**Open Journal of Applied Sciences**

Vol.06 No.12(2016), Article ID:71960,11 pages

10.4236/ojapps.2016.612071

Methods for Estimating Specific Loss Power in Magnetic Hyperthermia Revisited

Kenya Murase^{ }

Department of Medical Physics and Engineering, Division of Medical Technology and Science, Faculty of Health Science, Graduate School of Medicine, Osaka University, Osaka, Japan

Copyright © 2016 by author and Scientific Research Publishing Inc.

This work is licensed under the Creative Commons Attribution International License (CC BY 4.0).

http://creativecommons.org/licenses/by/4.0/

Received: October 10, 2016; Accepted: November 8, 2016; Published: November 11, 2016

ABSTRACT

Our purpose in this study was to present three methods for estimating specific loss power (SLP) in magnetic hyperthermia with use of an alternating magnetic field (AMF) and magnetic nanoparticles (MNPs) and to compare the SLP values estimated by the three methods using simulation studies under various diameters of MNPs (D), amplitudes (H_{0}) and frequencies of AMF (f). In the first method, the SLP was calculated by solving the magnetization relaxation equation of Shliomis numerically (SLP_{1}). In the second method, the SLP was obtained by solving Shliomis’ relaxation equation using the complex susceptibility (SLP_{2}). The third method was based on Rosensweig’s model (SLP_{3}). The SLP_{3} value changed largely depending on the magnetic field strength (H) in the Langevin parameter (ξ) and it became maximum () and minimum () when H was 0 and ±H_{0}, respectively. The relative difference between SLP_{1} and SLP_{2} was the largest and increased with increasing D and H_{0}, whereas that between SLP_{1} and was the smallest and was almost constant regardless of D and H_{0}, suggesting that H in ξ should be taken as H_{0} in estimating the SLP using Rosensweig’s model. In conclusion, this study will be useful for optimizing the parameters of AMF in magnetic hyperthermia and for the optimal design of MNPs for magnetic hyperthermia.

**Keywords:**

Magnetic Hyperthermia, Magnetic Nanoparticle, Specific Loss Power, Alternating Magnetic Field, Magnetization Relaxation

1. Introduction

Hyperthermia is one of the promising approaches to cancer therapy. The most commonly used heating method in the clinical setting is capacitive heating that uses a radiofrequency (RF) electric field [1] . However, a major technical problem with hyperthermia is the difficulty of heating the targeted tumor to the desired temperature without damaging the surrounding tissues, as the electromagnetic energy must be directed from an external source and penetrate normal tissue. Other hyperthermia modalities, including ultrasound hyperthermia, have been reported [2] , but the efficacy of these modalities depends on the size and depth of the tumor, and disadvantages include the ability to target the tumor and control the exposure.

Hyperthermia with use of magnetic nanoparticles (MNPs) (magnetic hyperthermia) was developed in the 1950s [3] and is still under development in the effort to overcome the above disadvantages [4] [5] . MNPs generate heat in an alternating magnetic field (AMF) as a result of hysteresis and relaxational losses, which results in heating of the tissue in which MNPs accumulate [6] . For small MNPs, the relaxational losses caused by a delay in magnetization relaxation are dominant for heat dissipation [6] . With the development of precise methods for synthesizing functionalized MNPs [7] , MNPs with functionalized surfaces, which have high specificity for tumor tissue, have been developed as heating elements for magnetic hyperthermia [8] . Recently, MNPs with a higher heating efficiency, i.e., specific loss power (SLP), have also been actively developed [9] . Furthermore, there is renewed interest in magnetic hyperthermia as a treatment modality for cancer, especially when it is combined with other, more traditional therapeutic approaches such as the co-delivery of anticancer drugs [10] or radiation therapy [11] . From these aspects, magnetic hyperthermia has received much recent attention.

