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Temperature Dependence of the Specific Absorption Rate of a Frozen Ferrofluid
Presented by:Nathaniel MosherKettering UniversityFlint, Michigan
Other contributors:R.J. Tackett, R.E. Kumon, C. Rablau, E. Perkins-Harbin,L. Wang, J.S. Thakur, and P.P. Vaishnava
Specific Absorption Rate (SAR) of Ferrofluid
S𝐴𝑅 =𝑀𝑠𝑎𝑚𝑝𝑙𝑒
𝑚𝑁𝑃𝐶𝑖𝑐𝑒
∆𝑇
∆𝑡
𝑆𝐴𝑅 =𝑃
𝑚𝑁𝑃=𝜇0𝜋𝜒
′′𝑓𝐻02
𝑚𝑁𝑃
First Law of Thermodynamics in the Adiabatic Limit
Cice(T) per Yen, et. al. CRREL-81-10 (1981).
Turning off Brownian Relaxation by Freezing
VS
Fluid Dependent
Magnetic AnisotropyDependent
Brownian Relaxation Néel Relaxation
Synthesis of Fe3O4 via coprecipitation
Iron oxidenanoparticles
+NaOH
Add Dextran (15-20 kDa)
Dextran coated Fe3O4
Sonicate for 24 h
FeCl2.4H2O+
HCl(aq)
Add NH4OH
until pH 10
Iron oxide nanoparticles
FeCl3.6H2O+
HCl(aq)
Fe3O4
Nanoparticle
Dextran
Molecule
O2
protection
Sample is Fe3O4 with a 13.4 ±4.7 nm diameter
1.5 2.0 2.5 3.0
(44
2)
(53
1)
(44
0)
(33
3)
(42
2)
(33
1)
(40
0)
(22
2)
(31
1)
I (a
rb. unit
s)
d (Å)
(22
0)
Space Group: Fm3m
a = 8.36 Å
20 nm
0 5 10 15 20 25 30 350
5
10
15
20
25
Nu
mb
er o
f P
arti
cles
Nanoparticle diameter (nm)
𝐷 = 13.4 nm ± 4.7 nm
Experimental Setup for Hyperthermia
Copper coil
Amplification Circuit
TransformerC1 C2
Induction Heating System
Sample vial
Frozen ferrofluid
Thermometer
Fiber optic sensor
Computer
Thermal insulation
Temperature curves were recorded with/without alternate magnetic fields and then fitted
𝑆𝐴𝑅magnetic 𝑇 =𝑀sample
𝑚np𝐶ice 𝑇
∆𝑇magnetic
∆𝑡𝑆𝐴𝑅ambient 𝑇 =
𝑀sample
𝑚np𝐶ice 𝑇
∆𝑇ambient
∆𝑡
0 30 60 90 120 150 180 210 240 270-110
-100
-90
-80
-70
-60
-50
-40
Ambient
T (
°C)
t (s)
0 10 20 30 40 50 60 70 80-110
-100
-90
-80
-70
-60
-50
-40
150kHz
232kHz
T (
°C)
t (s)
Magnetic Field On Magnetic Field Off
SAR has significant ambient component that was subtracted
𝑆𝐴𝑅corrected 𝑇 = 𝑆𝐴𝑅magnetic 𝑇 − 𝑆𝐴𝑅ambient 𝑇
-110 -100 -90 -80 -70 -60 -50 -40
45
50
55
60
65
70
75
80
Uncorrected
Corrected
SA
R (
W/g
)
T (°C)
150 kHz
-110 -100 -90 -80 -70 -60 -50 -40
85
90
95
100
105
110
115
Uncorrected
Corrected
SA
R (
W/g
)
T (°C)
232 kHz
SAR shows a temperature dependence
-110 -100 -90 -80 -70 -60 -50 -4082
84
86
88
90
92
SA
R (
W/g
)T (°C)
232 kHz
~10 % decrease in SAR
over the temperature interval
-110 -100 -90 -80 -70 -60 -50 -40
44
46
48
50
52
54
56
SA
R (
W/g
)
T (°C)
150 kHz
~20 % decrease in SAR
over the temperature interval
0 10 20 30 40 50 60 70 80-110
-100
-90
-80
-70
-60
-50
-40
150kHz
232kHz
T (
°C)
t (s)
-110 -100 -90 -80 -70 -60 -50 -40
45
50
55
60
65
70
75
80
Uncorrected
Corrected
SA
R (
W/g
)
T (°C)
150 kHz
-110 -100 -90 -80 -70 -60 -50 -40
44
46
48
50
52
54
56
SA
R (
W/g
)
T (°C)
150 kHz
~20 % decrease in SAR
over the temperature interval
Summary
Conclusions
-110 -100 -90 -80 -70 -60 -50 -40
44
46
48
50
52
54
56
SA
R (
W/g
)
T (°C)
150 kHz
~20 % decrease in SAR
over the temperature interval• SAR shows
temperature
dependence
in Néel regime
• Ambient needs
correcting for
accurate results
Future Work
• Extending results to liquid samples
• Quantify Brownian contribution