EMF shielding using a conductor

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SUMMARY

This discussion focuses on the principles of electromagnetic field (EMF) shielding using conductors, particularly in relation to circular coils with alternating current (AC) at radio frequencies. The key mechanism involved is the induction of Eddy currents in the conductor, which oppose changes in magnetic flux as described by Lenz's Law. While the induced magnetic field can mitigate fluctuations, it does not completely eliminate the residual magnetic field behind the conductor. The conversation also touches on the relationship between conductivity and the shiny appearance of metals, attributing this to the behavior of light at conducting surfaces.

PREREQUISITES
  • Understanding of Lenz's Law
  • Familiarity with Eddy currents
  • Knowledge of alternating current (AC) principles
  • Basic concepts of electromagnetic fields
NEXT STEPS
  • Research the properties and applications of Eddy currents in EMF shielding
  • Explore the design and effectiveness of Faraday cages for radio frequency interference
  • Study the relationship between conductivity and optical properties in metals
  • Investigate the effects of AC frequency on magnetic field induction
USEFUL FOR

Electrical engineers, physicists, materials scientists, and anyone interested in the principles of electromagnetic shielding and the optical properties of metals.

KDPhysics
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Homework Statement
How does placing a conductor in the path of a magnetic field of a circular coil shield anything behind the plate?
Relevant Equations
Lenz's Law
So I've been trying to figure out how EMF shielding works. More specifically, I've seen videos where placing a metal conductor in front of a circular coil (with AC running through at radio frequencies) apparently shielded anything behind it.

After searching online, I repeatedly saw Eddy currents popping up.

If I've understood everything correctly, when you place a conductor near a changing magnetic field (such as that of a circular coil), nature abhors any change in magnetic flux. Consequently, a current will be induced, called Eddy current, in the conductor, such that the induced magnetic field opposes the change in magnetic flux.

For example, I have the following set up (a circular coil attached to an AC supply and a conductor beneath it):
IMG_20200524_223939.jpg

Now consider an arbitrary instant in which the coil's magnetic field is decreasing. Then, by Lenz's law an Eddy Current will be induced in the conductor trying to "undo" this decrease in magnetic flux. Consequently, the current will be such that the induced magnetic field points in the same direction as the external magnetic field.
But then there still is residual magnetic field behind the conductor due to both the decreasing external field and the induced field. So, shielding has not occurred?
 
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The fluctuations will be mitigated by the induced currents and Lenz's Law. A good Faraday Cage can greatly reduce Radio frequency interference.
This is also why metals appear shiny.
Not static fields!
 
Oh, I see. So exactly because the external magnetic field is decreasing, the fact that we have an induced magnetic field keeps the change in magnetic flux approximately constant, thus shielding anything behind.

EDIT: Also, could you elaborate on why this causes metals to be shiny? Sounds very interesting.
 
Yes. And of course a conductor will also shield both static and dynamic E fields.
 
One question: if initially (before turning on the AC supply) there is no magnetic field outside, and then after some instants, as we saw in my diagram, there is a net magnetic field outside, this means that there must be some net change in flux right? Perhaps the moment the AC supply is turned on there is a surge in induced current, and then this stabilizes?
 
Exactly.
And the light is reflected from a conducting surface because field components are forced to be zero at the surface...this produces a reflected wave like sound off a hard wall...its a little more complicated for light but that is the fundamental issue.
 
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Oh ok thanks.
 

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