Power line EMI filter + feedthrough filter for a Faraday cage

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SUMMARY

The discussion focuses on the design and implementation of a 50Hz 250VAC power line EMI filter for a Faraday cage, specifically targeting frequencies between 100kHz and 20GHz with an attenuation requirement of at least 60dB from 1MHz to 5GHz. Participants suggest using a combination of a cheaper feedthrough filter and a regular power line filter, while emphasizing the importance of addressing issues such as seams and gaps in the Faraday cage to prevent electromagnetic interference (EMI) leakage. The conversation also highlights the necessity of understanding the frequency-dependent behavior of filters and the potential for series connections to achieve desired filtering outcomes.

PREREQUISITES
  • Understanding of EMI shielding principles and Faraday cage design
  • Familiarity with feedthrough filters and their frequency characteristics
  • Knowledge of parasitic properties of inductors and capacitors in high-frequency applications
  • Experience with power line EMI filters and their specifications
NEXT STEPS
  • Research the specifications and applications of Kemet EMI/RFI filter capacitors
  • Explore the design and implementation of series-connected filters for EMI applications
  • Study the effects of seams and gaps in Faraday cage construction on EMI performance
  • Investigate commercially available filtered feedthrough solutions for EMI shielding
USEFUL FOR

Electrical engineers, EMI shielding specialists, and hobbyists involved in the design and construction of Faraday cages or EMI filtering solutions.

  • #31
flowwolf said:
I remember reading that in more than one document, those showed that when doing precisely, the 2nd layer improves SE by some (30 or so) dB, but it will be less than double.
Double the energy is a change of 10*Log(2) = 3dB. I think you were expecting doubling the dB which is squaring the SE?

According to your ref; Kistenmacher and Schwab, 1996. IEEE. Page 351.
My statement is shown to be true for conductive non-magnetic materials, for Cu see fig. 12.
The effectiveness increases with frequency. Note the plot there assumes the same total mass of material.

My statement is false for magnetic resistive screen materials. See fig 13. Which is what you expect from ferrite slabs that are designed to allow EM propagation between the magnetic grains.

Your reference, the Bahadorzadeh, Moghaddasi and Attari, 2008, paper, appears to be discussing cascaded apertures in the wall of a cavity. Figure 2 shows two walls give about a 12dB advantage over one. That is significantly better than a factor of two and supports my suggestion that the same mass distributed amongst several walls is better than one thick wall. The paper goes on to show increased wall separation increases screening.

flowwolf said:
btw. Wouldn't a two-layered wall cause resonances and worsen SE at specific frequencies?
Resonant cavities need coupling to be part of the circuit. A 100mm thick timber stud wall supporting and separating two conductive sheets will not support a significant resonance. Galvanised steel is cheaper than copper and can be easily soldered along the seams.
 
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  • #32
Baluncore said:
Double the energy is a change of 10*Log(2) = 3dB. I think you were expecting doubling the dB which is squaring the SE?

Yes, for power 10*Log(2) = 3dB is the double.

Let's say that an enclosure with a single wall has an SE of 60dB. It seems logic that a nested enclosure (a double walled one) have an SE of 120dB, which is the doubling of dB (that is what I was expecting yes).

We can agree that double walls (the nested ones) improve SE anyway. What I wanted to ask that when done correctly, do I really need nested enclosures?

Baluncore said:
Resonant cavities need coupling to be part of the circuit. A 100mm thick timber stud wall supporting and separating two conductive sheets will not support a significant resonance.

What about something smaller like 20mm? Are there any rules on this, or do I have to do simulations to know the resonances? I didn't know that resonant cavities need coupling (you mean electrical connection?).

Baluncore said:
Galvanised steel is cheaper than copper and can be easily soldered along the seams.

+1 Yes, galvanised steel seems to be solderable.
 
  • #33
flowwolf said:
It seems logic that a nested enclosure (a double walled one) have an SE of 120dB, which is the doubling of dB (that is what I was expecting yes).
When you cascade two attenuators you square the attenuation, unfortunately that is not directly applicable to double walls. Is it better to use two conductive walls of half the thickness or one thick wall? Probably more walls, but it involves understanding SE as a function of wall thickness, which is frequency dependent.
A conductive wall has external circulating RF currents due to the external world on the outer surface, with internal circulating RF currents due to your activities on the inner surface. Those currents induced in one face only diffuse very slowly (100 m/s) through the material due to back emf, hence skin effect. You need to keep those surface currents separate which in reality comes down to the quality of the aperture seals, which provide the only short path around the wall.

That means your door and vent seals must be very reliable, because any break in conductivity concentrates surface currents and allows them to wrap around the edge of the conductive screening sheet. Keep apertures away from external edges where circulating currents are naturally higher, so the door should be in a face. It must have metallic wipers that eliminate the conductivity gap when closed. Any imperfect seal becomes a slot antenna or an aperture coupling inside to outside.

With double walls the door will also have two insulated conductive surfaces, each with it's own wipers. The only ground connection between the double walls will be the conduit used for the power supply which is the middle part of the cascaded filter box.

There is a construction requirement. A timber stud wall, floor and roof will all be self supporting. That suggests independent inner and outer conductive walls can be attached. Fold the material around the edges so your conducting joints are on less stressed flat faces. Avoid TIG or MIG welding, use plumbers solder along all the seams.

flowwolf said:
What about something smaller like 20mm?
You are talking waveguides with cutoff frequencies. But you must inject the energy and then couple it out again so avoid apertures.
 
  • #34
ETS-LINDGREN. Double Electrically Isolated RF Enclosures for Industrial, Communication, and Research and Development Applications.
http://www.ferret.com.au/ODIN/PDF/WebsiteCustomers/78.pdf
 
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  • #35
This is a great link, thanks. I like the way the panels joined, you're right, this method is excellent.

flowwolf said:
What about something smaller like 20mm?

I meant, what if the space is smaller than 100mm between the walls. 20mm would be a bit small but something like 40-50mm? Is there any rule?
 
  • #36
The shielding problem is hardest to solve in the audio frequency magnetic range. A current induced to flow around an outer face will couple into a parallel inner wall in the same way that a single turn transformer operates. Separation distance is not going to be critical so long as there is only one ground connection to an adjacent shell to prevent ground loops.

I think the design key is that a structural wall needs some thickness. Use that thickness to your benefit but do not exaggerate it. If you are building a portable room it will have cellular construction. If your room is fixed inside an existing building it can be an isolated double wall enclosure. There is a limit to the attenuation required, somewhere around the thermal noise floor in your instruments. Enough is sufficient, an extra layer of foil will not hurt, but it will cost time and money, and makes no difference to the shielding.You should take a look at these two publications I found on the web;

1. Theory, Design And Engineering Evaluation Of Radio-Frequency Shielded Rooms. Aeronautical Electronic and Electrical Laboratory. REPORT NO. NADC-EL-54129 13 AUG 1956. BUREAU OF AERONAUTICS TED Project No. ADC EL-538. 125 pages, 10.2Mbyte.

2. Military Handbook. Radio Frequency Shielded Enclosures. MIL-HDBK-1195. 30 SEPTEMBER 1988. U.S. Navy. 86 pages, 370kbyte.

Also, if you can find a copy, see; Architectural Electromagnetic Shielding Handbook. A Design and Specification Guide. Leland H. Hemming, 1992, IEEE Press. 229 pages.
 

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