一个紧的宽带毫米波交叉器,用于远程传感应用中的分相阵列天线系统
Fayyadh H Ahmed1, Rola Saad1, Salam K Khamas1
1Electromagnetics, Wireless Hardware & RF Devices Group, School of Electronic and Electrical Engineering, University of Sheffield, Sheffield S1 3JD, UK.
Sensors (Basel, Switzerland)
|June 27, 2025
概括
一个新的无线微带交叉器在宽带宽上实现了2dB的插入损失,非常适合毫米波应用. 这种紧的设计增强了用于遥感的分相阵列天线系统.
科学领域:
- 电气工程 电气工程
- 电磁学 电磁学 电磁学 电磁学
- 微波工程 微波工程
背景情况:
- 毫米波 (mmWave) 系统需要有效的信号路由.
- 传统的微带交叉通常涉及VIA,增加复杂性和成本.
- 远程传感中的分相阵列天线需要高性能料网络.
研究的目的:
- 设计和演示一个紧的,宽带的,没有VIA的微条式交叉车.
- 为了实现优良的散射参数,提高天线系统效率.
- 为了在遥感应用中实现更高的性能.
主要方法:
- 使用梯形微条线 (MST) 到地面支持的共平面波导 (GCPW) 过渡.
- 实现了微条纹和共平面的沙眼镜微条纹补丁之间的垂直合.
- 在单层基板上制造,以提供紧,无通道的配置.
主要成果:
- 在整个操作带宽 (9GHz重叠带宽从13-22GHz) 中实现了大约1dB的插入损失.
- 证明了10dB的回归损失和大约20dB的隔离.
- 紧的设计尺寸为6.5mm × 7.6mm,提供了一个不太可行的解决方案.
结论:
- 拟议的微带交叉提供有效的性能,低插入损失和高隔离.
- 该设计增强了阶段阵列天线输送网络中的功率传输和端口隔离.
- 这有助于提高遥感系统的灵敏度和精度.
相关概念视频
Design Example
375
The innovation of touch-tone telephony revolutionized the telecommunications industry by replacing the traditional rotary dial with a dual-tone multi-frequency (DTMF) signaling system. This system uses a matrix-style keypad with buttons arranged in four rows and three columns, creating 12 distinct signals each assigned to a pair of frequencies. Each button press results in a simultaneous generation of two sinusoidal tones – one from a low-frequency group (697 to 941 Hz) and one from a...
375
Transmission Line Design Considerations
220
Aluminum has become the material of choice for overhead transmission lines, surpassing copper due to its abundance and cost-effectiveness. The most prevalent type is the aluminum conductor, steel-reinforced (ACSR), which combines aluminum strands around a steel core. Other variants include all-aluminum conductors (AAC), all-aluminum alloy conductors (AAAC), aluminum conductor alloy-reinforced (ACAR), and aluminum-clad steel conductors. Advanced designs, such as aluminum conductors with steel...
220
Electromagnetic Waves
9.3K
James Clerk Maxwell formulated a single theory combining all the electric and magnetic effects scientists knew during that time, calling the phenomena his theory predicted “Electromagnetic waves”. He brought together all the work that had been done by brilliant physicists such as Oersted, Coulomb, Gauss, and Faraday and added his own insights to develop the overarching theory of electromagnetism. Maxwell’s equations, combined with the Lorentz force law, encompass all the laws...
9.3K
Generating Electromagnetic Radiations
4.1K
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in...
4.1K
Standing Electromagnetic Waves
1.7K
Electromagnetic waves can be reflected; the surface of a conductor or a dielectric can act as a reflector. As electric and magnetic fields obey the superposition principle, so do electromagnetic waves. The superposition of an incident wave and a reflected electromagnetic wave produces a standing wave analogous to the standing waves created on a stretched string.
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
1.7K
Standing Waves in a Cavity
1.1K
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.1K


