Filter of the type consisting of a primary waveguide having lateral secondary guides

Filter comprising a rectangular waveguide extended at both ends by rectangular guide-to-rectangular guide couplers and provided with lateral secondary guides. In order to enable the use of cylindrical secondary guides without introducing unwanted resonances, said couplers are given, at their ends, rectangular internal cross sections both the height and width whereof are smaller at the end coupled to the primary guide than at the end remote from the primary guide.

FIELD OF THE INVENTION 
This invention relates to a filter comprising a primary waveguide, the two 
ends whereof are coupled to the two filter openings, and at least one 
lateral, secondary guide one of the ends whereof issues into a hole 
drilled in the wall of the primary guide and the other end whereof is 
generally terminated by an absorbing material. 
BACKGROUND OF THE INVENTION 
Such filters are known and are, for example, connected in the output 
switching circuits of power amplifiers operating on centimeter waves in 
order to reduce the rate of harmonic radiation in space. 
The known filters consist of a rectangular primary waveguide the four sides 
or at least one of the two broad sides whereof are attached to lateral 
guides which are also rectangular but have a smaller cross section than 
the primary guide. The two openings of these filters are sometimes 
provided with a taper or a stepped impedance matching means; such 
impedance matching means, which forms a rectangular guide-to-rectangular 
guide coupler, is intended to boost the coupling of the lateral guides by 
reducing the distance between the two broad sides of the main guide, which 
is to say, by providing an internal cross section for the main guide the 
small sides whereof are smaller than those of the filter openings (inlets 
and outlets); the broad sides on the other hand are given the same 
dimensions as the broad sides of the outside rectangular guides to which 
the filter is coupled. 
These prior art filters are costly due to the large number of lateral 
guides which must generally be associated with the primary guide. 
Moreover, they are very difficult to manufacture using electroerosion or 
electroforming techniques. 
It is the object of this invention to obviate, or at least abate these 
disadvantages. 
SUMMARY OF THE INVENTION 
This object is attained, in particular, by using cylindrical secondary 
guides, said cylindrical guides being easier to make and easier to fit to 
the primary guide than are rectangular secondary guides. Significantly, 
although the substitution of cylindrical secondary guides for the 
rectangular secondary guides seems an obvious solution, it in fact raises 
problems which, it appears, had not been seriously analyzed and, above 
all, solved hereto. This explains why only rectangular-lateral-guide 
filters have been made so far. The description of the invention given 
hereinafter will point out the precautions which must be taken to ensure 
correct operation of filters with cylindrical secondary guides. 
The invention provides a filter comprising a rectangular primary guide, n 
secondary guides--where n is a whole number at least equal to 1--coupled 
by one of their ends to the primary guide via holes or apertures through 
the wall of said primary guide, and two impedance matching means of the 
rectangular guide-to-rectangular guide coupling type, respectively coupled 
to the two ends of the primary guide, wherein said n secondary guides are 
cylindrical guides and the ends of said impedance transformers have 
rectangular internal cross sections the width and height whereof are both 
smaller on the primary guide coupling side than on the side opposite the 
primary guide. 
The invention will be more readily understood and further features will 
become apparent from the following description, taken with reference to 
the accompanying drawings.