The estimation of SLP is important for evaluating the heating efficiency of MNPs, for optimizing the parameters of AMF, and for the optimal design of MNPs in an attempt to establish the effectiveness of magnetic hyperthermia. Rosensweig’s model [6] has often been used for the estimation of SLP. His model, however, is based on the so-called linear magnetization assumption [12] , and thus it is said that his model is strictly valid only in the limit of small amplitude and frequency of AMF. In this study, we presented three methods for estimating SLP and compared the SLP values estimated by the three methods under various conditions of MNPs and AMF. Especially, we investigated the validity of Rosensweig’s model in comparison with the numerical solution of the magnetization relaxation equation of Shliomis [13] .

2. Materials and Methods

2.1. Theory

The magnetization relaxation equation of Shliomis [12] [13] is given by

, (1)

where M is the magnetization of MNPs under the magnetic field H, Ω is the flow velocity, f is the volume fraction, and η is the viscosity of the suspending fluid. When there is no bulk flow and M and H are collinear, Equation (1) is reduced to the following equation [6] :

. (2)

In Equation (2), τ is the effective relaxation time given by

, (3)

where τ_{N} and τ_{B} are the Néel relaxation and Brownian relaxation time, respectively [6] . τ_{N} and τ_{B} are given by the following relationships [6] :

and, (4)

where τ_{0} is the average relaxation time in response to a thermal fluctuation, k_{B} is the Boltzmann constant, T is the temperature, and, with K being the anisotropy constant of MNP. V_{H} is taken as the hydrodynamic volume of MNP that is larger than the magnetic volume for MNP of diameter D. As a model for V_{H}, it is assumed that, where δ is the thickness of a sorbed surfactant layer [6] . in Equation (2) denotes the equilibrium magnetization and is given by

, (5)

where χ_{0} is the equilibrium susceptibility. In this study, was assumed to be

, (6)

where H_{0} and f denote the amplitude and frequency of AMF, respectively. Because the actual equilibrium susceptibility (χ_{0}) is dependent on the magnetic field, χ_{0} was assumed to be the chord susceptibility corresponding to the Langevin equation, given by [6]

, (7)

where χ_{i} is the initial susceptibility given by, ξ is the Langevin parameter given by, M_{d} is the domain magnetization of a suspended particle, and μ_{0} is the permeability of free space. It should be noted that ξ is magnetic field (H) dependent and thus time dependent.

Solving Equation (2) and using Equation (5) and Equation (6) yield

, (8)

where denotes the convolution integral and is at t = 0. In this study, was assumed to be. When, however, the second term of the right-hand side of Equation (8) can be neglected. It should be noted that if we calculate as a function of, we can obtain the hysteresis loop, i.e., M-H curve.

According to Rosensweig [6] , solving Equation (2) using the complex susceptibility given by and Equation (5) and Equation (6) with an assumption that χ_{0} is constant, yields

, (9)

where χ' (in-phase component) and χ'' (out-of-phase component) are, respectively, given by [6]

and. (10)

The average rate of energy dissipation per cycle of the period, i.e., is given by [6]

. (11)

Substituting Equation (6) into Equation (11) yields

. (12)

The rate of energy dissipation per unit mass of MNPs, i.e., specific loss power (SLP) can be obtained from as [12]

, (13)

where ρ is the density of suspending fluid.

In this study, we considered the following three methods for estimating SLP. In the first method, Equation (8) was used for in Equation (12). In this case, because must be time-periodic in the steady state, the SLP value for the i-th cycle of the M-H curve (denoted by) can be given by

(14)

It should be noted that when i is sufficiently large, the second term of the right-hand side of Equation (14) can be neglected and approaches the steady state. We denote the value in the quasi steady state by SLP_{1}. Actually, SLP_{1} was taken as the value in the case when, with ε being taken as 10^{−6}, where denotes the absolute value. The integration in Equation (14) was performed by use of the trapezoidal rule [14] (“trapz” in MATLAB®; The MathWorks, Inc., Natick, MA, USA) and the convolution integral was calculated using the MATLAB® function (“conv”).

