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. 2017 Aug 28;12:6273–6287. doi: 10.2147/IJN.S141072

Figure 2.

Figure 2

Comparison with the Rosensweig model.

Notes: The imaginary part of the magnetic susceptibility, χ″, and the SLP were computed by our revised cluster-based model (red solid line) and the Rosensweig model (blue dashed line). (A) χ″ as a function of the alternating magnetic field frequency, f, for magnetic nanoparticle diameter =18 nm, alternating magnetic field amplitude H0=11 kA/m, and magnetic anisotropy constant Ka =15 kJ/m3. (B) χ″ as a function of the magnetic nanoparticle diameter for alternating magnetic field frequency f=410 kHz, alternating magnetic field amplitude H0=11 kA/m, and magnetic anisotropy constant Ka =15 kJ/m3. (C) The SLP, as a function of the magnetic nanoparticle diameter, using the same parameters as those in (B).

Abbreviation: SLP, specific loss power.