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Engineering Science in
            Additive Manufacturing                                             AM-CFRP structures for EMWA properties










































                                                           35
            Figure 2. Electromagnetic wave loss with various microwave mechanisms.  Copyright © 2021 The Chinese Ceramic Society. Reproduced with permission
            of Elsevier.
            magnetic conductor moving inside a fluctuating magnetic   2.6. Interference loss
            field, may be calculated using Equation IV:        Interferometric loss is dependent on the idea that
            C  =≈ 2πµ µ σD f                           (IV)    electromagnetic waves interfere with one another and
                      ’2
                         2
             o      o                                          cancel each other out, giving rise to a zero net return.
              By creating a magnetic field in the opposite direction of   It  places  particular  demands  on  the  actual  material.
            the initial alternating current (AC) field, the eddy current   Refraction and reflection occur when an electromagnetic
            protects  the  magnetizing  field  inside  the  magnet  and   beam traveling in parallel hits a material’s surface. An
            exponentially reduces the strength of the AC field, which   outgoing wave is produced from the surface of the material
            ultimately results in the skinning effect. The magnetic loss   by the lower metal plate reflecting the incident component
            factor, which is based on the ratio of µ′ to µ′′, indicates   of the electromagnetic wave. The propagation direction of
            the capacity of a medium to retain a magnetic field. The   the wave stays constant. Based on the absorbing material’s
            skinning depth of the material and magnetic loss factor   quarter  wavelength, the  absorption principle states that
            can be expressed as follows:                       these waves cancel each other at this point, significantly
                                                               lowering the total reflected wave. The entering and
                  ''                                          outgoing waves have a phase difference of precisely 180°
            tgδ =                                      (V)     since the thickness of the absorbing material is equal to a
                  '
                                                               quarter wavelength. To enable better EMA characteristics
                                                               and cause the incident and reflected waves in the material
                 2 ρ                                           to  be out  of phase, the  thickness  t  is set  to be  an  odd
            δ =                                        (VI)
                 ωµσ                                           multiple of the quarter wavelength in the material.
              where δ is penetration depth, ω is angular frequency,   tn   m                           (VII)
            ω=2πf, ρ is resistivity, and σ is conductivity.         4



             Volume 1 Issue 2 (2025)                        5                          doi: 10.36922/ESAM025160008
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