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Hyperthermia and ablation  273


                   Fig. 8.13. It is important to underline that a supplementary restriction is introduced in
                   the study, and it refers to keeping the temperature within the therapeutic range. The
                   maximum temperature is easy to be monitored because it occurs near the radiating

                   slot of each antenna; it is set to 44 C, and the temperature control by the adjustment
                   of the feeding power of the antennae is thus applied if necessary.
                      For the next step of the analysis, the presence of a large blood vessel in the inter-
                   ventional zone is considered, as the computational domain in Fig. 8.15 is showing.
                   The numerical model is complemented with phenomena associated with the blood
                   flow through a large artery, that is, heat transfer by forced convection introduced in
                   Eq. (8.11b) and flow dynamics described in Eq. (8.13).
                      Some significant functional points are marked in Fig. 8.15: the Inlet is important
                   because an adequate boundary condition should be specified for the fluid flow at the
                   entrance of the bloodstream into the computational domain; Station Q represents the
                   exit point for the bloodstream; Station P marks the position of a temperature sensor
                   for the monitoring of the heating in the interventional region.
                      Three timescales govern the dynamics highlighted by the set of equations adopted
                   here: the problem of the electromagnetic wave evolves at high speed, or with the fast-
                   est time scale, followed by the flow problem at a slower time scale and finally the heat
                   transfer problem, which has the slowest evolution, that is, slowest time scale. The solv-
                   ing algorithm applied here for moderate hyperthermia does not take into consideration
                   the variation of physical properties with the temperature; in such circumstances, the
                   EMF problem, Eq. (8.10), is solved first and its solution is used for the estimate of the
                   resistive heat Q emf .
                      Heat transfer and flow, Eqs. (8.11b) and (13), should be solved in one step, due to
                   the convective term coupling. Aiming to get a proper balance between the actual
                   time step size, and the total time required to get the steady-state of the heating




















                   Figure 8.15 Computational domain with an arterial tree segment. Temperature is recorded at
                   Station P.
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