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. 2017 Aug 11;29(37):373003. doi: 10.1088/1361-648X/aa7933

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© 2017 IOP Publishing Ltd

Original content from this work may be used under the terms of the Creative Commons Attribution 3.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.

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Figure 21. — Energy of a magnetic ellipsoidal particle at an interface as function of its orientation. (a) The results for particle aspect ratios $b / a = α = 1.2$ , $b / a = α = 1.6666$ , and $b / a = α = 5$ correspond to a representative field strength $\bar{B} = 0.1$ . (b) Energies for an ellipsoidal nanoparticle with aspect ratio $α = 1.6666$ for different external field strengths $\bar{B} = 0.1$ , $\bar{B} = 0.134$ , and $\bar{B} = 0.145$ . Reprinted from [41]. © IOP Publishing Ltd. All rights reserved.

Figure 21. — Energy of a magnetic ellipsoidal particle at an interface as function of its orientation. (a) The results for particle aspect ratios $b / a = α = 1.2$ , $b / a = α = 1.6666$ , and $b / a = α = 5$ correspond to a representative field strength $\bar{B} = 0.1$ . (b) Energies for an ellipsoidal nanoparticle with aspect ratio $α = 1.6666$ for different external field strengths $\bar{B} = 0.1$ , $\bar{B} = 0.134$ , and $\bar{B} = 0.145$ . Reprinted from [41]. © IOP Publishing Ltd. All rights reserved.