EP0245404A1

EP0245404A1 - Horn antenna

Info

Publication number: EP0245404A1
Application number: EP86906819A
Authority: EP
Inventors: Johann Mutschlechner
Original assignee: WOHLLEBEN Rudolf
Current assignee: WOHLLEBEN Rudolf
Priority date: 1985-11-18
Filing date: 1986-11-17
Publication date: 1987-11-19
Also published as: DE3540900C2; US4873534A; WO1987003143A1; DE3540900A1

Abstract

Une antenne en cornet pour l'excitation focalisée d'une antenne à réflexion dont la bride du cornet est dotée de nervures est conçue de manière à réaliser une élimination de réflecteurs profonds à performance superficielle élevée, une faible radiation excédentaire et une atténuation du lobe secondaire élevée. A cette fin, le demi-angle o de la bride de l'antenne (7) est réglé à 70o < o < 80o et le guide d'onde d'alimentation (3) est disposé de manière appropriée en saillie par rapport à la gorge du cornet (21).A horn antenna for focused excitation of a reflecting antenna having ribs in the horn flange is designed to achieve high surface performance deep reflector suppression, low excess radiation and sidelobe attenuation high. For this purpose, the half angle o of the antenna flange (7) is set to 70o < o < 80o and the feed waveguide (3) is suitably arranged projecting relative to the throat of the cornet (21).

Description

Horn blaster

The invention relates to a horn radiator for the focus excitation of a reflector antenna, with a horn flange arranged in the output-side end region of a tubular feed waveguide, which flanges out in a funnel shape from its horn throat located on the feed waveguide and has grooves aligned on its inside of the funnel parallel to the axis of the feed waveguide.

In such a known horn radiator (DE-OS 3 144 319), in which the feed waveguide is flush with the horn throat, the axially parallel alignment of the grooves coaxially surrounding the longitudinal axis of the feed waveguide strives for a structure which is as simple as possible as accurate as possible Production of the grooves enables. In particular, such exact dimensioning of the grooves can be achieved that a high suppression of cross polarization takes place. The known horn radiator is thus specially designed to provide a radiation diagram with as little cross polarization as possible, whereas the surface illumination or assignment of the reflector antenna to be excited by the horn radiator is less important.

The object of the invention, however, is to improve the illumination of deep reflector antennas or mirrors, in particular with a ratio f / D <0.35, where f is the focal length and D is the opening of the mirror, in such a way that a high cross polarization is maintained while maintaining the lowest possible cross polarization Area efficiency is achieved with low overexposure efficiency and high secondary attenuation.

This object is achieved in that the half opening angle θ _{o of} the horn flange enclosed between the longitudinal axis of the feed waveguide and the inside of the funnel is in the range of 70 ° <θ _o <80 ° and the feed waveguide of the TE ₁₁ -wave type protrudes from the horn throat, whereby this waveguide projection is set to an optimal width of the radiation pattern of the horn, which corresponds to the aperture of the mirror of the reflector antenna.

With regard to the illumination or assignment of the reflector antenna, ie the mirror, the ideal state would be to provide a uniform field of illumination on the entire mirror with a sudden drop in field strength to zero at the edge of the mirror. This would presuppose that the exciting horn emitter has a cone-shaped radiation characteristic that has a constant illumination field within its opening angle corresponding to the opening of the mirror Strength However, this ideal case cannot be realized: the uniformity of the illumination becomes more and more difficult, especially with deep mirrors. However, deep mirrors with f / D <0.35 are desirable because the horn emitter forming the pathogen is stronger against ground radiation, ie additional thermal noise. is shielded than with flat mirrors, but surprisingly it has been shown that the inventive dimensioning of the opening angle of the horn flange and the suitable adaptation of the feed waveguide projection compared to the horn throat can achieve unusually favorable illumination properties, for example an area efficiency of 50 to 60%, a very high one Overexposure efficiency (overexposure of the mirror edge about 2%) and a high auxiliary zip field attenuation of about 25 dB. Since, in addition, the cross polarization is strongly suppressed, ie the radiation characteristic is practically cylindrical symmetry, the horn emitter according to the invention is particularly suitable for circularly polarized waves, such as those emitted by television satellite transmitters in the direct radiation range. The definition of the above-mentioned quantities: area efficiency. Overexposure efficiency and secondary zip field attenuation follow the definitions customary in the field of antennas, such as that used for example by JOHNSON. RC, JASIK H., Antenna Engineering Handbook, McGraw Hill New York. 1984. Pages 1-5 to 1-7 or RUDGE. AW, MILNE, K., OLVER, AD, KNIGHT, P., The Handbook of Antenna Design, Peregrinus, London, 1982, Vol. 1, pages 21-24.

