The Role of Anisotropy in Distinguishing Domination of Néel or Brownian Relaxation Contribution to Magnetic Inductive Heating: Orientations for Biomedical Applications
Magnetic inductive heating (MIH) has been a topic of great interest because of its potential applications, especially in biomedicine. In this paper, the parameters characteristic for magnetic inductive heating power including maximum specific loss power (SLP<sub>max</sub>), optimal nanop...
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doaj-7b1067f0061943459ad96f923a57ed992021-04-09T23:04:51ZengMDPI AGMaterials1996-19442021-04-01141875187510.3390/ma14081875The Role of Anisotropy in Distinguishing Domination of Néel or Brownian Relaxation Contribution to Magnetic Inductive Heating: Orientations for Biomedical ApplicationsLuu Huu Nguyen0Pham Thanh Phong1Pham Hong Nam2Do Hung Manh3Nguyen Thi Kim Thanh4Le Duc Tung5Nguyen Xuan Phuc6Laboratory of Magnetism and Magnetic Materials, Advanced Institute of Materials Science, Ton Duc Thang University, Ho Chi Minh City 700000, VietnamLaboratory of Magnetism and Magnetic Materials, Advanced Institute of Materials Science, Ton Duc Thang University, Ho Chi Minh City 700000, VietnamInstitute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet Street, Cau Giay District, Ha Noi 100000, VietnamInstitute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet Street, Cau Giay District, Ha Noi 100000, VietnamBiophysics Group, Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UKBiophysics Group, Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UKDuy Tan University, K7/25 Quang Trung Street, Da Nang City 550000, VietnamMagnetic inductive heating (MIH) has been a topic of great interest because of its potential applications, especially in biomedicine. In this paper, the parameters characteristic for magnetic inductive heating power including maximum specific loss power (SLP<sub>max</sub>), optimal nanoparticle diameter (D<sub>c</sub>) and its width (ΔD<sub>c</sub>) are considered as being dependent on magnetic nanoparticle anisotropy (K). The calculated results suggest 3 different Néel-domination (N), overlapped Néel/Brownian (NB), and Brownian-domination (B) regions. The transition from NB- to B-region changes abruptly around critical anisotropy K<sub>c</sub>. For magnetic nanoparticles with low K (K < K<sub>c</sub>), the feature of SLP peaks is determined by a high value of D<sub>c</sub> and small ΔD<sub>c</sub> while those of the high K (K > K<sub>c</sub>) are opposite. The decreases of the SLP<sub>max</sub> when increasing polydispersity and viscosity are characterized by different rates of d(SLP<sub>max</sub>)/dσ and d(SLP<sub>max</sub>)/dη depending on each domination region. The critical anisotropy K<sub>c</sub> varies with the frequency of an alternating magnetic field. A possibility to improve heating power via increasing anisotropy is analyzed and deduced for Fe<sub>3</sub>O<sub>4</sub> magnetic nanoparticles. For MIH application, the monodispersity requirement for magnetic nanoparticles in the B-region is less stringent, while materials in the N- and/or NB-regions are much more favorable in high viscous media. Experimental results on viscosity dependence of SLP for CoFe<sub>2</sub>O<sub>4</sub> and MnFe<sub>2</sub>O<sub>4</sub> ferrofluids are in good agreement with the calculations. These results indicated that magnetic nanoparticles in the N- and/or NB-regions are in general better for application in elevated viscosity media.https://www.mdpi.com/1996-1944/14/8/1875magnetic heatingNéel & Brownian relaxationparticle anisotropypolydispersityferrofluid viscosity |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Luu Huu Nguyen Pham Thanh Phong Pham Hong Nam Do Hung Manh Nguyen Thi Kim Thanh Le Duc Tung Nguyen Xuan Phuc |
spellingShingle |
Luu Huu Nguyen Pham Thanh Phong Pham Hong Nam Do Hung Manh Nguyen Thi Kim Thanh Le Duc Tung Nguyen Xuan Phuc The Role of Anisotropy in Distinguishing Domination of Néel or Brownian Relaxation Contribution to Magnetic Inductive Heating: Orientations for Biomedical Applications Materials magnetic heating Néel & Brownian relaxation particle anisotropy polydispersity ferrofluid viscosity |
author_facet |
Luu Huu Nguyen Pham Thanh Phong Pham Hong Nam Do Hung Manh Nguyen Thi Kim Thanh Le Duc Tung Nguyen Xuan Phuc |
author_sort |
Luu Huu Nguyen |
title |
The Role of Anisotropy in Distinguishing Domination of Néel or Brownian Relaxation Contribution to Magnetic Inductive Heating: Orientations for Biomedical Applications |
title_short |
The Role of Anisotropy in Distinguishing Domination of Néel or Brownian Relaxation Contribution to Magnetic Inductive Heating: Orientations for Biomedical Applications |
title_full |
The Role of Anisotropy in Distinguishing Domination of Néel or Brownian Relaxation Contribution to Magnetic Inductive Heating: Orientations for Biomedical Applications |
title_fullStr |
The Role of Anisotropy in Distinguishing Domination of Néel or Brownian Relaxation Contribution to Magnetic Inductive Heating: Orientations for Biomedical Applications |
title_full_unstemmed |
The Role of Anisotropy in Distinguishing Domination of Néel or Brownian Relaxation Contribution to Magnetic Inductive Heating: Orientations for Biomedical Applications |
title_sort |
role of anisotropy in distinguishing domination of néel or brownian relaxation contribution to magnetic inductive heating: orientations for biomedical applications |
publisher |
MDPI AG |
series |
Materials |
issn |
1996-1944 |
publishDate |
2021-04-01 |
description |
Magnetic inductive heating (MIH) has been a topic of great interest because of its potential applications, especially in biomedicine. In this paper, the parameters characteristic for magnetic inductive heating power including maximum specific loss power (SLP<sub>max</sub>), optimal nanoparticle diameter (D<sub>c</sub>) and its width (ΔD<sub>c</sub>) are considered as being dependent on magnetic nanoparticle anisotropy (K). The calculated results suggest 3 different Néel-domination (N), overlapped Néel/Brownian (NB), and Brownian-domination (B) regions. The transition from NB- to B-region changes abruptly around critical anisotropy K<sub>c</sub>. For magnetic nanoparticles with low K (K < K<sub>c</sub>), the feature of SLP peaks is determined by a high value of D<sub>c</sub> and small ΔD<sub>c</sub> while those of the high K (K > K<sub>c</sub>) are opposite. The decreases of the SLP<sub>max</sub> when increasing polydispersity and viscosity are characterized by different rates of d(SLP<sub>max</sub>)/dσ and d(SLP<sub>max</sub>)/dη depending on each domination region. The critical anisotropy K<sub>c</sub> varies with the frequency of an alternating magnetic field. A possibility to improve heating power via increasing anisotropy is analyzed and deduced for Fe<sub>3</sub>O<sub>4</sub> magnetic nanoparticles. For MIH application, the monodispersity requirement for magnetic nanoparticles in the B-region is less stringent, while materials in the N- and/or NB-regions are much more favorable in high viscous media. Experimental results on viscosity dependence of SLP for CoFe<sub>2</sub>O<sub>4</sub> and MnFe<sub>2</sub>O<sub>4</sub> ferrofluids are in good agreement with the calculations. These results indicated that magnetic nanoparticles in the N- and/or NB-regions are in general better for application in elevated viscosity media. |
topic |
magnetic heating Néel & Brownian relaxation particle anisotropy polydispersity ferrofluid viscosity |
url |
https://www.mdpi.com/1996-1944/14/8/1875 |
work_keys_str_mv |
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