R&D Report: EMF Interaction Calculations for Aires K8 Resonator at 2.4 GHz WiFi (Aires Shield Extreme 2016)

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R&D Report: EMF Interaction Calculations for Aires K8 Resonator at 2.4 GHz WiFi (Aires Shield Extreme 2016)

R&D: Aires K8 Resonator EMF Interaction at 2.4 GHz WiFi

Aires Shield Extreme (2016 Model) • Project Manager: I. Serov • Consultants: Prof. A. Kopyltsov, Prof. A. Jukna

R&D ReportK8 ResonatorAires Shield Extreme2.4 GHz WiFiMEMS Technology2016

Overview

This R&D report documents the electromagnetic field strength and intensity calculations for the interaction of 2.4 GHz WiFi radiation with the Aires K8 resonator (microprocessor) used in the Aires Shield Extreme 2016 model. The study was managed by I. Serov, with researchers K. Korshunov, I. Soltovskaya, and T. Shamko, and scientific consultants Prof. A. Kopyltsov (St. Petersburg) and Prof. A. Jukna (VGTU Vilnius).

7.5 mm
resonator substrate size
0.4 μm
slit width (fractal etching)
0.8 μm
slit depth

Physical Model: Self-Affine Fractal Silicon Substrate

The K8 resonator is a type-n monocrystalline silicon substrate (7.5 mm × 7.5 mm, 0.5 mm thick) with crystallographic plane 100 (Miller index). Its surface carries a fractal system of annular slits with rectangular cross-section (0.4 μm wide, 0.8 μm deep), forming a regular self-affine structure obeying self-similarity and scale invariance laws.

Interaction Mechanism

When electromagnetic radiation strikes the resonator surface, a surface wave appears and is reflected — with absorption occurring in the slits — leading to redistribution of electromagnetic field characteristics. The slit structure acts as a regular topology that transforms incident radiation through counter-wave interaction and derivative resonances that existing classical software packages cannot model.

Mathematical Model

The calculation tracks radiation along DCA trajectories (D = source sphere, C = resonator surface node, A = receiver point), computing electric field strength at each receiver point. The model accounts for both surface reflection (angle of incidence = angle of reflection) and slit absorption, summing contributions across all resonator nodes to yield the full superimposed field distribution.

Why Custom Software Was Required

Standard commercial electromagnetic simulation packages consider interactions only in the context of classical physics. The K8 resonator's operation requires accounting for counter-wave interaction on the resonator surface and numerous derivative resonances — effects not available in off-the-shelf tools. Custom algorithms were developed specifically for this modeling.

Research Team

Project Manager: I. Serov | Responsible Researcher: K. Korshunov | Researchers: I. Soltovskaya, T. Shamko | Scientific Consultants: Prof. Dr. A. Kopyltsov (Doctor of Technical Sciences, St. Petersburg Electrotechnical University LETI) and Prof. A. Jukna (Department of Physics, Vilnius Gediminas Technical University)