A cassegrain antenna
A Cassegrain antenna and antenna technology, applied in the direction of antenna, antenna grounding switch structure connection, waveguide horn, etc., can solve the problems of narrow beam and target loss
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Embodiment 1
[0030] Embodiment 1, a Cassegrain antenna, comprising a feed antenna 11, a main reflector 13, a secondary reflector 12, and a main and secondary reflector fixing device 14; the feed antenna 11 is a conical horn in a horn antenna, The main reflector 13 is in the form of a paraboloid, and the secondary reflector 12 is a frequency selective surface with a side length of 4-7mm square holes at the center, such as figure 1 As shown, the frequency selective surface can generate resonance at some specific frequency points, so that the electromagnetic wave at this frequency point is transmitted, resulting in a wider beam width, while it is reflected at other frequency points, and the beam width narrower.
[0031] The feed antenna 11 is a conical horn, a kind of horn antenna. The feeding structure of the conical horn includes a hollow cone with a base radius of 10 mm and a height of 8-10 mm. Round tube waveguide. The structure is simple, the feeding method is simple, it has a moderate...
Embodiment 2
[0035] Embodiment 2, the frequency selective surface 15 in the embodiment 1 is composed of the frequency selective surface 15, and the inclination angle is 8-12°, such as Figure 6 As shown, the incident angle of the electromagnetic wave has a certain change, but it has little effect on its transmission characteristics, and its reflection characteristics change the direction of the reflected wave due to the change of the angle, and the reflected wave received by the feed antenna is small, effectively improving Standing wave characteristics; the electromagnetic wave is radiated from the conical horn 11 to the sub-reflecting surface, because the sub-reflecting surface has a certain angle to the incident wave, so the vertical reflection of the electromagnetic wave can be avoided, and the return loss of the antenna can be reduced to less than - 18dB effect.
Embodiment 3
[0036] In Embodiment 3, the frequency selective surface 15 described in Embodiment 1 is composed of a hyperboloid secondary reflection surface, such as Figure 7 As shown, the improvement according to the geometric principle can achieve the effect of reducing the return loss of the antenna to less than -17dB.
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