Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles
Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Murase, Kenya [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2011 |
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| Schlagwörter: |
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| Anmerkung: |
© Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011 |
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| Übergeordnetes Werk: |
Enthalten in: Radiological physics and technology - Tokyo : Springer, 2008, 4(2011), 2 vom: 11. Juni, Seite 194-202 |
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| Übergeordnetes Werk: |
volume:4 ; year:2011 ; number:2 ; day:11 ; month:06 ; pages:194-202 |
| Links: |
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| DOI / URN: |
10.1007/s12194-011-0123-4 |
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SPR025176625 |
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| 245 | 1 | 0 | |a Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles |
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| 520 | |a Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it. | ||
| 650 | 4 | |a Magnetic hyperthermia |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Magnetic nanoparticle |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Superparamagnetic iron oxide (SPIO) |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Alternating magnetic field |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Oonoki, Junko |4 aut | |
| 700 | 1 | |a Takata, Hiroshige |4 aut | |
| 700 | 1 | |a Song, Ruixiao |4 aut | |
| 700 | 1 | |a Angraini, Anggia |4 aut | |
| 700 | 1 | |a Ausanai, Prapan |4 aut | |
| 700 | 1 | |a Matsushita, Taro |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Radiological physics and technology |d Tokyo : Springer, 2008 |g 4(2011), 2 vom: 11. Juni, Seite 194-202 |w (DE-627)571166032 |w (DE-600)2433581-2 |x 1865-0341 |7 nnns |
| 773 | 1 | 8 | |g volume:4 |g year:2011 |g number:2 |g day:11 |g month:06 |g pages:194-202 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/s12194-011-0123-4 |z lizenzpflichtig |3 Volltext |
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10.1007/s12194-011-0123-4 doi (DE-627)SPR025176625 (SPR)s12194-011-0123-4-e DE-627 ger DE-627 rakwb eng Murase, Kenya verfasserin aut Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011 Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it. Magnetic hyperthermia (dpeaa)DE-He213 Magnetic nanoparticle (dpeaa)DE-He213 Superparamagnetic iron oxide (SPIO) (dpeaa)DE-He213 Alternating magnetic field (dpeaa)DE-He213 Oonoki, Junko aut Takata, Hiroshige aut Song, Ruixiao aut Angraini, Anggia aut Ausanai, Prapan aut Matsushita, Taro aut Enthalten in Radiological physics and technology Tokyo : Springer, 2008 4(2011), 2 vom: 11. Juni, Seite 194-202 (DE-627)571166032 (DE-600)2433581-2 1865-0341 nnns volume:4 year:2011 number:2 day:11 month:06 pages:194-202 https://dx.doi.org/10.1007/s12194-011-0123-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 4 2011 2 11 06 194-202 |
| spelling |
10.1007/s12194-011-0123-4 doi (DE-627)SPR025176625 (SPR)s12194-011-0123-4-e DE-627 ger DE-627 rakwb eng Murase, Kenya verfasserin aut Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011 Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it. Magnetic hyperthermia (dpeaa)DE-He213 Magnetic nanoparticle (dpeaa)DE-He213 Superparamagnetic iron oxide (SPIO) (dpeaa)DE-He213 Alternating magnetic field (dpeaa)DE-He213 Oonoki, Junko aut Takata, Hiroshige aut Song, Ruixiao aut Angraini, Anggia aut Ausanai, Prapan aut Matsushita, Taro aut Enthalten in Radiological physics and technology Tokyo : Springer, 2008 4(2011), 2 vom: 11. Juni, Seite 194-202 (DE-627)571166032 (DE-600)2433581-2 1865-0341 nnns volume:4 year:2011 number:2 day:11 month:06 pages:194-202 https://dx.doi.org/10.1007/s12194-011-0123-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 4 2011 2 11 06 194-202 |
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10.1007/s12194-011-0123-4 doi (DE-627)SPR025176625 (SPR)s12194-011-0123-4-e DE-627 ger DE-627 rakwb eng Murase, Kenya verfasserin aut Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011 Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it. Magnetic hyperthermia (dpeaa)DE-He213 Magnetic nanoparticle (dpeaa)DE-He213 Superparamagnetic iron oxide (SPIO) (dpeaa)DE-He213 Alternating magnetic field (dpeaa)DE-He213 Oonoki, Junko aut Takata, Hiroshige aut Song, Ruixiao aut Angraini, Anggia aut Ausanai, Prapan aut Matsushita, Taro aut Enthalten in Radiological physics and technology Tokyo : Springer, 2008 4(2011), 2 vom: 11. Juni, Seite 194-202 (DE-627)571166032 (DE-600)2433581-2 1865-0341 nnns volume:4 year:2011 number:2 day:11 month:06 pages:194-202 https://dx.doi.org/10.1007/s12194-011-0123-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 4 2011 2 11 06 194-202 |
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10.1007/s12194-011-0123-4 doi (DE-627)SPR025176625 (SPR)s12194-011-0123-4-e DE-627 ger DE-627 rakwb eng Murase, Kenya verfasserin aut Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011 Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it. Magnetic hyperthermia (dpeaa)DE-He213 Magnetic nanoparticle (dpeaa)DE-He213 Superparamagnetic iron oxide (SPIO) (dpeaa)DE-He213 Alternating magnetic field (dpeaa)DE-He213 Oonoki, Junko aut Takata, Hiroshige aut Song, Ruixiao aut Angraini, Anggia aut Ausanai, Prapan aut Matsushita, Taro aut Enthalten in Radiological physics and technology Tokyo : Springer, 2008 4(2011), 2 vom: 11. Juni, Seite 194-202 (DE-627)571166032 (DE-600)2433581-2 1865-0341 nnns volume:4 year:2011 number:2 day:11 month:06 pages:194-202 https://dx.doi.org/10.1007/s12194-011-0123-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 4 2011 2 11 06 194-202 |
