigaHertz cutoff filter, is lost for
communications purposes.
BRIEF SUMMARY OF THE INVENTION
The present invention arises from the discovery that a section of
waveguide having alternate sections of different wall conductivity
has more abrupt cutoff characteristics than a uniform section. Thus
a high pass filter comprising a section of waveguide having
periodic variations in wall conductivity produces considerably less
distortion of the propagation constants of signal frequencies near
cutoff with a negligible increase in the loss. In addition,
improved band-pass and band-reject filters can also be
constructed.
BRIEF DESCRIPTION OF THE DRAWINGS
These and other features, the nature of the present invention and
its various advantages will appear more fully upon consideration of
the specific illustrative embodiments shown in the accompanying
drawings and described in detail in the accompanying detailed
description. In the drawings:
FIG. 1 shows an illustrative embodiment of a high pass filter in
accordance with the invention;
FIG. 2 is a graphical illustration useful in understanding the
invention;
FIG. 3 shows an illustrative embodiment of a low-pass filter in
accordance with the invention;
FIG. 4 shows an improved band-pass filter in accordance with the
invention; and
FIG. 5 shows an improved band-reject filter in accordance with the
invention.
DETAILED DESCRIPTION
FIG. 1 is a schematic illustration of a high pass electromagnetic
wave filter in accordance with the invention comprising a periodic
structure of waveguide 10 having a cutoff frequency F.sub.c and
composed of sections 11 having a first wall conductivity C.sub.1 ,
and length L.sub.1 , alternated with sections 12 having a second
and smaller wall conductivity C.sub.2 and a length L.sub.2 .
Experimentally, it has been found that there should typically be
between 10 and 50 sections of each conductivity to establish
periodicity without incurring excessive loss.
The values of the parameters L.sub.1 , L.sub. 2, C.sub.1 , and
C.sub.2 are also chosen to establish periodicity with respect to
waves of frequency near F.sub.c without producing excessive loss.
For example, the total length of two sections, i.e., L.sub.1
+L.sub.2 , should be appropriate to establish periodicity with
respect to wave energy of frequency F.sub.c . If the length is much
smaller than a wavelength, the structure will behave much like a
uniform guide while, on the other hand, if the length is much
greater than a wavelength, it will behave as a plurality of
serially connected uniform guides. Experimentally it has been found
that the length of two alternate sections advantageously lies
between 0.25 and 5 wavelengths at the cutoff frequency. In
addition, it has been generally found that a sharper cutoff is
produced when the length L.sub.2 of the lower conductivity region
is slightly larger than that of the higher conductivity section.
Experimentally a length ratio of 5:3 has been found to be
particularly advantageous. The ratio between the two conductivities
C.sub.1 and C.sub.2 typically exceeds 2:1 in order to have any
measurable effect on the performance of the filter and is
advantageously less than 15:1 in order to avoid excessive
losses.
The following example further illustrates more specifically a high
pass filter in accordance with the invention. The filter comprises
a length of circular waveguides having an inside wall which has a
3.9 cm. radius and which is composed of alternate sections of
silver and stainless steel. The silver can be coated onto a less
expensive metal waveguide. The stainless steel sections are 5 cm.
long and the silver sections are 3 cm. long. The entire filter
comprises 20 sections of each type.
The graphical illustration of FIG. 2 compares the transmission
propagation characteristic of this filter with those of a uniform
silver waveguide having the same cutoff frequency, F.sub.c , at
about 2.95 gigahertz. Curve 1 shows the phase propagation constant,
B, measured in radians per meter, of the transmitted wave as a
function of frequency for the above-described periodic filter.
Curve 2 shows the same characteristic for a uniform waveguide. It
will be noted that in the region between 3.04 and 3.1 gigaHertz,
the characteristic of the periodic filter is more nearly linear
than that of the uniform filter, and that the periodic filter has a
much sharper cutoff at 3.03 gigaHertz
Curve 3 shows the attenuation propagation constant, .alpha.,
measured in nepers per meter for the periodic filter; and curve 4
shows .alpha. for the uniform waveguide. It will be noted that
.alpha. for the periodic filter is more linear than that for the
uniform waveguide and is only slightly greater.
In addition to having more linear characteristics for the
transmitted wave, the periodic filter also has more linear
characteristics for the reflected wave as can be inferred from FIG.
2 by examining the curves below cutoff frequency. Thus the
structure can also be used as a low-pass filter by selectively
extracting the reflected signal as is illustrated in FIG. 3. In the
figure there is shown a low-pass filter comprising a three-port
circulator 31 with a terminated high pass filter 32 at one of the
ports. In particular, a signal enters the device at the input port
1, passes to port 2 where it enters a periodic high pass filter 32
as described above. The frequencies above cutoff pass through the
filter to termination 33 while the frequencies below cutoff are
reflected back and leave through the output 34 at port 3.
As is well known, band-pass and band-reject filters can be made
from high pass and low-pass filters by selectively combining the
outputs of a pair of filters having different cutoff
frequencies.
FIG. 4 illustrates an improved band-pass filter in accordance with
the invention comprising a high pass filter as described in
connection with FIG. 1 in series with a low-pass filter as
described in connection with FIG. 3. The low-pass filter is
designed to pass only frequencies below a certain frequency,
F.sub.1 , and the high pass filter is designed to pass only
frequencies above a certain frequency, F.sub.2 . If F.sub.1 is
larger than F.sub.2 , only frequencies in the band between F.sub.2
and F.sub.1 will pass to the output 45.
FIG. 5 illustrates an improved band-reject filter according to the
invention. The device comprises a pair of circulators 51 and 53, a
pair of periodic filters 52 and 54, a termination 56 and a
directional coupler 55. A signal enters the input 50 at port 1 of
circulator 51, passes through port 2 to filter 52. The portion
above the cutoff frequency F.sub.1 passes through the filter to
port 1 of the second circulator 53 where it passes to port 2 to a
second filter 54. Frequencies above the cutoff frequency, F.sub.2 ,
of the second filter pass through to directional coupler 55.
Frequencies below cutoff are reflected and dissipated at
termination 56. Referring back to circulator 51, those frequencies
reflected by filter 52 pass to port 3 and then enter the
directional coupler 55. Thus at the output of the directional
coupler are all frequencies below F.sub.1 and above F.sub.2 .
In all cases, the above-described arrangements are merely
illustrative of a small number of the many possible specific
embodiments which can represent applications of the principles of
the invention. For example, while a specific example using circular
waveguide has been described, rectangular waveguide can also be
used, and while silver and stainless steel were given as examples
of metals having the required conductivity ratios, many other pairs
of metals, such as, for example, brass and silver or brass and
copper, can also be used. Thus numerous and varied other
arrangements can be readily devised in accordance with these
principles by those skilled in the art without departing from the
spirit and scope of the invention.
* * * * *