2004
DOI: 10.1109/tmag.2004.825436
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Computation of the Induced Current Density Into the Human Body Due to Relative LF Magnetic Field Generated by Realistic Devices

Abstract: A three-dimensional finite-element formulation to compute induced currents into the human body due to relative low-frequency magnetic field is described. Magnetic source field and induced currents are computed separately, allowing to handle sources due to realistic devices. This method is validated using analytical solutions over a sphere. The limit of validity of the formulation is established. Computations using an accurate model of the human body are presented.Index Terms-Bioelectric phenomena, dosimetry, q… Show more

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Cited by 12 publications
(11 citation statements)
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“…Therefore, a quasi-static approximation can be used, and the effects of the external electric and magnetic fields on the human body can be computed independently [31]. The magnetic permeability of the human body is similar to that of free space [32]. As a consequence, the magnetic field’s effect on the human body can be neglected, when considering indoor applications.…”
Section: Operation Principlementioning
confidence: 99%
“…Therefore, a quasi-static approximation can be used, and the effects of the external electric and magnetic fields on the human body can be computed independently [31]. The magnetic permeability of the human body is similar to that of free space [32]. As a consequence, the magnetic field’s effect on the human body can be neglected, when considering indoor applications.…”
Section: Operation Principlementioning
confidence: 99%
“…where b s is the imposed flux density to whi the body is exposed. e computational domain can thus be restried to the human body [15] with an imposed boundary condition at its surface given by: n · j| ∂Ω = 0. At the continuous level, these fields (together with associated potentials-see below) can be organized in the following Tonti's diagram [16]:…”
Section: F   mentioning
confidence: 99%
“…Faraday's law (1a) one obtains that: e = −∂ t a − grad ϕ, where ϕ is an unknown eleric scalar potential. e weak form of Ampère's law (1b) reads [15]: Find ϕ ∈ H(grad, ) su that…”
Section: F   mentioning
confidence: 99%
“…Due to the particular features of the living tissues, specific formulations have been developed [13]. …”
Section: Formulationmentioning
confidence: 99%