An inverse boundary element method computational framework for designing optimal TMS coils
An inverse boundary element method and efficient optimisation techniques were combined to produce a versatile framework to design optimal TMS coils. The presented approach can be seen as an improvement and extension of the work introduced by Cobos Sanchez et al. [1] where the optimality of the resul...
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Published in | Engineering analysis with boundary elements Vol. 88; pp. 156 - 169 |
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Abstract | An inverse boundary element method and efficient optimisation techniques were combined to produce a versatile framework to design optimal TMS coils. The presented approach can be seen as an improvement and extension of the work introduced by Cobos Sanchez et al. [1] where the optimality of the resulting coil solutions was not guaranteed. This new numerical framework based on a constant boundary element method has been efficiently applied to produce optimal TMS coils with arbitrary geometry, allowing the inclusion of new coil features in the design process, such as optimised maximum current density or reduced temperature. Even the structural properties of the human head were considered using this approach at the design stage to produce more realistic TMS stimulators. Several examples of TMS coils were designed and simulated to demonstrate the validity of the proposed boundary element method approach, and the obtained results show that the described method is an efficient tool for the design of optimal TMS stimulators, which can be applied to a wide range of coil geometries and performance requirements considering the natural variability in the human head properties. |
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AbstractList | An inverse boundary element method and efficient optimisation techniques were combined to produce a versatile framework to design optimal TMS coils. The presented approach can be seen as an improvement and extension of the work introduced by Cobos Sanchez et al. [1] where the optimality of the resulting coil solutions was not guaranteed. This new numerical framework based on a constant boundary element method has been efficiently applied to produce optimal TMS coils with arbitrary geometry, allowing the inclusion of new coil features in the design process, such as optimised maximum current density or reduced temperature. Even the structural properties of the human head were considered using this approach at the design stage to produce more realistic TMS stimulators. Several examples of TMS coils were designed and simulated to demonstrate the validity of the proposed boundary element method approach, and the obtained results show that the described method is an efficient tool for the design of optimal TMS stimulators, which can be applied to a wide range of coil geometries and performance requirements considering the natural variability in the human head properties. |
Author | Garcia-Pacheco, Francisco Javier Hill, Justin Robert Cobos Sánchez, Clemente Rodriguez, Jose Maria Guerrero |
Author_xml | – sequence: 1 givenname: Clemente surname: Cobos Sánchez fullname: Cobos Sánchez, Clemente email: clemente.cobos@uca.es organization: Departamento Ingeniería de Sistemas y Electrónics, Avenida de la Universidad, 10, E-11519 Puerto Real Cádiz, Spain – sequence: 2 givenname: Francisco Javier surname: Garcia-Pacheco fullname: Garcia-Pacheco, Francisco Javier organization: Departamento de Matemáticas, Avenida de la Universidad, 10, E-11519, Puerto Real Cádiz, Spain – sequence: 3 givenname: Jose Maria Guerrero surname: Rodriguez fullname: Rodriguez, Jose Maria Guerrero organization: Departamento Ingeniería de Sistemas y Electrónics, Avenida de la Universidad, 10, E-11519 Puerto Real Cádiz, Spain – sequence: 4 givenname: Justin Robert surname: Hill fullname: Hill, Justin Robert organization: Department of Mathematics, Temple College, Temple Texas, 76504 USA |
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Cites_doi | 10.1215/20088752-2017-0016 10.1016/j.jmr.2014.04.015 10.1109/4235.985692 10.1016/j.enganabound.2017.02.007 10.1016/j.brs.2017.04.001 10.1016/j.brs.2012.02.005 10.1016/S0955-7997(97)00114-8 10.1016/j.enganabound.2007.11.015 10.1109/22.310584 10.1016/S0955-7997(96)00057-4 10.1016/j.enganabound.2015.06.004 10.1109/TMAG.2011.2159510 10.1088/0031-9155/55/11/007 10.1088/1361-6560/62/1/73 10.1016/j.enganabound.2010.11.001 10.1016/j.brs.2014.10.002 10.2528/PIERB10011504 10.1016/j.enganabound.2015.11.002 |
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