In the second method, Equation (9) was used for in Equation (12). In this case, the SLP value (denoted by SLP_{2}) can be given by

. (15)

As in Equation (14), the integration in Equation (15) was also performed by use of the trapezoidal rule [14] (“trapz” in MATLAB®; The MathWorks, Inc., Natick, MA, USA).

In the third method, χ' and χ'' (basically χ_{0}) were assumed to be constant in Equation (15), though they are actually magnetic field (H) dependent. In this case, the SLP value (denoted by SLP_{3}) can be obtained from Equation (10) and Equation (15) as

. (16)

It should be noted that is equal to the equation for the energy dissipation derived by Rosensweig [6] . As shown afterwards, SLP_{3} changes depending on the magnetic field strength. Thus, we denote the maximum, minimum, and mean SLP_{3} values in a cycle of the period, i.e., by, , and, respectively. was calculated from

. (17)

For comparison of SLP_{1}, SLP_{2}, , , and, we calculated the relative differences (RD_{2}, , , and) defined by

, (18)

, (19)

, (20)

and

. (21)

2.2. Simulation Studies

In this study, we assumed that MNPs consisted of maghemite (γ-Fe_{2}O_{3}) and fixed τ_{0}, δ, M_{d}, K, η, ρ, f, and T to be 10^{−9} s, 2 nm, 414 kA/m, 4.7 kJ/m^{3}, 0.00235 kg/m/s, 4600 kg/m^{3}, 0.003, and 37˚C, respectively [15] . When H_{0}, f, and D were fixed, they were taken as 20 mT, 300 kHz, and 20 nm, respectively. It should be noted that the unit of mT can be converted to kA/m by use of the relationship 1 mT = 0.796 kA/m.

3. Results

As shown in Equation (14), the value depends on the cycle number of the M-H curve. Thus, we calculated the value in the quasi steady state, i.e., the SLP_{1} value under the condition of with ε being taken as 10^{−6}, as previously described. When we neglected the second term in the right-hand side of Equation (14), the value reached the steady state after a few cycles in all the cases studied. Figure 1(a) shows the M-H curves in the quasi steady state calculated from Equation (8) for various frequencies of AMF. For comparison, Figure 1(b) shows the M-H curves calculated from Equation (9). It should be noted that was normalized by the saturation magnetization (M_{s}) given by. In these simulations, H_{0} was fixed at 20 mT and D was assumed to be 20 nm. Figure 2 shows the case when D was varied from 10 nm to 30 nm with steps of 5 nm. As shown in Figure 1 and Figure 2, a large difference between the M-H curves obtained by Equation (8) and Equation (9) was observed and it increased with increasing f and D.

Figure 3(a) shows the SLP_{3} values calculated from Equation (16) as a function of H with f being varied from 200 kHz to 1000 kHz with steps of 200 kHz, whereas Figure 3(b) shows the case when D was varied from 10 nm to 30 nm with steps of 5 nm. In

(a) (b)

Figure 1. (a) M-H curves (hysteresis loops) in the quasi steady state calculated from Equation (8) for various frequencies of an alternating magnetic field (AMF) (f); (b) M-H curves calculated from Equation (9) for various f. In these simulations, the amplitude of AMF (H_{0}) and diameter of magnetic nanoparticles (D) were assumed to be 20 mT and 20 nm, respectively. Note that the unit of mT can be converted to kA/m by use of the relationship 1 mT = 0.796 kA/m.

(a) (b)

Figure 2. (a) M-H curves in the quasi steady state calculated from Equation (8) for various D; (b) M-H curves calculated from Equation (9) for various D. In these simulations, H_{0} and f were assumed to be 20 mT and 300 kHz, respectively.

these simulations, H_{0} was fixed at 20 mT. As shown in Figure 3, the SLP_{3} value became maximum, i.e., when H was zero. When |H| was the maximum, i.e., H_{0}, the SLP_{3} value became minimum, i.e.,.

