Rsjp. Kaatee et al., A 27-MHZ CURRENT SOURCE INTERSTITIAL HYPERTHERMIA SYSTEM FOR SMALL ANIMALS, International journal of hyperthermia, 11(6), 1995, pp. 785-796
Citations number
18
Categorie Soggetti
Radiology,Nuclear Medicine & Medical Imaging",Oncology
Temperature distribution is an important factor in thermo-radiotherapy
and it is greatly dependent on the applied heating technique. Consist
ency of the heating method is therefore important in translating in vi
vo experimental data to the clinical situation. To further evaluate th
e combination of interstitial hyperthermia and interstitial radiothera
py, an experimental interstitial hyperthermia system has been develope
d for small (500-2000 mm(3)) tumours growing in the flank of a rat. Th
e system used reproduces the properties of our clinical current source
interstitial hyperthermia system. The heating system consists of four
applicators, each with independent tuning and power control. The appl
icators are situated inside plastic afterloading catheters and are cap
acitively coupled with the surrounding tissue. The tumour is heated th
rough dissipation of a 27 MHz current flowing to an external ground pl
ane. An effective RF-filter allows reliable thermocouple temperature m
easurements when the power is switched on. The tumour temperature is e
asily controlled by means of a continuous temperature read-out and a c
lear temperature display. A minimum temperature up to 46 degrees C can
be reached within 4-10 min and maintained (+/- 0.5 degrees C) through
out the treatment period. Modelling calculations performed for this he
ating system indicate that the applicator temperatures should be kept
equal in order to minimize the difference between maximum and minimum
tumour temperature. Significantly higher applicator currents are neede
d at larger distances from the ground plane. In addition, the homogene
ity of the temperature distribution is improved when either the tumour
is isolated or when the environmental temperature is increased. The c
alculations also show that temperature distribution is strongly depend
ent on effective heat conductivity. A description of the system and it
s performance is presented.