Abstract
This study investigates the spatiotemporal evolution and dynamic microwave absorption properties of ferrofluid interfaces under lateral confinement and vertical magnetic excitation. We examine the morphological transition of a magnetite-based ferrofluid in a confined cylindrical domain (D = 2 cm) subjected to oscillating magnetic fields (Bmax = 40.5 mT, f = 0–105 Hz). Electromagnetic characterization in the Ku-band (12–18 GHz) was conducted using a metal-backed configuration to explicitly isolate Reflection Loss (RL). Results reveal that microwave absorption is governed by a synergy between bulk dissipation and surface geometry. While static layers exhibit thickness-dependent absorption, dynamic excitation enables an active “geometric enhancement” mechanism. We demonstrate an optimal operational window at low frequencies (f = 15–35 Hz) for thick layers (d≥7 mm), where the stable ferromagnetic soliton functions as a gradient-index impedance matcher. Although the absolute peak RL of −9.46 dB at 17.8 GHz is numerically modest compared to traditional solid-state absorbers, its significance lies in its in-situ, reversible spatial tunability. This dynamic topology minimizes surface reflection and maximizes energy coupling, establishing a design strategy for adaptive electromagnetic absorbers capable of switching their reflection characteristics through precise fluid control.
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