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MEDICAL<br />

HARVARD MEDICAL SCHOOL & MASSACHUSETTS GENERAL HOSPITAL, BOSTON, MA<br />

Microscopic Magnetic Field <strong>Simulation</strong>s with COMSOL Multiphysics<br />

Micro-magnetic fields hold the promise of new medical treatments. Researchers turn to modeling<br />

<strong>for</strong> designing a MEMS field generator device.<br />

BY GIORGIO BONMASSAR, HARVARD MEDICAL SCHOOL AND A.A. MARTINOS CENTER, MASSACHUSETTS GENERAL HOSPITAL<br />

Electrical stimulation is currently used<br />

as a therapeutic option <strong>for</strong> treating a<br />

wide range of human diseases including<br />

cardiovascular, sensory and neurological<br />

disorders. Despite the remarkable success<br />

of electrical stimulation, there are significant<br />

limitations to its application; these<br />

limitations include incompatibility with<br />

magnetic resonance imaging (MRI) and the<br />

association with tissue inflammation. Here,<br />

we present an alternative method that uses<br />

micro-magnetic fields instead of direct electrical<br />

currents to activate excitable tissue.<br />

MEMS Microinductor<br />

COMSOL Multiphysics allowed us to<br />

estimate microscopic magnetic fields generated<br />

by a custom made micro-coil. The<br />

field estimation was per<strong>for</strong>med using the<br />

AC/DC Module, which gives the ability to<br />

solve Maxwell equation <strong>for</strong> the description<br />

of electromagnetic fields with the magnetic<br />

quasi static approximation. This approximation<br />

holds when considering low<br />

frequencies and ignoring the contribution<br />

of the displacement<br />

currents. We<br />

studied the MEMS<br />

microinductor (Fig.<br />

1) designed to create<br />

a microscopic<br />

magnetic field using<br />

a 3D model of<br />

electromagnetic<br />

quasistatic approximation.<br />

An inductor is<br />

the ideal magnetic<br />

field generator, and<br />

it stores the magnetic<br />

field energy<br />

generated by the<br />

supplied electric<br />

current. The 3D<br />

model of the square<br />

inductor was solved<br />

<strong>for</strong> the electric and<br />

Fig. 1. Image of a μMS coil. The typical overall<br />

dimensions of the coils are 350 μm × 350 μm.<br />

magnetic potentials using the Lagrange<br />

Quadratic vector with constant input current.<br />

The geometry (Fig. 2) consisted of a<br />

680×680×400 µm block, which contained<br />

three different objects: a seven-turn coil<br />

composed of gold traces (red), surrounded<br />

by air and the tissue substrate (blue). The<br />

assumption made was that no displacement<br />

currents were present. However, a<br />

capacitive component may still have been<br />

Fig. 2. Geometrical model of the 7 turns spiral square<br />

inductor (red) on top of the neuronal tissue (blue)<br />

and connected to a current generator. This model of<br />

the proposed coils was used in the Finite Element 3D<br />

studies to estimate the induced currents in the tissue<br />

(i.e., 50μm).<br />

present in our stimulation. Future studies<br />

should address this important point.<br />

Micro-Magnetic Fields <strong>Simulation</strong><br />

In setting up the model, all set the<br />

steps were per<strong>for</strong>med in COMSOL Multiphysics,<br />

including: (1) drawing, (2) defining<br />

the boundary conditions, (3) meshing,<br />

(4) solving and (5) post-processing.<br />

The drawing procedure was facilitated<br />

by the existence of a similar example in<br />

the COMSOL Model Library named “Integrated<br />

Square-Shaped Spiral Inductor”.<br />

This model examines the case of a<br />

MEMS square inductor that is used <strong>for</strong><br />

LC bandpass filters but with fewer turns<br />

than in our case. As in the example, the<br />

boundary conditions allowed <strong>for</strong> the definition<br />

of the excitation with the use of a<br />

port. The mesh was a Delaunay set with<br />

a maximum element size of 2.5 10 -5 m on<br />

the coil domain and with the adaptive refine<br />

meshing option, generating a mesh<br />

consisting of 7,782 tetrahedral base mesh<br />

elements, and 61,685 degrees of freedom.<br />

Fig. 3. Distribution of the magnetic field (arrows) generated<br />

around the μMS coil as predicted by the 3D FEM simulations.<br />

The size of the arrow is directly proportional to the magnitude of<br />

the magnetic field (A/m) in each (x, y, z) point of space uni<strong>for</strong>mly<br />

sampled in 7×7×7 locations. The colormap represents the electric<br />

potential (V).<br />

4 2 // C O M S O L N E W S 2 0 1 1<br />

➮<br />

Cov ToC + – A<br />

➭<br />

42-43 CN Harvard 2011.indd 42 5/16/11 9:29 AM

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