期刊文献+

Equivalent circuit model including magnetic and thermo sources for the thermo–magneto–electric coupling effect in magnetoelectric laminates

Equivalent circuit model including magnetic and thermo sources for the thermo–magneto–electric coupling effect in magnetoelectric laminates
下载PDF
导出
摘要 The nonlinear thermo–magneto–mechanical magnetostrictive constitutive and the linear thermo–mechanical-electric piezoelectric constitutive are adopted in this paper. The bias magnetic field and ambient temperature are equivalent to a magnetic source and a thermo source, respectively. An equivalent circuit, which contains a magnetic source and a thermo source at the input, for the thermo–magneto–electric coupling effect in magnetoelectric(ME) laminates, is established. The theoretical models of the output voltage and static ME coefficient for ME laminates can be derived from this equivalent circuit model. The predicted static ME coefficient versus temperature curves are in excellent agreement with the experimental data available both qualitatively and quantitatively. It confirms the validity of the proposed model. Then the models are adopted to predict variations in the output voltages and ME coefficients in the laminates under different ambient temperatures, bias magnetic fields, and the volume ratios of magnetostrictive phases. This shows that the output voltage increases with both increasing temperature and increasing volume ratio of magnetostrictive phases; the ME coefficient decreases with increasing temperature; the ME coefficient shows an initial sharp increase and then decreases slowly with the increase in the bias magnetic field, and there is an optimum volume ratio of magnetostrictive phases that maximize the ME coefficient.This paper can not only provide a new idea for the study of the thermo–magneto–electric coupling characteristics of ME laminates, but also provide a theoretical basis for the design and application of ME laminates, operating under different sensors. The nonlinear thermo–magneto–mechanical magnetostrictive constitutive and the linear thermo–mechanical-electric piezoelectric constitutive are adopted in this paper. The bias magnetic field and ambient temperature are equivalent to a magnetic source and a thermo source, respectively. An equivalent circuit, which contains a magnetic source and a thermo source at the input, for the thermo–magneto–electric coupling effect in magnetoelectric(ME) laminates, is established. The theoretical models of the output voltage and static ME coefficient for ME laminates can be derived from this equivalent circuit model. The predicted static ME coefficient versus temperature curves are in excellent agreement with the experimental data available both qualitatively and quantitatively. It confirms the validity of the proposed model. Then the models are adopted to predict variations in the output voltages and ME coefficients in the laminates under different ambient temperatures, bias magnetic fields, and the volume ratios of magnetostrictive phases. This shows that the output voltage increases with both increasing temperature and increasing volume ratio of magnetostrictive phases; the ME coefficient decreases with increasing temperature; the ME coefficient shows an initial sharp increase and then decreases slowly with the increase in the bias magnetic field, and there is an optimum volume ratio of magnetostrictive phases that maximize the ME coefficient.This paper can not only provide a new idea for the study of the thermo–magneto–electric coupling characteristics of ME laminates, but also provide a theoretical basis for the design and application of ME laminates, operating under different sensors.
出处 《Chinese Physics B》 SCIE EI CAS CSCD 2015年第7期496-502,共7页 中国物理B(英文版)
基金 Project supported by the National Natural Science Foundation of China(Grant Nos.11172285 and 11472259) the Natural Science Foundation of Zhejiang Province,China(Grant No.LR13A020002)
关键词 magnetoelectric laminates thermo–magneto–electric coupling effect thermo source magneto source magnetoelectric laminates,thermo–magneto–electric coupling effect,thermo source,magneto source
  • 相关文献

参考文献39

  • 1Nan C W, Bichurin M I, Dong S X, Viehland D and Srinivasan G 2008 J. Appl. Phys. 103 031101.
  • 2Rao W, Wang Y B, Wang Y A, Gao J X, Zhou W L and Yu J 2014 Chin. Phys. Lett. 31 017503.
  • 3Wan H, Shen R F and Wu X Z 2005 Acta Phys. Sin. 54 1426 (in Chinese).
  • 4Dong S X, Li J F and Viehland D 2004 Appl. Phys. Lett. 85 2307.
  • 5Dong S X, Li J F and Viehland D 2004 Appl. Phys. Lett. 84 4188.
  • 6Pan D A, Zhang S G, Tian J J, Sun J S, Volinsky A A and Qiao L J 2010 Chin. Phys. B 19 027201.
  • 7Dai X Z, Wen Y M, Li P, Yang J and Zhang G Y 2009 Sens. Actuat. A 156 350.
  • 8Dai X Z, Wen Y M, Li P, Yang J and Jiang X F 2010 Acta Phys. Sin. 59 2137 (in Chinese).
  • 9Chen L, Li P, Wen Y M and Qiu J 2012 J. Appl. Phys. 111 07E503.
  • 10Zhu Y and Zu J W 2012 IEEE Tran. Magn. 48 3344.

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部