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254   Computational Modeling in Biomedical Engineering and Medical Physics


                hotspot that kills the cancer cells situated in the electrode range (Radiology). The heat
                source is then the electrothermal (Joule) effect. Numerical modeling may complement
                other medical assertive elements in the preinterventional phase with the aim of pre-
                cisely positioning the antenna and adjust its power level. An as simple and as accurate
                possible prediction of the RFA protocol is a desideratum, and to this aim difficulties
                related to the realistic representation of the tumor volume have to be surmounted.
                   Microwave ablation (MWA) is also a minimally invasive intervention used for the
                same indications as RFA to heat and kill the tumor. MWA provides low risk and a
                short hospital stay as an outpatient procedure, with overnight supervision in the hospi-
                tal if general anesthesia is recommended. The electrodes for RFA and interstitial
                MWA, specialized needle-like probes (Mulier et al., 2005), are inserted using an
                image-guided technique: magnetic resonance imagery (MRI), ultrasound (US), or
                computed tomography (CT). Multiple tumors may be treated simultaneously, and the
                procedure can be repeated if remittance occurs. RFA electrodes for soft tissue (kidney
                and liver) are expanding rapidly (Goldberg et al., 2003). Recently the International
                Working Group on Image-Guided Tumor Ablation (IWGIGTA) proposed their clas-
                sification. Many new electrodes, commercial and experimental, have been introduced
                since then, including “multiple electrode systems”.
                   The heat source characterization and its numerical modeling are one significant
                part of the problem. The other part is the heat transfer in vascularized tissues. This
                “physics” is usually addressed by the continuous media bioheat equation (Pennes)
                (Chapter 1: Physical, Mathematical, and Numerical Modeling), which accounts for the
                blood vessels heat transfer. However, this homogenization approach may be prone to
                underestimation of the required power levels for a successful procedure when larger
                than the capillaries vessels are present too.
                   This chapter presents several models of localized (interstitial) thermal therapy
                (hyperthermia and ablation) with a focus on modeling the power sources (power level
                and duration) and their sizing when applied to tissues where heat is conveyed through
                hemodynamic flow in larger size vessels and the tissue, approximated to be a saturated
                porous medium, called here the general heat transfer (GHT) model. The results are
                compared to those obtained by using the bioheat (BHT) model. The exposure to
                EMF is limited in time and power level to provide for the success of the procedure
                and to avoid the thermally produced damage of the neighboring healthy tissue.
                Numerical simulations may add to the experimental work in solving this matter (Sands
                and Layton, 2000), as affordable, noninvasive and accurate methods used to solve
                thought experiments and studies focused on patient-specific data, electrode design
                (Koda et al., 2011), procedure duration, and power level. Numerical experiments are
                normally performed on validated and reasonably realistic models of utmost utility for
                exploring a wide spectrum of correlations between various interventional parameters
                and for the assessment of corresponding physical consequences. For instance the power
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