摘要
本文研究了Fe83Ga17合金在静态磁场H中的阻尼性能。结果表明, 在磁场作用下, 阻尼峰值可以在0.020 ~ 0.085之间调节, 并在临界磁场 (Hcr = 0.2 mT) 处达到最大值。当H小于Hcr时, 磁畴发生畴壁可逆位移。磁场对磁畴运动起启动作用, 增强畴壁移动能力, 磁机械阻尼随着磁场的增加而增加。当H大于Hcr时, 磁畴开始发生不可逆壁移和畴转, 并逐渐占主导地位。磁场对磁畴运动起钉扎作用, 阻碍畴壁运动, 磁机械阻尼随着磁场的增加而减小, 直到无磁机械阻尼发生。磁化饱和后, Fe83Ga17合金的阻尼主要由位错提供, 验证了磁机械滞后和位错能量耗散的协同阻尼效应。
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This study was financially supported by the National Key Research and Development Program of China (No. 2021YFB3501403).
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Yan, SW., Mu, X., Liu, BJ. et al. Damping capacity of Fe83Ga17 magnetostrictive alloy under magnetic field. Rare Met. 43, 402–409 (2024). https://doi.org/10.1007/s12598-023-02382-1
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DOI: https://doi.org/10.1007/s12598-023-02382-1