Ingenieurbüro für EMV

Dipl.-Ing. Heinz Lindenberger

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Shielded Enclosure

Shielding

Mu--Cu-01-mm
Fe-3mm+Al-6mm
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If you wish to take into account the Magnetostatic Shielding Effect, in addition to the eddy current shielding, much more complicated formulas are required


Below are the calculated approximations for homogeneous magnetic field shown for housings with the dimensions

L1 = L2 = 300 mm and B = 400 mm

Calculated Shielding Effect            Kurve 1:  Mu-Metal   100 µm thickness   µr = 80000           Kurve 2:  Copper   100 µm thickness   µr = 1


However, the Mu-Metal's excellent effect comes at a price: Like all high-permeability materials, Mu-Metal saturates even at comparatively low field strengths - and then has virtually no effect


The maximum permissible magnetic field strength follows from   Hmax  =  Bmax / (μ0 μr)

Assuming a Bmax of 0.3 Tesla (for linear behavior) and μr of 80,000 gives a permissible Hmax of about 3 A/m

Whereas magnetic field strengths of up to 1000 A/m can be expected in the shielding area of power electronics

Calculated Shielding Effect             Kurve 1:   Steel   3 mm thickness   µr = 300           Kurve 2:   AlMgSi   6 mm thickness   µr = 1  


Despite the significantly better conductivity of the aluminum alloy (30 x 10^6   to   8.6 x 10^6   S/m), the steel shields better because of its magnetic property. Even with half the wall thickness, a higher shielding effect is achieved throughout.    


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