两种不同线栅结构的水平极化辐射波模拟器

Horizontally polarized radiation-wave simulator with two different wire grating structures

  • 摘要: 比较了末端收拢和均匀拉线的双锥-平面线栅水平极化辐射波模拟器辐射场的分布规律,讨论了拉线根数和收拢组数对辐射场的影响。结果表明,双锥中心正下方测点辐射场基本不受线栅结构变化的影响。对于其他位置,两种结构的模拟器各有特点:拉线根数相同时,末端均匀拉线的模拟器可令辐射场强提高约5%~20%,但前沿会变慢10%左右;末端收拢的模拟器场强幅值相对较低,但具有较快的前沿,并且架设相对容易。增加拉线根数和收拢组数有利于提高辐射场强,但场强增加的幅度逐渐减小。拉线根数由24增加到96时前沿可加快约10%,半宽变化不大。增加收拢组数会使前沿变慢。综合辐射场变化规律及施工难易程度,可令末端均匀拉线模拟器的拉线根数取48,此时对收拢结构的天线,可令收拢组数取16。

     

    Abstract: This paper compares the E-field distributions of two horizontally polarized radiation-wave simulator with different wire grating structure. The antenna wires of one simulator are uniformly distributed on the ground, while the other simulator’s antenna wires are converged to several groups at the end. Meanwhile, the influences of wire number and group number on the radiated field are discussed. Results show that the E-fields below the bicone apex are not affected by the wire grating structure. While in other positions, the E-field characteristics of the two simulators are different: when the wire number is the same, the simulator with uniform wire will increase the E-field amplitude by 5% to 20%, but its rise time increases about 10% at the same time; the simulator whose antenna wires are converged shows lower E-field amplitude, but its rise time is shorter. Besides, the latter is easy to establish in practice. On the other hand, increasing the wire number and wire group is helpful to improve the radiation amplitude, but the improvement reduces gradually. If the wire number increases from 24 to 96, the rise time can be improved by about 10%, but the half width of radiated E-field shows little difference. The increase of group number will lead to longer rise time. Taking into account the variation law of the E-field and the complexity to establish, the wire number of the simulator with uniform wire can be set to 48, and for the simulator whose antenna wires are converged, the group number can be set to 16.

     

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