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10.1007/s12194-011-0123-4 doi (DE-627)SPR025176625 (SPR)s12194-011-0123-4-e DE-627 ger DE-627 rakwb eng Murase, Kenya verfasserin aut Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011 Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it. Magnetic hyperthermia (dpeaa)DE-He213 Magnetic nanoparticle (dpeaa)DE-He213 Superparamagnetic iron oxide (SPIO) (dpeaa)DE-He213 Alternating magnetic field (dpeaa)DE-He213 Oonoki, Junko aut Takata, Hiroshige aut Song, Ruixiao aut Angraini, Anggia aut Ausanai, Prapan aut Matsushita, Taro aut Enthalten in Radiological physics and technology Tokyo : Springer, 2008 4(2011), 2 vom: 11. Juni, Seite 194-202 (DE-627)571166032 (DE-600)2433581-2 1865-0341 nnns volume:4 year:2011 number:2 day:11 month:06 pages:194-202 https://dx.doi.org/10.1007/s12194-011-0123-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 4 2011 2 11 06 194-202 |
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Enthalten in Radiological physics and technology 4(2011), 2 vom: 11. Juni, Seite 194-202 volume:4 year:2011 number:2 day:11 month:06 pages:194-202 |
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Enthalten in Radiological physics and technology 4(2011), 2 vom: 11. Juni, Seite 194-202 volume:4 year:2011 number:2 day:11 month:06 pages:194-202 |
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Murase, Kenya @@aut@@ Oonoki, Junko @@aut@@ Takata, Hiroshige @@aut@@ Song, Ruixiao @@aut@@ Angraini, Anggia @@aut@@ Ausanai, Prapan @@aut@@ Matsushita, Taro @@aut@@ |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR025176625</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230519214014.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s2011 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s12194-011-0123-4</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR025176625</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s12194-011-0123-4-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Murase, Kenya</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2011</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Magnetic hyperthermia</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Magnetic nanoparticle</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Superparamagnetic iron oxide (SPIO)</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Alternating magnetic field</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Oonoki, Junko</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Takata, Hiroshige</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Song, Ruixiao</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Angraini, Anggia</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ausanai, Prapan</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Matsushita, Taro</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Radiological physics and technology</subfield><subfield code="d">Tokyo : Springer, 2008</subfield><subfield code="g">4(2011), 2 vom: 11. 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simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles |
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Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles |
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Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it. © Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011 |
| abstractGer |
Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it. © Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011 |
| abstract_unstemmed |
Abstract Our purpose of this study was to present simulation and experimental studies on magnetic hyperthermia (MH) with use of an alternating magnetic field (AMF) and superparamagnetic iron oxide nanoparticles ($ Resovist^{®} $). In the simulation studies, the energy dissipation (P) and temperature rise rate (∆T/∆t) were computed under various conditions by use of the probability density function of the particle size distribution based on a log-normal distribution. P and ∆T/∆t and their dependence on the frequency of the AMF (f) largely depended on the particle size of $ Resovist^{®} $. P and ∆T/∆t reached maximum at a diameter of ~24 nm, and were proportional to the amplitude of the AMF (H0) raised to a power of ~2.0. In the experimental studies, we made a device for generating an AMF, and measured the temperature rise under various concentrations of $ Resovist^{®} $, H0, and f. The temperature rise at 10 min after the start of heating was linearly proportional to the concentration of $ Resovist^{®} $, and proportional to H0 raised to a power of ~2.4, which was slightly greater than that expected from the simulation studies. There was a tendency for the temperature rise to saturate with increasing f. In conclusion, this study will be useful for investigating the feasibility of MH with $ Resovist^{®} $ and optimizing the parameters for it. © Japanese Society of Radiological Technology and Japan Society of Medical Physics 2011 |
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Simulation and experimental studies on magnetic hyperthermia with use of superparamagnetic iron oxide nanoparticles |
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Oonoki, Junko Takata, Hiroshige Song, Ruixiao Angraini, Anggia Ausanai, Prapan Matsushita, Taro |
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Oonoki, Junko Takata, Hiroshige Song, Ruixiao Angraini, Anggia Ausanai, Prapan Matsushita, Taro |
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10.1007/s12194-011-0123-4 |
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| score |
7.4002256 |