The AMC-8 system is capable of 3-D SAR control and its SAR distribution is more favourable than for the 2-D AMC-4 system. This result promises improvement in clinical tumour temperatures.

Background: Hyperthermic intraperitoneal chemotherapy (HIPEC) after cytoreductive surgery (CRS) is used for treating peritoneal metastases of various origins. Present HIPEC protocols have rarely been validated for relevant parameters such as optimal agent, duration and perfusate temperature. In vitro experiments are not completely representative of clinical circumstances. Therefore, a good preclinical in vivo HIPEC model is needed in which temperature distributions can be well-controlled and are stable throughout treatments. Methods: We designed a setup able to generate and maintain a homogeneous flow during a 90-min HIPEC procedure using our in-house developed treatment planning tools and computer aided design (CAD) techniques. Twelve rats were treated with heated phosphate-buffered saline (PBS) using two catheter setups (one vs. four- inflows) and extensive thermometry. Simulated and measured thermal distribution and core temperatures were evaluated for the different setups. Results: Overall, the four-inflow resulted in more stable and more homogeneous thermal distributions than the one-inflow, with lower standard deviations (0.79 °C vs. 1.41 °C at the outflow, respectively) and less thermal losses. The average thermal loss was 0.4 °C lower for rats treated with the four-inflow setup. Rat core temperatures were kept stable using occasional tail cooling, and rarely exceeded 39 °C. Conclusion: Increasing the number of inflow catheters from one to four resulted in increased flow and temperature homogeneity and stability. Tail cooling is an adequate technique to prevent rats from overheating during 90-min treatments. This validated design can improve accuracy in future in vivo experiments investigating the impact of relevant parameters on the efficacy of different HIPEC protocols.

Modeling convection in the urinary bladder is very important for accurate hyperthermia treatment planning in the pelvic area.

The limited aperture size through which the em-field of the applicator is emanated and the constraining of this em-field near the bolus' edge is related to the appearance of superficial 'hot spot' phenomena in radiative hyperthermia. Regarding systems based on the concept of the annular phased array two questions arise: (1) what is the relative strength of the radial component present in the incident field of the radiators, and (2) in what way are fringing fields related to the bolus size? To address both of the above questions, the spatial distribution of the em-field emanated through the aperture of an applicator of the Amsterdam four waveguide-array system has been investigated for a long bolus and a short bolus. The em vector field emanated by the applicator has been characterized in two perpendicular planes, i.e. the aperture midplane and the sagittal midplane. It should be noted that this distribution depends on the propagation conditions throughout the coupling bolus, the phantom and other volumes attached, such as other applicators. Therefore two sets of propagation conditions have been measured: (1) the minimum number of parameters determining the propagation of the em-field namely one single waveguide, one bolus and a homogeneous phantom, and (2) the propagation conditions as for the clinical setting. It is stressed that the study concerns one specific radiative hyperthermia system, namely the AMC four-waveguide array, but that, based on the similarities discussed above, results may be extrapolated towards other radiative hyperthermia systems. According to the current study, bolus prolongation might lead to a clear clinical improvement, which is due to a decrease of the fringing field amplitude compared to the field amplitude in the centre of the aperture midplane. Bolus prolongation will lead to an extended heating area, the field lines being more aligned to the patient's main axis.