Particularly good results are achieved for deep mirrors in a narrower angular range of the horn flange, which is characterized in that half the opening angle θ _{o is} in the range of 73 ° ≤ θ _o ≤76 °.

Similarly, for the adjustment of the hollow a preferred range was found, which is dimensioned such that the waveguide projection in the range of - 0.25 £ • 0.35 is where the operating wavelength and L is the vertical distance between the aperture level of the horn flange and the aperture level of the waveguide, and the sign is chosen to be positive for the distances L located outside the funnel between the horn flange and its aperture level, and negative for distances L inside the funnel interior.

In particular, the invention can be used in connection with a horn, in which the feed waveguide is a round waveguide. In this context, it then proves to be expedient for the horn flange to be rotationally symmetrical with respect to the axis of the feed waveguide. In particular, a preferred embodiment is that the horn flange has the shape of the casing of a rotation cone.

In the context of the invention, it is not only provided that the waveguide protrusion experiences a unique and permanent setting, but in a further development of the inventive idea, the possibility has also been created to change the dimension of the waveguide protrusion as necessary and to readjust it. This further embodiment is characterized in that the horn flange is axially displaceable on the feed waveguide.

For the constructive implementation of this idea, it is provided in one embodiment of the invention that the horn flange is arranged on a sleeve which is positively guided on the outer jacket of the feed waveguide. This ensures the high-frequency connection of the horn flange to the feed waveguide and at the same time enables a change in the waveguide projection by shifting the horn flange. To ensure a defined high-frequency connection, the horn flange is preferably connected to a contact spring sliding on the outer waveguide jacket.

To carry out a precisely controllable displacement of the horn flange on the waveguide, an electric drive device for the displacement movement of the horn flange is also provided in a practical embodiment. This is expediently designed in such a way that the horn flange has a toothed rack which extends parallel to the axis of the feed waveguide and meshes with a gearwheel which is driven by an electric motor and is stationary with respect to the feed waveguide.

Finally, certain dimensional ranges standardized to the operating wavelength were found to be particularly expedient for practical exemplary embodiments of the horn emitter according to the invention. These are that the outer diameter d of the Hornflansches _ges, the inner diameter of the waveguide the axial groove depth s, the radial groove distance b and the radial groove thickness t in the areas

lie, the operating p wavelength is t. Other features, details and advantages of

Invention emerge from the following description and the drawing, with respect to an essential to the invention

Disclosure of all details not mentioned in the text is expressly noted. Show here:

1 is a partially longitudinally sectioned side view of a horn,

2 shows an E and H plane diagram of the horn, the radiation angle measured against the longitudinal axis of the feed waveguide being plotted on the abscissa and the power radiated at this angle being plotted on the ordinate, and

Fig. 3 is a graphical representation of the position of the phase center of the horn. in Fig. 3 (a) the position of the phase center as a function of the waveguide projection and in Fig. 3 (b) the sizes plotted on the abscissa and the ordinate.

According to FIG. 1, a horn emitter designated as a whole by reference number 1 has a feed waveguide 2 of the TE ₁₁ wave type. which is designed in the form of a circular waveguide with a cylindrical inner cross section. The on the operating wavelength J standardized inside diameter of the

Round waveguide is designated in Fig. 1 with. The

Outer jacket 3 of the circular waveguide is in its the in Fig.

1 on the right-hand side of the microwave feed side, the free end region is designed as a sliding surface that extends axially from the open free end 5 of the feed waveguide that defines the aperture level 4 of the feed waveguide 2

2 extends up to an annular shoulder 6 of the outer jacket 3. On the end area of the outer casing 3 which forms the sliding surface, a horn flange 7 is arranged which has a sleeve 8 which is guided in a form-fitting manner on the sliding surface and which surrounds the outer casing 3 of the feed waveguide 2 in a ring shape. To ensure a defined radio frequency Contact between the sleeve 8 and the feed waveguide 2 is in a to the outer jacket / open recess 9 of the sleeve

8 a leaf-shaped contact spring 10 is arranged, which rests under spring pressure on the sliding surface of the outer casing 3.

