1990
DOI: 10.1088/0031-9155/35/11/005
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A fractal interpretation of the dielectric response of animal tissues

Abstract: An improvement to Schwan's model of the dielectric response of biological tissues is proposed which is based on a fractal interpretation of the power law behaviour (epsilon' alpha epsilon" alpha f"-1) often observed. This interpretation allows the response to be more specifically related to the sub-cellular and cellular organization of the tissue through its self-similar hierarchical nature. A number of examples are discussed ranging in tissue type from the mostly cellular liver tissue to nerve tissue (grey ma… Show more

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Cited by 65 publications
(46 citation statements)
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“…The tissue conductivities in the model were assigned the mean value from multiple compiled references; skin at 0.465 S/m, bone at 0.010 S/m, CSF at 1.654 S/m, gray matter at 0.276 S/ m, and white matter at 0.126 S/m (Crille et al 1922;Oswald 1937;Lepeschkin 1951;Freygang and Landau 1955;Ranck 1963;Radvan-Ziemnowicz et al 1964;Hasted 1973;Geddes 1987;De Mercato and Garcia Sanchez 1992;Gabriel and Gabriel 1996;Akhtari et al 2002;Kammer et al 2004); thus, each individual tetrahedron of the FEM was assigned the conductivity corresponding to its tissue type. Tissue permittivities were also assigned values reflective of trends in the literature (see Table 1) (Pethig and Kell 1987;Dissado 1990;Foster and Schwan 1996;Gabriel and Gabriel 1996;Hart et al 1996). The source was modeled as a figure-of-eight copper coil with two 3.5 cm radius windings made of a single turn of 7 mm radius copper wire.…”
Section: Mri Guided Finite Element Head Modelmentioning
confidence: 99%
“…The tissue conductivities in the model were assigned the mean value from multiple compiled references; skin at 0.465 S/m, bone at 0.010 S/m, CSF at 1.654 S/m, gray matter at 0.276 S/ m, and white matter at 0.126 S/m (Crille et al 1922;Oswald 1937;Lepeschkin 1951;Freygang and Landau 1955;Ranck 1963;Radvan-Ziemnowicz et al 1964;Hasted 1973;Geddes 1987;De Mercato and Garcia Sanchez 1992;Gabriel and Gabriel 1996;Akhtari et al 2002;Kammer et al 2004); thus, each individual tetrahedron of the FEM was assigned the conductivity corresponding to its tissue type. Tissue permittivities were also assigned values reflective of trends in the literature (see Table 1) (Pethig and Kell 1987;Dissado 1990;Foster and Schwan 1996;Gabriel and Gabriel 1996;Hart et al 1996). The source was modeled as a figure-of-eight copper coil with two 3.5 cm radius windings made of a single turn of 7 mm radius copper wire.…”
Section: Mri Guided Finite Element Head Modelmentioning
confidence: 99%
“…This type of response was termed anomalous low frequency dispersion (LFD) by Jonscher [9] since it commonly appears as the lowest frequency dispersion process observed, however the theoretical q-dc mechanism of Dissado and Hill [7] is not restricted to such low frequency for its operation [10] as it depends upon the speed of the charge carriers on restricted paths. The q-dc mechanism exhibits a characteristic (or threshold) frequency ω c that defines the cross-over between a high frequency range where charge carriers are bound together as dipoles giving only a weak dispersion, and a low frequency range where the charge carriers become free to move along the restricted paths.…”
Section: Dielectric Response Models Of Oil-paper Insulationmentioning
confidence: 99%
“…According to Nivikov et al [226], this type of hierarchical relaxation process should lead to a CC or HN relaxation behaviour. However, more details about the microscopic geometry of pressboard insulation are required to confirm whether this type of relaxation exists in the frequency band of our interest (10 -4 -10 3 Hz) [227].…”
Section: Loss Peak Behaviourmentioning
confidence: 98%
“…He has identified that [227], most of the biological systems are composed of self-similar hierarchal structures on average such that small structural units with their own dielectric responses are embedded in larger units which are themselves embedded in even larger units [227]. The dielectric susceptibility of such material can be characterised by a series of fractional power law similar to eq (6.4).…”
Section: Universal Relaxation Lawmentioning
confidence: 99%
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