Shielded magnetic loop probe / antennas

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Discussion Overview

The discussion revolves around the performance tradeoffs of different types of shielded H-field pickups or antennas, specifically comparing two designs referred to as type "A" and type "B". Participants explore the implications of shielding configurations on the effectiveness of these probes in various applications, including RF probing and magnetic field measurements.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express concerns about type "B" design, suggesting it may be susceptible to electrostatic noise due to its shielding configuration.
  • There is a discussion on the importance of symmetry in the design of shielded loops to prevent electric field detection and to minimize common mode noise.
  • One participant notes that the alternating B-field inside the loop does not have an associated electric field, attributing this to the small size of the loop relative to the wavelengths involved.
  • Another participant references a paper that suggests type "B" could be effective under certain conditions, particularly when the diameter of the loop is not negligible compared to the wavelength, indicating that the outer conductor may play a role in the pickup structure.
  • Different scenarios are proposed where the performance of the probes may vary, such as when the probe signal is above the noise floor versus when it is weak and susceptible to common mode interference.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the effectiveness of type "B" design, with some expressing skepticism while others suggest it may have merit under specific conditions. The discussion remains unresolved regarding the optimal design for different applications.

Contextual Notes

Participants highlight limitations related to the assumptions about shielding effectiveness, the dependence on specific configurations, and the varying goals of different probing scenarios. There is an acknowledgment that the design must consider both magnetic and electric field interactions.

Swamp Thing
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From a purely physics point of view, what would be the performance tradeoffs between the following types of shielded H-field pickups or antennas?

Sources:

(A)[/size]
sloop.gif


(B)[/size]
SimplerLoop-300x214.png

https://owenduffy.net/blog/wp-content/uploads/2020/05/SimplerLoop-300x214.png
 
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I have experience with this type of probe, and have built several for my work. But you need to go first -- what are your thoughts on this type of B-Field RF probe?
 
The type "B" looks a bit sus to me. The outer is used as half of the loop, so it is exposed to all the electrostatic noise. But there may be some other big advantage to that design, idk.
 
Screened loops are magnetic field antennas, hence the term "B-field RF probe". If the external electrostatic shield is asymmetrical, or carries signal current, the output from the probe will also be influenced by the electric field. Screened loops must be significantly smaller in diameter than the operating wavelength, so they have a simple dipole pattern.
Swamp Thing said:
The type "B" looks a bit sus to me.
It is more than suspicious, it is bad.
 
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It isn't common for shielding something "half way" to make sense. That's why the others have a tiny gap in the shield. Although I'm sure someone will give us a counter example.

1705378128935.png
 
DaveE said:
It isn't common for shielding something "half way" to make sense.
The shield cannot cover the full turn, or the shield will become a shorted turn on the pickup loop.

The gap in the shield is there to prevent a shield current flowing. The shield must be symmetric, so it cannot be open on one side, or it will detect the electric field.

Metal detectors also often use a multi-turn coil, inside a shield that has a narrow insulated gap.
 
I accept that shielded loops do work, for example in direction finders, but it is unclear to me why the alternating B-field inside the loop does not have an associated electric field.
 
tech99 said:
... why the alternating B-field inside the loop does not have an associated electric field.
Because the loop is small in wavelengths and the local E-field is 'shorted' by the external conductive shield.
 
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Found this paper
https://ieeexplore.ieee.org/document/1284886

also accessible here without login:
https://www.researchgate.net/public...neration_of_Magnetic_Fields_Using_Loop_Probes

If they are right, then there can be situations where Fig (B) in my question could actually make sense. A key point they assert is that if the diameter is not negligible compared to wavelength, then the outer conductor can't be regarded as a short, nor is it really working as a shield -- it is actually part of the pickup structure. So if your aim is to minimize common mode noise then symmetry is the key. The loop has to be designed to work as a balun as well as a pickup loop.

I realized also that there are different scenarios with different goals, for example:

(1) The probe signal is well above our amplifier's noise floor, the instrumentation itself doesn't produce much common mode noise, and we want to isolate the magnetic field from electrical fields near the probe. Example: probing currents and magnetics around a switched power supply circuit.

(2) The probe signal is quite weak, and our equipment (e.g. computer) emits common mode interference into the feed line. Example: a shortwave loop antenna connected to an SDR receiver which is connected to a computer via USB.

My interest happens to be focused on scenario (2) where you can't really have diameter <<<< wavelength because then the signal would be below the amplifier/SDR's noise floor. In this case symmetry is important, and Fig (B) can have some merit.
 

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