The horn flange 7, which is rotationally symmetrical with respect to the central axis of the feed waveguide 2 in FIG. 1, extends radially outward from the sleeve 8, the funnel shape opening towards the free end 5 of the feed waveguide 2 on the outlet side and with the central one Axis 11 includes a half opening angle θo. In the inside of the horn of the horn flange 7, recesses are provided in the form of grooves 12 concentric with respect to the central axis 11 and having an axially sectional rectangular cross section of the same axial depth and the same radial width. The radial width standardized to the operating wavelength these grooves 12 are denoted by b in FIG. 1. The individual grooves 12 are formed by axially parallel axially parallel partition walls 13 in the form of rings which are also concentric with respect to the central axis 11 and which are integral components of the horn flange 7. The radial thickness of these partition walls 13 standardized to the operating wavelength L is shown in FIG. 1 as t / designated. In addition, in Fig. 1 d the outer diameter of the feed waveguide 2 standardized to the length of operation in the region of the cylindrical sliding surface formed on the outer jacket 3.

Thus, such grooves 12 are separated from one another in the horn flange 7 by the illustrated five partition walls 13 of the same radial wall thickness 5, the partition walls 13 determining the axial depth of the grooves 12 each having the same axial length, which when normalized to the operating wavelength in FIG. 1 with s is designated. The radially outermost groove 12 'is delimited on the outside by the cylindrical outer wall 14 of the horn flange 7, which has the same radial thickness and the same has an axial length like the dividing walls 13. Between the radially innermost dividing wall 13 'and the outer jacket 3 forming the sliding surface of the feed waveguide 2, a further annular recess 15 of axially sectional rectangular shape is delimited, which has the same radial width as the grooves 12, 12'.

The free ends 16 of the dividing walls 13, 13 'and the cylindrical outer wall 14 facing the free end 5 of the feed waveguide 2 thus lie on a straight line 17 indicated in FIG. 1, which with the central axis 11 of the feed waveguide 2 is half the opening angle θ _o of Horn flange includes. So are. these free ends 16 are each offset from one another by a distance denoted by Δ _s in FIG. 1. The radially aligned bottom surfaces 18, 18 'of the grooves 12, 12' and the annular recess 15 are consequently axially offset from one another by the same amount Δ _s . The rear side 19 of the horn flange 7 opposite the free ends 16 is, seen in axial section, parallel to the straight line 17. This configuration of the horn flange forms a hybrid wave-type horn. Half the opening angle θ _{o of} the horn flange is in the range 70 ° <θ _o <80 °, preferably in the narrower range of 73 ° ≤ θ _o ≤76 °.

The front of the horn radiator 1 opposite the rear side 19 is closed off with a dielectric protective cover 20, for example of a mirror-image shape with respect to the horn flange 7 with respect to a radial plane. The wall thickness of the protective cover 20 has a -Λ with respect to the operating wavelength. small thickness on. The on the operating wavelength standardized thickness is designated in FIG. 1 with t _d / λ ₀ . As is further apparent from Fig. 1, this is the

Aperture level 4 defining free end 5 in front of the horn throat formed by the section line 21 of the straight line 17 with the feed waveguide 2. This hollow guide. The overlap is shown in FIG. 1 by the axial distance L / ₀ standardized to the operating wavelength by the free end 5 of the feed waveguide 2 determined aperture plane 4 of the feed waveguide 2 and by the free end 16 of the cylindrical outer wall 14 of the horn flange 7 determined radial aperture plane 22 of the horn flange 7. The preferred range for the waveguide projection was experimentally the interval -0.25 ___ L + 0.35 found, the sign chosen to be positive if the aperture level 4 of the feed waveguide 2 lies outside the space enclosed between the aperture level 22 of the horn flange 7 and the bottom surfaces 18, 18 'of the horn flange 7 and is chosen to be negative if the aperture level 4 of the feed waveguide 2 lies within this space. In the case of the waveguide projection shown in FIG. 1, the sign is accordingly positive.

