Related Experiment Video
Updated: Jun 9, 2025

07:28
Terahertz Microfluidic Sensing Using a Parallel-plate Waveguide Sensor
Published on: August 30, 2012
10.7K
An Ultra-Broadband Conductor-Backed Coplanar Waveguide with Sine Edges.
Tingting Xie1, Pengwei Gong1, Xiaohe Cheng2
1Beijing Institute of Radio Metrology and Measurement, Beijing 100854, China.
Sensors (Basel, Switzerland)
|October 26, 2024
Summary
A novel conductor-backed coplanar waveguide with sine edges (CBCPW-SE) offers a constant 50 Ω impedance across a wide frequency range. This new transmission line (TL) minimizes signal loss and dispersion for high-frequency applications.
Area of Science:
- Electrical Engineering
- Electromagnetics
- Microwave Engineering
Background:
- High-frequency transmission lines (TLs) are crucial for millimeter-wave and terahertz (THz) applications.
- Traditional TLs often require complex impedance matching networks, increasing system complexity and loss.
- Maintaining signal integrity and minimizing dispersion are critical challenges at these frequencies.
Purpose of the Study:
- To propose and characterize a novel conductor-backed coplanar waveguide with sine edges (CBCPW-SE).
- To demonstrate the CBCPW-SE's capability for constant 50 Ω impedance over a broad frequency spectrum.
- To evaluate the performance of the CBCPW-SE in terms of insertion loss, reflection coefficient, and group velocity dispersion (GVD).
Main Methods:
- Design and fabrication of the CBCPW-SE transmission line.
- Experimental characterization using S-parameter measurements from 10 MHz to 100 GHz.
- Analysis of insertion loss, reflection coefficient, group delay, and GVD.
Main Results:
- The fabricated CBCPW-SE maintained a constant 50 Ω input impedance without impedance matching transitions.
- Measured insertion loss was below 0.1 dB/mm and reflection coefficient better than -10 dB across the tested frequency range.
- Minimal signal degradation was observed, with S21 (dB) < -5 dB for a 50 mm section and near-zero GVD.
Conclusions:
- The CBCPW-SE is a promising transmission line for millimeter-wave and THz frequencies due to its inherent 50 Ω impedance and low loss.
- The design simplifies high-frequency systems by eliminating the need for impedance matching circuits.
- The minimal GVD ensures excellent signal integrity for high-speed data transmission.
Related Concept Videos
Standing Waves in a Cavity
876
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:
876
Plane Electromagnetic Waves I
3.6K
The existence of combined electric and magnetic fields that propagate through space as electromagnetic (EM) waves is the most significant prediction of Maxwell's equations. As Maxwell's equations hold in free space, the predicted electromagnetic waves do not require a medium for their propagation. An EM wave comprises an electric field, defined as the force per charge on a stationary charge, and a magnetic field, which is the force per charge on a moving charge.
The EM field is assumed...
The EM field is assumed...
3.6K
Transmission Line Design Considerations
128
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...
128
Propagation Speed of Electromagnetic Waves
3.3K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
3.3K
Standing Electromagnetic Waves
1.5K
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...
1.5K