Figure 4(a) shows the comparison of SLP_{1}, SLP_{2}, , , and as a function of D, whereas Figure 4(b) shows the RD_{2}, , , and values as a function of D. As shown in Figure 4(b), was the largest and

(a) (b)

Figure 3. (a) Specific loss power (SLP) values calculated from Equation (16) (SLP_{3}) as a function of the magnetic field (H) for various f. In these simulations, H_{0} and D were assumed to be 20 mT and 20 nm, respectively; (b) SLP_{3} values calculated from Equation (16) as a function of H for various D. In these simulations, H_{0} and f were assumed to be 20 mT and 300 kHz, respectively. Note that the SLP_{3} values for D of 10 nm and 15 nm are too small to be seen in the figure.

(a) (b)

Figure 4. (a) SLP_{1}, SLP_{2}, , , and values as a function of D. Note that SLP_{1} and SLP_{2} were calculated from Equation (14) and Equation (15), respectively. and denote the maximum and minimum values of SLP_{3} calculated from Equation (16), respectively. was calculated from Equation (17); (b) RD_{2}, , , and values as a function of D. Note that RD_{2}, , , and represent the relative differences calculated from Equation (18), Equation (19), Equation (20), and Equation (21), respectively. In these simulations, H_{0} and f were assumed to 20 mT and 300 kHz, respectively.

increased with increasing D, whereas was the smallest and was almost constant regardless of D.

Figure 5(a) shows the comparison of SLP_{1}, SLP_{2}, , , and as a function of H_{0}, whereas Figure 5(b) shows the RD_{2}, , , and values as a function of H_{0}. As shown in Figure 5(b), was the largest and increased with increasing H_{0}, whereas was the smallest and was almost constant regardless of H_{0}.

Figure 6(a) shows the comparison of SLP_{1}, SLP_{2}, , , and as a function of f, whereas Figure 6(b) shows the RD_{2}, , , and values as a function of f. In this case, the RD_{2}, , , and values were almost constant regardless of f (Figure 6(b)).

(a) (b)

Figure 5. (a) SLP_{1}, SLP_{2}, , , and values as a function of H_{0}; (b) RD_{2}, , , and values as a function of H_{0}. In these simulations, D and f were assumed to be 20 nm and 300 kHz, respectively.

(a) (b)

Figure 6. (a) SLP_{1}, SLP_{2}, , , and values as a function of f; (b) RD_{2}, , , and values as a function of f. In these simulations, H_{0} and D were assumed to be 20 mT and 20 nm, respectively.

4. Discussion

In this study, we presented three methods for the estimation of SLP in magnetic hyperthermia and compared the SLP values estimated by the three methods (SLP_{1}, SLP_{2}, and SLP_{3}). SLP_{1} was derived by solving the magnetization relaxation equation of Shliomis [13] numerically. SLP_{2} was derived by solving Shliomis’ relaxation equation [13] using the complex susceptibility. SLP_{3} was derived based on Rosensweig’s model, in which the complex susceptibility with χ' and χ'' (basically χ_{0}) being assumed to be constant has been used.

As previously described, Rosensweig’s model [6] has often been used for the estimation of SLP. To the best of our knowledge, however, few studies have been performed to validate the SLP estimation based on Rosensweig’s method [6] in comparison with that based on the numerical solution of the magnetization relaxation equation of Shliomis [13] .

As shown in Figure 1 and Figure 2, a large difference was observed between the M-H curves calculated from Equation (8) and Equation (9), especially when H is zero, and the difference increased with increasing f and D. When using Equation (9), becomes equal to at, i.e., and it becomes equal to at, i.e.,. On the other hand, becomes equal to at, i.e., and it becomes equal to at, i.e.,. Thus, the above difference in the M-H curves shown in Figure 1 and Figure 2 may suggest that given by Equation (10) is overestimated compared to the case when using Equation (8). Furthermore, the area of the M-H curve calculated from Equation (9) (Figure 1(b) and Figure 2(b)) was larger than that calculated from Equation (8) (Figure 1(a) and Figure 2(a)). The area of the M-H curve directly represents the power loss during one cycle of the hysteresis loop. Thus, the above finding corresponds to the fact that SLP_{2} is larger than SLP_{1} (Figure 4(a), Figure 5(a), and Figure 6(a)).

