When an applied magnetic field has an arbitrary direction with respect to the lattice axes of a periodically microstructured or nanostructured metamaterial, the effective permittivity tensor of the metamaterial sample becomes anisotropic and all its components can be nonzero. This is true even if the microstructure has a high symmetry, e.g., cubic or triangular. It is found that the strong magneto-induced anisotropy which appears in the macroscopic response leads to unusual anisotropic behavior of the Voigt effect and other magneto-optical (MO) effects. I.e., these phenomena become strongly dependent on the direction of the applied static magnetic field, as well as on the direction of the time dependent electromagnetic field, with respect to the symmetry axes of the periodic microstructure.It is known that the Voigt, Faraday and other magneto-optical (MO) effects can be significantly enhanced in the vicinity of an electromagnetic (EM) resonance. One such resonance, which is currently under intensive study, is the surface plasma resonance. It is widely believed that this or similar resonances are responsible for the Extraordinary Light Transmission (ELT) through a metal film, perforated by a periodic array of subwavelength holes. 1 Application of a static magnetic field B 0 to such systems (see Fig. 1) induces strong optical and transport anisotropy and leads to the appearance of additional off-diagonal tensor components in the macroscopic permittivity tensorε e (see Fig. 2) and changes the frequency of the surface plasma resonance 2-4 Therefore, the application of a static magnetic field to a conducting system with dielectric islands or to a dielectric system with metallic islands should lead to the appearance of strong magneto-optical effects and to possibilities for the manipulation of light propagation. 2, 3, 5, 6After the phenomenon of ELT in the presence of applied static magnetic field was discussed in Refs. 3, 5, several attempts were made to consider different MO effects in the case of light propagating through a perforated metallic film. 7-16 However in all of them only the Faraday configuration was considered, where the magnetic field B 0 is normal to the film plane. In none of them, as far as we know, was the Voigt configuration, (i.e., where the magnetic field is applied parallel to the film plane) considered. From intuitive physical considerations we expect that when an in-plane magnetic field is rotated with respect to the main axes of the microstructure, a magneto-induced angular anisotropy of the different MO effects will be observed. In this manuscript we consider the general case of arbitrary orientation of the magnetic filed with respect to the film microstructure.In the case where B 0 has an arbitrary direction with respect to the lattice axes of the microstructure all components of the permittivity tensor can be nonzero. 2, 3, 5 When both the external magnetic field B 0 and the EM electric field E are rotated in the film plane, the angular profiles of all the permittivity tensor components ar...