As can finally be seen from FIG. 1, an electrical drive device for the displacement movement of the horn flange 7 on the feed waveguide 2 is provided. In the exemplary embodiment shown, this has an axially extending toothed rack 23 which is connected to the sleeve 8 and meshes with a toothed wheel 24 driven by an electric motor. The electric motor and the gearwheel 24 are fixed in place by a holding part 25 which is fixed to a radial flange part 26 on the outside of the feed waveguide 2. The motor can thus be excited to a controlled rotation by an electrical signal and the horn flange 7 on the feed waveguide 2 can thereby be axially displaced. It was determined by series of tests that in the above-mentioned dimensioning of half the opening angle θ _{o of} the horn flange 7, the waveguide protrusion

L can be set in such a way that a high surface efficiency with high secondary lobe attenuation and only very little overexposure even in the case of deep mirrors, ie mirrors in which the ratio of focal length f to the aperture determined by the diameter of the mirror is <0.35 (f / D <0.35). In particular, these tests were carried out using various practical models in which the total diameter dges of the horn flange 7 normalized to the operating wavelength in the range 1,86≤ d _tot / ≤ 3.6 and the other dimensions defined in Fig. 1 .. were in the following ranges:.

Such a measurement result is shown for an operating frequency of 10.69 GHz, ie an operating frequency in the X-band. Half the opening angle θ _{o of} the horn flange was θ _o = 73.5 ° and the waveguide projection L = 2 mm. The radiation angle measured against the longitudinal axis of the feed waveguide is plotted on the abscissa and the power radiated at this angle is plotted in relative units on the ordinate. The curves labeled E and H represent the measured values for the E and H planes.

Usually, a drop in intensity of - 14 dB compared to the central assignment is considered acceptable for the edge assignment of the mirror of the reflector antenna. On the basis of this compromise value, it follows from FIG. 2 that a mirror with an angular aperture of -86 ° to + 86 ° can be satisfactorily illuminated with the horn radiator used there. Moreover 2 within this - 14 dB edge assignment, the deviation between the E level and the H level is in any case less than 2 dB and thus meets the usual symmetry requirements for the radiation diagram. As the experiments have further shown, if the area is left 70 ° <θ _o <80 °, there is an inadmissible deterioration in the symmetry of the E plane against the H plane. In addition, there is a sharp narrowing of the angular range lying within the - 14 dB margin.

Finally, the experiments have shown that the horn described has very good bandwidth properties. For example, the measurements have shown that the power measured in the E-plane and the H-plane has a substantially flat frequency response over a diagram bandwidth of approximately 20% of the center frequency. The maximum cross polarization is better than -18 dB compared to the main lobe maximum of the useful polarization. The relative impedance bandwidth of such exciters can be kept offset from the round waveguide aperture 5 in the range of ± 5% below -20 dB (return loss) by inserting a narrow-band aperture approximately 1/4 of the waveguide wavelength.

In order to actually take advantage of the high surface efficiency which can be achieved by the horn radiator in the manner described above in a reflector antenna, it is necessary to move the phase center of the horn radiator 1 into the Airyzone of the reflector mirror, that is to say in its focal zone. However, as can be seen from FIG. 3, when the horn flange 7 is displaced on the feed waveguide 2, the position of the phase center p.c. on the central axis 11 of the

Feed waveguide 2. Specifically, above the abscissa of the curve diagram shown in FIG. 3a, the projection L / darge normalized to the operating wavelength is shown 3b, the definition of the size L as the distance between the aperture level 4 of the feed waveguide 2 and the aperture level 22 of the horn flange 7 is clarified again in FIG. 3b. The numerical values given below the abscissa of FIG. 3 represent half the opening angle at which the occupancy of the mirror has dropped to the marginal occupancy of -14 dB, which is usually used for comparison. The ordinate of the curve diagram of FIG. 3a gives the position z _pc / normalized to the operating wavelength J o o of the phase center on the

Axis 11 of the feed waveguide 2 with respect to the aperture plane 22 of the horn flange 7, which is also illustrated in FIG. 3b.

As for the values for half the opening angle of the mirror, which belong to the -14 dB edge assignment can be seen, this opening angle decreases rapidly with increasing misadjustment of the phase center, a decrease from 85 ° to 60 ° being shown in the diagram. It is therefore provided in a further embodiment that the horn 1 is slidably arranged in the reflector antenna for a given setting of the horn flange 7, so that it is displaced along the axis 11 of the feed waveguide 2 relative to the mirror of the reflector antenna and thus always in the central Airyzone or firing ball of the Mirror can be moved. For this tracking, for example, a further electrical drive device, not shown in FIG. 1, can be provided, similar to the drive device 23 to 25 of the horn flange 7, but on the entire horn radiator

1 attacks and this with a fixed with respect to the waveguide 2 horn flange 7 overall along the axis

1 1 moves.

