Frequency selective surface radome

In summary: Yes, the reflected power is two times as high because the wave has gone out and back through the material.
  • #1
garryA
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TL;DR Summary
Transmission coefficient vs Reflection coefficient of FSS radome
So I was reading about frequency selective surface radome, basically this is the kind of cover over the antenna which allow a certain frequency wave to pass through and reflect wave at any other frequencies.

What I don't understand is the reflection vs transmission coefficient chart.
So as I understand it.
The transmission coefficient is a measure of how much of an electromagnetic wave passes through a surface
The reflection coefficient is a a measure of how much of an electromagnetic wave reflected when it hit a surface, The reflection coefficient determines the ratio of the reflected wave amplitude to the incident wave amplitude.

So logically, wouldn't the two value always opposite?
Let me give a practical example:
below, the band pass frequency is 10Ghz, so the transmission coefficient is 0 dB while the reflection coefficient is extremely small (like -40 dB). That make total sense because if it reflect nothing then most energy can pass through the layer

But take for example at 6Ghz, the reflection coefficient is at 0 dB, meaning it reflect everything, so how come the transmission coefficient is not at -40 dB?.
Shouldn't the shape of the two curve for reflection/transmission coefficient completely reverse each other?

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  • #2
garryA said:
So logically, wouldn't the two value always opposite?
Energy that is lost to heat within the material, is neither transmitted, nor reflected.
 
  • #3
Baluncore said:
Energy that is lost to heat within the material, is neither transmitted, nor reflected.
I got your point, but to be able to be converted to heat, the wave must entered the material first, so the fraction of energy that get reflected can’t be transmitted or converted to heat.
Let me clarify my point with an example:
Let say the amount of energy of the wave at the start is 100%. Once it hit the radome, 99.99% of that get reflected. So I would expected that the amount that can be transmitted is at most 0.001%. But the chart basically telling me that 99.99% energy get reflected but 10% get transmitted. That why for me it make no sense
 
  • #4
If the radome is loss free, the transmitted power and the reflected power should always add up to incident power. To compare transmitted power and reflected power you have to deduct the two powers. To do this you cannot use decibels, you must first convert from decibels (relative to incident power) to watts. Then subtract the watts.
For example, incident power Pi = 1 watt, and transmitted power 1 W -1 dB = 0.8W.
So reflected power = 1 - 0.8 = 0.2W. Or if preferred, 0.2W = -7dB.
 
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  • #5
tech99 said:
If the radome is loss free, the transmitted power and the reflected power should always add up to incident power.
Yes, that is my deduction as well

tech99 said:
To compare transmitted power and reflected power you have to deduct the two powers. To do this you cannot use decibels, you must first convert from decibels (relative to incident power) to watts. Then subtract the watts.
For example, incident power Pi = 1 watt, and transmitted power 1 W -1 dB = 0.8W.
So reflected power = 1 - 0.8 = 0.2W. Or if preferred, 0.2W = -7dB. if I understand correctly,
the incident power will be reflected before it can be transmitted
So for example in the point in the graph bellow
let say the incident power is 100W, then the reflected power is also 100W
how come the transmitted power is still there?
Shouldn't the shape of two line completely opposite?

Capture.PNG
 
  • #6
garryA said:
let say the incident power is 100W, then the reflected power is also 100W
No, roughly 5W is transmitted through the radome, leaving a reflected power of about 95W by conservation of energy. That's an S11 of -0.22dB, only slightly below zero and nearly impossible to see on the dB graph. Observe also that the S11 and S21 lines cross at a value of -3dB, corresponding to 50% transmitted/50% reflected powers, which demonstrates that no power loss due to absorption is included in these model results.
TRdB.jpg
 
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  • #7
The graph is plotted inm decibels. If it was plotted in watts, then the two plots would be the inverse of each other.
 
  • #8
renormalize said:
No, roughly 5W is transmitted through the radome, leaving a reflected power of about 95W by conservation of energy. That's an S11 of -0.22dB, only slightly below zero and nearly impossible to see on the dB graph. Observe also that the S11 and S21 lines cross at a value of -3dB, corresponding to 50% transmitted/50% reflected powers, which demonstrates that no power loss due to absorption is included in these model results.
View attachment 323599
Thank you, it make sense to me now.
Also If i understand correctly , if we put a radar behind this radome, then the process of reflected happen twice right? one when the wave go out the randome, and one when it come back
 

Related to Frequency selective surface radome

What is a frequency selective surface radome?

A frequency selective surface (FSS) radome is a structure that selectively allows electromagnetic waves of certain frequencies to pass through while blocking others. This is achieved through a periodic array of conductive elements or apertures. The design of the FSS can be tailored to specific frequency bands, making it useful for applications like antenna systems, where it can protect the antenna while allowing desired signals to pass.

How does a frequency selective surface radome work?

A frequency selective surface radome works by exploiting the resonant properties of its periodic structure. When electromagnetic waves encounter the FSS, certain frequencies resonate with the structure, allowing them to pass through with minimal attenuation. Other frequencies, which do not resonate, are reflected or absorbed. The design parameters, such as the shape, size, and spacing of the elements, determine the resonant frequencies.

What are the applications of frequency selective surface radomes?

Frequency selective surface radomes have a wide range of applications, particularly in the fields of telecommunications and defense. They are used in antenna systems to protect sensitive components while allowing desired signals to pass. They are also employed in stealth technology to reduce radar cross-section and in satellite communications to filter out unwanted frequencies. Additionally, they find use in wireless communication systems to enhance signal quality and reduce interference.

What materials are used to construct frequency selective surface radomes?

The materials used to construct frequency selective surface radomes typically include conductive elements such as metals (e.g., copper, aluminum) or conductive coatings applied to dielectric substrates. The choice of materials depends on factors like the operating frequency range, environmental conditions, and mechanical requirements. Dielectric substrates might include materials like fiberglass, PTFE, or other composites that provide structural support while minimally affecting the electromagnetic properties of the FSS.

What are the design challenges associated with frequency selective surface radomes?

Designing frequency selective surface radomes involves several challenges, including achieving the desired frequency selectivity, maintaining structural integrity, and ensuring minimal signal loss. Engineers must carefully design the periodic elements to resonate at specific frequencies while considering manufacturing tolerances. Additionally, the radome must withstand environmental factors such as temperature fluctuations, moisture, and mechanical stress. Balancing these requirements while maintaining performance can be complex and requires advanced simulation and testing techniques.

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