WHAT IS EMI/RFI SHIELDING?
WHERE EMI SHIELDING IS NEEDED?
WHY DO PLASTIC ENCLOSURES NEED TO BE SHIELDED?
WHAT ARE EMI SHIELDING PRINCIPLES?
WHY USE EMI/RFI SHIELDING COATINGS?
WHAT ARE DB'S AND OHMS/SQUARE/MIL?
















 
WHAT ARE EMI SHIELDING PRINCIPLES?

The importance of wave impedance is shown by an electromagnetic wave encountering an obstacle such as a metal shield. If the impedance of the wave differs greatly form the natural impedance of the shield, much of the energy is reflected and the rest is transmitted across the surface boundary, where absorption in the shield further attenuates it . Because most metals have an intrinsic impedance of only milliohms, less low impedance H-field energy is reflected and more is absorbed. This is because the metal is more closely matched to the impedance of the field. This is also why it is difficult to shield against magnetic fields. On the other hand the wave impedance of electric fields is high, so most of the energy is reflected for this case. At higher frequencies, typically over 10 MHZ, EMI shielding is governed mostly by absorption.

Shielding effectiveness of metallic enclosures is not infinite, because the conductivity of all metals is finite. They can, however, approach very large values. Because metallic shields have less than infinite conductivity, part of the field is transmitted across the boundary and supports a current in the metal. The amount of current flow at any depth in the shield, and the rate of decay is governed by the conductivity of the metal, its permeability, and the frequency and amplitude of the field source. The residual current appearing on the opposite face is the one responsible for generating the field which exists on the other side.

The current density in a metal shield is not affected by the shieldĄ¯s thickness. A secondary reflection occurs at the far side of the shield for all thicknesses. The only difference with thin shields is that a large part of the re-reflected wave may appear on the front surface. This wave can add to or subtract from the primary reflected wave depending upon the phase relationship between them. For this reason, a correction factor appears in shielding equations to account for reflections form the far surface of a thin shield.

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