Instead of striving for the smallest possible over-radiation efficiency, as described above, the optimization of the setting of the waveguide projection can also consist in that when the illumination of the fixed mirror changes, the radiation diagram, such as the width of the main lobe, the position of the side lobes, etc., to a desired optimum is set.

Claims

Patent claims:

1. Horn radiator for excitation of the focus of a reflector antenna, with a horn flange arranged in the output-side end region of a tubular feed waveguide, which widens in a funnel shape from its horn throat located on the feed waveguide and has grooves aligned on its inside of the funnel parallel to the axis of the feed waveguide, characterized in that between the longitudinal axis (11) of the hollow waveguide (2) and the inside of the funnel included half opening angle θ _{o of} the horn flange (7) is in the range of 70 ° ≤θ _o ≤80 ° and the hollow waveguide (2) of the TE ₁₁ -wave type protrudes from the horn throat, whereby this waveguide projection is set to an optimal width of the radiation pattern of the horn (1) corresponding to the aperture of the mirror of the reflector antenna.

2. Horn emitter according to claim 1, characterized in that half the opening angle θ _{o is} in the range of 73 ° ≤ θ _o ≤ 76 °.

3. Horn emitter according to claim 1 or 2, dadurcgek Indicates that the waveguide projection is in the range of - 0.25 + 0.35, wherein the operating wavelength and L is the vertical distance between the aperture plane (22) of the horn flange (7) and the aperture plane (4) of the waveguide (2) and the sign for outside the funnel interior enclosed between the horn flange (7) and its aperture plane (22) located distances L positive and negative for distances L located within the funnel interior.

4. Horn emitter according to one of claims 1 to 3, d a d u r c h g e k e n n z e i c h n e t that the feed waveguide (2) is a round waveguide.

5. Horn emitter according to one of claims 1 to 4, that the horn flange (7) is rotationally symmetrical with respect to the axis (11) of the feed waveguide (2).

6. Horn emitter according to claim 5, so that the horn flange (7) has the shape of the jacket a rotary cone.

7. Horn emitter according to one of claims 1 to 6, d a d u r c h g e k e n n z e i c h n e t that the

Horn flange (7) on the feed waveguide (2) is axially displaceable.

8. Horn emitter according to one of claims 1 to 7, d a d u r c h g e k e n n z e i c h n e t that the

Horn flange (7) is arranged on a sleeve (8) which is positively guided on the outer casing (3) of the feed waveguide (2).

9. Horn emitter according to claim 7 or 8, so that the horn emitter (7) is connected to a contact spring (10) which slides on the outer waveguide jacket (3).

10. Horn emitter according to one of claims 1 to 9, characterized in that an electrical drive device is provided for a displacement movement of the horn flange (7).

11. Horn emitter according to claim 10, characterized in that the horn flange (7) has a rack (23) which extends parallel to the axis (11) of the feeder waveguide (2) and which is stationary with a drive by an electric motor with respect to the feeder waveguide (2) Gear (24) combs.

12. Horn radiator according to one of claims 5 to 11, characterized in that the outer diameter of the horn flange d _ges the inner diameter of the waveguide, the axial groove depth s, the radial groove spacing b and the radial groove thickness t in the areas

1.86 ≤: d total £. 3.6

0.59 ^'~ dTE - 0.82 T ^E 11

A,

0.25 t__ 0.35 o

£ 0.07 _ b <=. 0.12

_PVo

0.016≤_. 0.024

--_ O

where A is the operating wavelength.

13. Horn emitter according to one of claims 1 to 12, characterized in that the phase center (p.c.) of

Horn emitter (1) for each predetermined setting of the horn flange (7) on the feed tube (2) by tracking the entire horn (1) along the axis (11) of the feed tube (2) relative to the mirror of the reflector antenna in the focal zone of the mirror is.

14. Horn emitter according to claim 13, characterized in that one of the follow-up serving further electrical drive device is provided t.