The preliminary electromagnetic shielding behavior of metal foams, a novel class of materials, is developed and discussed. The use of metal foams in electromagnetic applications is a new fleld of scientiflc investigation. More speciflcally, the realization of electromagnetic shields has been considered and experimental Shielding Efiectiveness (SE) measurements have been performed, demonstrating very good performance. In order to allow the design of metal foam EM shields, a double 3D wire-mesh screens, obtained as a development of previously 2D laminated shield, has been present, compared the relative results with experimental measure. The good agreement between the preliminary results, encourages the development of an e-ciency analytical model of the complex electromagnetic behavior of metal foams. The analysis of the shielding properties of difierent kinds of Duocelr aluminium foams slabs obtained by varying porosity and apparent density, has been investigated, performed through ex- perimental measurements, and their shielding properties has been shown and discussed (2). Metal foams are complex an random structures which requiring sophisticated analytical mod- els. Moreover, because of its versatility and its capability to deal with heterogeneous media, the Variable-Mesh Finite Difierence Time Domain (VM-FDTD) method, is naturally the most ap- propriate approach (2), though unfortunately, it is computationally onerous. The 2D laminated wire-mesh screen model, developed by Casey (3) and compared with commercial aluminium shield perforated periodically with apertures (4), was a flrst step to solve the EM problem of the rigor- ous evaluation of the metal foam's shielding efiectiveness (5). Encouraged by the results, we have improved the previously 2D model, developing a preliminary analytical 3D models. Therefore the electromagnetic shielding behavior of a slab of metal foam, has been investigated considering a model with a double wire-screens mesh, separated by an air space. The single screen, whose meshes are assumed to be square, is described by an equivalent sheet impedance operator as mentioned in (3). The agreement of both experimental and theoretical data is a challenging to optimize this model in 3D.
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