Effects of wire properties on the field-tunable behaviour of continuous-microwire composites (original) (raw)

2012, Sensors and Actuators A: Physical

The microwire composites consisting of continuous Co-rich amorphous glass-coated ferromagnetic microwires embedded in a E-glass prepreg matrix were fabricated, and the influences of wire periodicity (b), composition and radius on the field-tunable properties have been systematically investigated in a broad microwave frequency range of 0.9-18 GHz. It has been found that the field tunability, effective operational frequency and field of the composites are strongly dependent on these factors. With decreasing b from 15 to 7 mm, the field tunability of effective permittivity (n ε ) increases from 0.77% to 16% m/A by more than 20 times. The detected cups and resonances of the transmission and reflection spectra are identified. Their changes with wire periodicity have been shown to be due to a combination of the dielectric and magnetic response arising from the interactions between microwave and microwires and microwires by themselves. The best possible field tunability occurs below the plasma frequency. The effective magnetic field for realisation of the field-tunable properties has been found to be about 500 A/m, which is associated with the anisotropy field. In addition, field tunability is found to be positively correlated with the magnetic softness and GMI properties of the wire fillers, which are determined by the wire composition and geometry. These findings are of practical importance in developing multifunctional microwire composites for a broad range of engineering applications, such as structural health monitoring, NDT and microwave tunable devices. interests span a wide range of experimental and theoretical topics in magnetism and magnetic materials such as giant magnetoimpedance (GMI) materials and giant magnetocaloric (GMC) materials.

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Microwave response of amorphous microwires: magnetoimpedance and ferromagnetic resonance

It has been established that giant magnetoimpedance (GMI) in amorphous wires is due to a rapid change in the skin depth, caused by the low-field sensitivity of the azimuthal dynamic permeability (a classical electromagnetic effect). In 5 mm diameter glass-covered amorphous wires, GMI may be observed at the microwave range. A correlation between GMI and ferromagnetic resonance (FMR) was proposed in this microwave range. We have measured the microwave response of amorphous microwires for several alloys from the system (Co 100Àx Fe x Þ 75 Si 15 B 10 (x ¼ 2; 6; 10) with positive, zero, and negative magnetostriction, respectively. Our main results indicate: (i) GMI and FMR effects are well separated at different fields, (ii) GMI follows the magnetization process, confirming its classical electromagnetic origin, and (iii) FMR fields are also affected by the skin effect. r

Magnetoimpedance sensitive to dc bias current in amorphous microwires

Applied Physics Letters, 2010

We have investigated the impedance dependence of magnetically soft microwire on the internal circumferential magnetic field H B created by the dc bias current I B and theoretically and experimentally demonstrated that in a conductor with helical magnetic anisotropy, the high frequency impedance depends on the dc bias current I B ͑or the corresponding bias field H B ͒ and this dependence is hysteretic. We have experimentally observed a change of impedance more than 35% upon changing the bias current. The possible applications of the dc current-driven magnetoimpedance effect are discussed.

Magneto-impedance in glass-coated CoMnSiB amorphous microwires

IEEE Transactions on Magnetics, 1998

A magneto-impedance (MI) effect has been experimentally detected and systematically studied in Co 68:5 Mn 6:5 Si 10 B 15 glass-coated amorphous microwire 14 m in diameter. The dependence of MI on a dc applied magnetic field (up to 20 Oe) for a range of values of ac current (less than 4 mA and having a frequency between 0.2 and 2.0 MHz) flowing along the microwire has been measured in as-prepared samples, as well as after heat treatments up to 400 C. A maximum relative change in MI of around 16% is observed in the optimum conditions, that is, for about 5 Oe dc axial applied field and 3 mA, 2 MHz ac current flowing along the microwire, which finally corresponds to a magnetic field sensitivity of about 0.4 V/Oe. Such modifications are interpreted considering the dependence of the skin-effect on those parameters through the induced changes in the circular permeability. MI in these ferromagnetic wires with micrometric dimension is of technological interest for local detection of magnetic fields.

Giant magnetoimpedance in glass-covered amorphous microwires at microwave frequencies

Journal of Applied Physics, 2002

In this work, results on the giant magnetoimpedance of glass-covered amorphous microwires with nominal composition Co 70.4 Fe 4.6 Si 15 B 10 are presented. The impedance ZϭRϩiX has been investigated as function of frequency ͑1 MHz-1.8 GHz͒ and magnetic field ͑up to Ϯ400 Oe͒, using a HP4396B impedance analyzer and an appropriate coaxial microwave cavity. The effects of the thermal treatments ͑Joule heating, from 1 up to 50 mA for 10 min͒ for anisotropy induction and/or to induce recrystallization have been investigated.

Giant magnetoimpedance effect in a positive magnetostrictive glass-coated amorphous microwire

Physical Review B, 2002

The giant magnetoimpedance ͑GMI͒ effect in positive magnetostrictive glass-coated amorphous Co 83.2 Mn 7.6 Si 5.8 B 3.3 microwire has been studied as a function of a dc magnetic field Ϫ140ϽH dc Ͻ140 Oe and frequency 0.1Ͻ f Ͻ12.85 MHz. A maximum change of 43% in the MI of the as-quenched sample has been observed around 5 MHz frequency. Heat treatment of the sample by passing a dc current of 50 mA through it enhances the MI value to a large extent ͑maximum change ϳ94%͒ by increasing the outer domain volume and inducing a transverse anisotropy. On the other hand, application of an external tensile stress reduces the GMI value by increasing the inner core domain and developing an axial anisotropy. In an as-quenched sample, the maximum value of MI is observed at H dc ϳ0 when measured at frequency f Ͻ8 MHz beyond which a two peak MI profile is seen. The heat-treated sample shows this two peak behavior from a much lower frequency ͑below 1 MHz͒ and additional peaks at H dc ϳ0 for f Ͼ10 MHz. Asymmetry in the MI peaks of a microwire has been produced by passing a dc current through the sample during impedance measurement. The magnetization of the as-quenched and heat-treated samples has also been studied to understand the domain structure and magnetoimpedance results.

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