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Comparison of Temperature Distribution in Agar Phantom and Gel Bolus Phantom by Radiofrequency Hyperthermia

  • Jung, Dong Kyung (Department of Radiation Oncology, Daegu Fatima Hospital) ;
  • Kim, Sung Kyu (Departments of Radiation Oncology, Yeungnam University College of Medicine) ;
  • Lee, Joon Ha (Department of Biochemistry & Molecular Biology, Yeungnam University College of Medicine) ;
  • Youn, Sang Mo (Department of Radiation Oncology, Daegu Fatima Hospital) ;
  • Kim, Hyung Dong (Department of Radiation Oncology, Daegu Fatima Hospital) ;
  • Oh, Se An (Department of Radiation Oncology, Yeungnam University Medical Center) ;
  • Park, Jae Won (Departments of Radiation Oncology, Yeungnam University College of Medicine) ;
  • Yea, Ji Won (Departments of Radiation Oncology, Yeungnam University College of Medicine)
  • Received : 2016.12.16
  • Published : 2016.12.31

Abstract

The usefulness of Gel Bolus phantom was investigated by comparing the temperature distribution characteristic of the agar phantom produced to investigate the dose distribution characteristic of radiofrequency hyperthermia device with that of the Gel Bolus phantom under conditions similar to those of an agar phantom that can continuously carry out temperature measurement. The temperatures of the agar phantom and the Gel Bolus phantom were raised to $36.5{\pm}3^{\circ}C$ and a temperature sensing was inserted at depths of 5, 10, and 15 cm from the phantom central axis. The temperature increase rate and the coefficient of determination were analyzed while applying output powers of 100 W and 150 W, respectively, at intervals of 1 min for 60 min under conditions where the indoor temperature was in the range $24.5{\sim}27.5^{\circ}C$, humidity was 35~40%, internal cooling temperature of the electrode was $20^{\circ}C$, size of the upper electrode was 250 mm, and the size of the lower electrode was 250 mm. The coefficients of determination of 150 W output power at the depth point of 5 cm from the central axis of the phantom were analyzed to be 0.9946 and 0.9926 in the agar and Gel Bolus phantoms, respectively; moreover, the temperature change equation of the agar and Gel Bolus phantoms with time can be expressed as follows in the state the phantom temperature is raised to $36^{\circ}C:Y(G)$ is equation of Gel Bolus phantoms (in 5 cm depth) applying output power of 150 W. Y(G)=0.157X+36. It can be seen that if the temperature is measured in this case, the Gel Bolus phantom value can be converted to the measured value of the agar phantom. As a result of comparing the temperature distribution characteristics of the agar phantom of a human-body-equivalent material with those of the Gel Bolus phantom that can be continuously used, the usefulness of Gel Bolus phantom was exhibited.

Keywords

References

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