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| United States Patent | 4106026 |
| Link to this page | http://www.wikipatents.com/4106026.html |
| Inventor(s) | Bui-Hai; Nhu (Paris, FR);
Bourgeois; Alain (Paris, FR) |
| Abstract | A corrugated horn of the exponential type is provided with corrugations
whose depth decreases exponentially from the throat of the horn towards
its mouth. Such corrugations have the effect of reducing the stationary
wave ratio. |
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Title Information  |
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Drawing from US Patent 4106026 |
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Corrugated horn with a low standing wave ratio |
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| Publication Date |
August 8, 1978 |
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| Filing Date |
November 1, 1976 |
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| Priority Data |
Nov 04, 1975[FR]75 33698 |
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Title Information  |
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Claims  |
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What is claimed is:
1. A corrugated horn of the exponential type, wherein the depth of the
corrugations decreases exponentially from the throat of the horn towards
its mouth, the extreme depth values of said corrugations are respectively
.lambda./2 and .lambda./4, .lambda. being a wavelength corresponding to a
mean frequency of the operational frequency band, and the width of the
corrugations varies exponentially from the throat of the horn towards its
mouth.
2. A corrugated horn of the exponential type, wherein the depth of the
corrugations decreases exponentially from the throat of the horn towards
its mouth, the extreme depth values of said corrugations are respectively
.lambda./2 and .lambda./4, .lambda. being a wavelength corresponding to a
mean frequency of the operational frequency band, and the distance between
two consecutive corrugations varies exponentially from the throat of the
horn towards its mouth. |
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Claims  |
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Description  |
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This invention relates to corrugated horns with symmetry of revolution, of
the type used in the hyperfrequency field as antennae or as primary
sources of antennae.
The radiation diagrams of such horns have a symmetry of revolution.
Known horns of this type are conical horns. The depth of the corrugations
is constant, generally equal to about .lambda./4 (.lambda., operational
wavelength of the horn), the width of the corrugation is about .lambda./10
and the length of the smooth part (i.e. the part without corrugations) is,
in order to facilitate the matching of the horn, about one .lambda..
The corrugations improve the symmetry of the radiation diagram and reduce
the secondary lobes. However those known horns have a comparatively high
stationary wave ratio.
The object of the present invention is to overcome this drawback while
preserving the symmetry of revolution of the radiation diagram and a low
level of the secondary lobes.
This object is achieved in particular by the use of horns of the
exponential type, i.e. horns the cross-sectional area of which increases
exponentially with axial distance.
According to the invention, their is provided a corrugated horn of the
exponential type, wherein the depth of the corrugations decreases
exponentially from the throat of the horn towards its mouth.
The invention will be better understood and other features thereof will
become apparent from the following description in conjunction with the
accompanying drawings, wherein:
FIG. 1 is a section through a horn according to the invention.
FIG. 2 is a diagram relating to the horn shown in FIG. 1.
FIGS. 3 and 4 are sections through other horns according to the invention.
FIG. 1 is a longitudinal section through a corrugated horn, 1, of the
exponential type, which has symmetry of revolution and, hence, a circular
cross-section. From its throat 10 towards its mouth 11, this horn
comprises:
A connection flange 12,
A smooth part 13,
A part 14, with 14 transverse corrugations.
This horn, which has been designed to operate in the band from 6.43 to 7.11
GHz, has a length of 140 mm, an aperture diameter of 100 mm and a diameter
of 34 mm at the narrowest point of its throat.
The smooth part 13 of this horn has a length of approximately 40 mm which
substantially corresponds to the mean operational wavegength .lambda. of
the horn.
The corrugations of the part 14 all have a width of 5 mm and the thickness
of the wall between two consecutive corrugations is 2 mm. The depth of
these corrugations decreases exponentially from the throat of the horn
towards its mouth. The corrugation closest to the throat of the horn has a
depth of 23 mm, i.e. approximately .lambda./2, whilst the corrugation
closest to the mouth of the horn has a depth of 11.5 mm, i.e.
approximately .lambda./4.
By comparison with conical corrugated horns, the stationary wave ratio is
greatly reduced without the symmetry of revolution of the principal lobe
being affected, whilst the level of the secondary lobes is kept below -40
dB relative to the maximum level of the principal lobe.
FIG. 2 shows how the stationary weve ratio R of the horn shown in FIG. 1
varies in dependence upon the operational frequency F expressed in
gigahertz. Thus, for a band of 10% centred on 6.75 GHz, the stationary
wave ratio is below 1.06.
By way of indication, the aperture angle of the antenna shown in FIG. 1 is:
at -3dB, 36.degree. in the planes E and H,
at -10dB, 63.degree. in the planes E and H,
and at -20dB, 88.degree. in the plane E and 91.degree. in the plane H.
FIGS. 3 and 4 are longitudinal sections through two other corrugated horns
of the exponential type, with symmetry of revolution; these horns have an
overall length of 200 mm and are intended to operate in the band from 6.43
to 7.11 GHz.
The horn 2 shown in FIG. 3 comprises a smooth part 21 and a part 20 with
twelve transverse corrugations. As in the case of the horn shown in FIG.
1, the depth of these corrugations decreases exponentially from .lambda./2
to .lambda./4 (where .lambda. is a length corresponding to the mean
operational frequency of the horn) from the smooth part 21 towards the
mouth 22 of the horn, and the thickness of the walls between consecutive
corrugations is constant, i.e. is the same irrespective of the
corrugations in question. On the other hand, in the horn 2, in contrast to
the horn shown in FIG. 1, the width of the corrugations is not the same
from one corrugation to the following corrugation. It increases
exponentially from the smooth section 21 towards the mouth 22. This
exponential variation of the width of the corrugations, in conjunction
with the exponential variation of their depth, contributes towards
providing this horn with a very low stationary wave ratio.
The horn 3 shown in FIG. 4 comprises a smooth part 31 and a part 30 with
eleven transverse corrugations. As in the case of the horn shown in FIG.
1, the depth of these corrugations decreases exponentially from .lambda./2
to .lambda./4 from the smooth part 31 towards the mouth 32 of the horn,
and all the corrugations have the same width. On the other hand, in the
horn 3, in contrast to the horn shown in FIG. 1, the thickness of the
walls separating two consecutive corrugations is not constant: it
increases exponentially from the smooth part 31 towards the mouth 32. This
exponential variation of the thickness of the walls between the
corrugations, in conjunction with the exponential variation of the depth
of these corrugations, also contributes towards providing the horn with a
low stationary wave ratio.
Naturally the invention is by no means limited to the examples described
above. Thus, the width of the corrugations may also decrease exponentially
from the smooth section of the horn towards its mouth, as may the
thickness of the walls between the corrugations. In addition, the
variations in the thickness of corrugations and in the width of the walls
between the corrugations may be combined in one and the same horn.
Of course, the invention is not limited to the embodiments described and
shown which were given solely by way of example.
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Description  |
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