DESCRIPTION OF THE PREFERRED EMBODIMENT 
FIG. 1 shows a partial side view of a filter according to the invention, 
with a part thereof shown broken away. 
FIG. 2, which shows an end view of the same filter, includes an axial line, 
XX, locating the broken away section of FIG. 1; besides this breakaway, 
the transition from FIG. 2 to FIG. 1 involves removing part H of FIG. 2. 
As can be seen from the first two figures, the filter comprises the 
following parts: 
a mounting flange 3; 
an impedance matching coupler 2 which, together with the flange 3, is 30 mm 
long and which tapers from an internal cross section of 15.8.times.7.9 mm 
at the flange end to 14.times.7 mm at the other end; 
a rectangular primary guide 1, 270 mm-long, with an internal cross section 
of 14.times.7 mm; said primary guide is surrounded by forty lateral 
assemblies each comprising six cylindrical secondary guides, such as A1, 
B1, C1, D1, E1, F1, arranged in the same cross-sectional plane of primary 
guide 1; 
an impedance matcher 4, arranged symmetrically to impedance matcher 2 about 
a plane of symmetry formed by the plane, not shown, crossing through the 
center of guide 1; 
and a mounting flange 5, symmetrical to flange 3 with respect to the 
above-mentioned plane of symmetry. 
It should be noted that in the embodiment described, the entire filter, and 
not just flanges 3 and 5 and impedance transformers 2 and 4, is 
symmetrical with respect to said plane of symmetry, thus making the filter 
fully reversible. 
Each of the 40 previously-mentioned assemblies comprises: 
six cylindrical secondary guides such as A1 through F1, distributed along a 
same transverse plane of main guide 1, two of which, such as A1, B1 in 
FIG. 2, issue into one of the broad sides of said primary guide 1, two 
more of which, such as D1, E1, issue into the other broad side of guide 1, 
and the remaining two of which, such as C1, F1, issue respectively into 
the two small sides of guide 1, all of the secondary guides in said forty 
assemblies having an internal diameter of 5.38 mm and a length of 30 mm, 
said secondary guides forming, in the lengthwise direction of guide 1, six 
alignments of forty parallel and contiguous guides, such as B1-B40 and 
D1-D40 in FIG. 1; 
covers closing off the ends of said secondary guides opposite the primary 
guide, said end covers being associated to form four large covers G, H, I 
and J respectively covering all the secondary guides such as A1, B1, C1, 
D1, E1 and F1; 
and terminations such as Lb1,Lb9, Lb40(FIG. 1) consisting a 2 mm-thick 
absorbing materials inserted into the ends of all of the secondary guides 
opposite the primary guide, the fillers of all forty secondary guides in a 
given row being connected together through slots such as K provided in the 
outside ends of the secondary guides in contiguous portions thereof, said 
terminations so forming six saw blades, such as L, the forty teeth whereof 
thus constitute forty secondary guide fillers. 
The filter's secondary guides issue into guide 1 via circular apertures 
with a diameter of 5.38 mm, equal to the internal diameter of the guides, 
except for the first five and last five guides in each row, the coupling 
apertures whereto are given a smaller diameter to avoid capturing too 
large a fraction of the energy of primary guide 1. The diameters of the 
first four apertures from the ends of the rows are 4.16, 4.40, 4.67 and 
4.95 mm, respectively. Thus, the secondary waveguide couplings increase 
gradually after the first from the filter openings--a feature which 
reduces the power applied to the first fillers and prevents their 
destruction by a high input power. Since this gradual augmentation of the 
secondary waveguide couplings occurs at both ends of the filter, both ends 
can serve as inlets, there being no reason to favor one end over the other 
for purposes of power dissipation in the first fillers. The thirty 
remaining secondary guides of each row all being identical and issuing by 
identical apertures into guide 1, the middle portion of the filter in FIG. 
1 has been left out of the drawing to allow the parts shown to be drawn to 
a large enough scale to enable a clear rendering of their details. 
FIG. 3, the cross section of the same filter as in FIGS. 1 and 2, taken at 
the eighth lateral assembly counting from the left end of FIG. 1, shows 
the six secondary guides A8, B8, C8, D8, E8, F8 with their respective 
fillers La8, Lb8, Lc8, Ld8, Le8, Lf8 and covers G, H, I, J. The fillers 
are secured in the covers by glueing. 
The filter just described is a 2nd harmonic filter designed to pass a 
fundamental frequency in the 17.3 to 18.1 GHz range. It performed as 
follows with a test input power of 1.3 kW: losses affecting the 
fundamental were 0.11 dB and the standing-wave ratio was 1.035; for a 2nd 
harmonic in the range 34.6-36.2 GHz, losses were above 50 dB and the 
standing-wave ratio was 1.23. 
The manufacture of this filter raised a number of problems. In fact, it was 
attempted to start from a conventional filter with rectangular secondary 
guides and merely replace the latter by cylindrical guides. However, there 
appeared, in addition to the TE11 mode, unwanted modes TE10 and TE20 (TE01 
and TE02 in the French language transcription). This occurrence can be 
explained by the fact that the rectangular secondary waveguides of the 
prior art were relatively "flat", making their internal cross section and 
consequently their coupling aperture small, this feature avoiding the 
creation of interferences in the primary guide. With cylindrical secondary 
guides on the other hand, the cross sections are large, since it is no 
longer possible to reduce width without reducing height, and large 
discontinuities (cutouts) are necessarily provided in the wall of the 
primary guide. Such discontinuities bring about an artificial widening of 
the primary guide and accordingly the cutoff frequency for the first two 
spurious modes TE10 and TE20 is lowered, causing unwanted resonances, 
particularly in the 17.3-18.1 GHz band. 
It might have been possible to cut back the size of the coupling apertures 
to each of the secondary guides to avoid such interferences. However, 
again because of the large cross sections of the cylindrical guides, it 
would not have been possible to align enough such cylindrical secondary 
guides to receive the same amount of energy per unit length of filter and 
the resulting filters would have to be roughly twice the length of 
rectangular secondary guide filters for the same performance. Such 
bulkiness is unacceptable for most applications. 
The solution for avoiding the stated disadvantages, as appears from the 
description made herein with reference to FIGS. 1 through 3, consists in 
reducing both the height and width of the primary guide, and, 
incidentally, gradually reducing the coupling of the secondary guides 
towards the filter openings. 
It will be understood that the present invention is not limited to the 
embodiment described and that certain changes might occur to those skilled 
in the art without departing from the scope and spirit of the invention. 
For example, the primary guide could be provided with lateral secondary 
guides only on its two broad sides or on one side alone. Also, the number 
of secondary guides, although it must be at least equal to 1, is limited 
only by the space available for the filter. The secondary guides could 
also be filled with a dielectric to reduce their cross section without 
raising their cutoff frequency, or they could be differently distributed 
along the primary guide, notably in an irregular pattern. As for the 
impedance matchers in the filter openings, such as 2 and 4, these could be 
either taper types or stepped types.