The SLP_{3} given by Equation (16) has often been used for characterizing the heating property of MNPs [16] . As previously described, SLP_{3} has been derived with an assumption that χ_{0} is constant. However, χ_{0} is actually magnetic field (H) dependent, because χ_{0} is the function of the Langevin parameter (ξ) as shown in Equation (7) and ξ is the function of H. To investigate to what extent SLP_{3} depends on H, we showed the SLP_{3} values as a function of H in Figure 3. As shown in Figure 3, the SLP_{3} value changed largely depending on H. χ_{0} in Equation (16) is the monotonically decreasing function of |ξ| or |H| (data not shown). Thus, the SLP_{3} value becomes maximum when H is zero (Figure 3). In this case, χ_{0} becomes equal to χ_{i}, because in Equation (7) approaches ξ/3 when ξ approaches zero. On the other hand, when |H| is maximum, i.e., H is equal to ±H_{0}, the SLP_{3} value becomes minimum.

To compare the SLP values estimated by Equation (15) and Equation (16) with that estimated using the numerical solution of the magnetization relaxation equation of Shliomis [13] , we calculated the relative differences given by Equation (18) to Equation (21). As shown in Figure 4 and Figure 5, the value was the largest and increased with increasing D and H_{0}, whereas the value was the smallest and was almost constant regardless of D and H_{0}. These results suggest that when estimating SLP using Rosensweig’s model [6] , H in ξ should be taken as H_{0}.

In this study, we solved the magnetization relaxation equation of Shliomis [13] (Equation (1)) with an assumption that there is no bulk flow and the magnetization of MNPs and magnetic field are collinear. In this case, Equation (1) is reduced to Equation (2), which can be easily solved using convolution integral as shown in Equation (8). Although Equation (2) appears to be valid in considering the magnetic hyperthermia with use of small MNPs in the superparamagnetic state and we believe that this study will provide the basis for establishing the effectiveness of such magnetic hyperthermia, it will be necessary to solve Equation (1) without any assumptions or another magnetization equation derived microscopically from the Fokker-Planck equation [12] [17] for more detailed analysis. These studies are currently in progress. As previously described, we targeted the MNPs consisting of maghemite with the magnetic and physical properties described in the “Simulation Studies” section, because maghemite is the core iron oxide of Resovist®, which is a commercially-available organ-specific contrast agent for magnetic resonance imaging and has been approved for clinical use in Japan [15] . We will also perform further studies for other MNPs.

5. Conclusion

We presented three methods for estimating SLP in magnetic hyperthermia and compared the SLP values estimated by the three methods under various conditions of MNPs and AMF. This study will be useful for optimizing the parameters of AMF in magnetic hyperthermia and for developing the MNPs suitable for magnetic hyperthermia. We also investigated the validity of Rosensweig’s model in comparison with the numerical solution of the magnetization relaxation equation of Shliomis, suggesting that when estimating SLP using Rosensweig’s model, the magnetic field strength in the Langevin parameter should be taken as the amplitude of AMF.

Acknowledgements

This work was supported by a Grant-in-Aid for Scientific Research (Grant Number: 25282131 and 15K12508) from the Japan Society for the Promotion of Science (JSPS).

Cite this paper

Murase, K. (2016) Methods for Estimating Specific Loss Power in Magnetic Hyperthermia Revisited. Open Journal of Applied Sciences, 6, 815-825. http://dx.doi.org/10.4236/ojapps.2016.612071

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