Modeling Current Sources for Neural Stimulation in COMSOL

Background: Computational modeling provides an important toolset for designing and analyzing neural stimulation devices to treat neurological disorders and diseases. Modeling enables efficient exploration of large parameter spaces, where preclinical and clinical studies would be infeasible. Current commercial finite element method software packages enable straightforward calculation of the potential distributions, but it is not always clear how to implement boundary conditions to appropriately represent metal stimulating electrodes. By quantifying the effects of different electrode representations on activation thresholds for model axons, we provide recommendations for accurate and efficient modeling of neural stimulating electrodes. Methods: We quantified the effects of different representations of current sources for neural stimulation in COMSOL Multiphysics for monopolar, bipolar, and multipolar electrode designs. Results: We recommend modeling each electrode contact as a thin platinum domain, modeling the electrode substrate with the conductivity of silicone, and either using a point current source in the center of each electrode contact or using a boundary current source. Alternatively, to avoid possible numerical instabilities associated with a large range of conductivity values (i.e., platinum and silicone) and to eliminate the small mesh elements required for thin electrode contacts, the electrode substrate can be assigned the conductivity of platinum by using insulating boundaries between the substrate and surrounding medium, and within the substrate to isolate the contacts from each other. When modeling more than one contact, we recommend using superposition by solving the model once for each contact, leaving inactive contacts floating, and superposing the resulting potentials. We computed comparable errors in activation thresholds across the different implementations in a simplified model (electrode in a homogeneous, isotropic medium), and in realistic models of rat spinal cord stimulation (SCS) and human deep brain stimulation, indicating that the recommended approaches are applicable to different stimulation targets.

[1]  J. B. Ranck,et al.  THE SPECIFIC IMPEDANCE OF THE DORSAL COLUMNS OF CAT: AN INISOTROPIC MEDIUM. , 1965, Experimental neurology.

[2]  J. Davis Silicone electrical insulation , 1959 .

[3]  Dustin Tyler,et al.  Optimizing nerve cuff stimulation of targeted regions through use of genetic algorithms , 2011, 2011 Annual International Conference of the IEEE Engineering in Medicine and Biology Society.

[4]  Kristen W. Carlson,et al.  Investigation of mechanisms of vagus nerve stimulation for seizure using finite element modeling , 2016, Epilepsy Research.

[5]  Michael L. Hines,et al.  The NEURON Book , 2006 .

[6]  J Holsheimer,et al.  MR assessment of the normal position of the spinal cord in the spinal canal. , 1994, AJNR. American journal of neuroradiology.

[7]  Andrian Sue,et al.  Development of HEATHER for Cochlear Implant Stimulation Using a New Modeling Workflow , 2015, IEEE Transactions on Biomedical Engineering.

[8]  L. Geddes,et al.  The specific resistance of biological material—A compendium of data for the biomedical engineer and physiologist , 1967, Medical and biological engineering.

[9]  Allen Taflove,et al.  Incorporation of the electrode–electrolyte interface into finite-element models of metal microelectrodes , 2008, Journal of neural engineering.

[10]  Valéria Paula Sassoli Fazan,et al.  Morphology and morphometry of the vagus nerve in male and female spontaneously hypertensive rats , 2008, Brain Research.

[11]  Warren M Grill,et al.  Analysis of the quasi-static approximation for calculating potentials generated by neural stimulation , 2008, Journal of neural engineering.

[12]  P. G. Larsson,et al.  Application of a computational model of vagus nerve stimulation , 2012, Acta neurologica Scandinavica.

[13]  Kevin L Kilgore,et al.  Computational Analysis of Kilohertz Frequency Spinal Cord Stimulation for Chronic Pain Management , 2015, Anesthesiology.

[14]  J. Latikka,et al.  Conductivity of living intracranial tissues. , 2001, Physics in medicine and biology.

[15]  C. McIntyre,et al.  Cellular effects of deep brain stimulation: model-based analysis of activation and inhibition. , 2004, Journal of neurophysiology.

[16]  Alain Glière,et al.  Current approaches to model extracellular electrical neural microstimulation , 2014, Front. Comput. Neurosci..

[17]  Bryan Howell,et al.  Quantifying axonal responses in patient-specific models of subthalamic deep brain stimulation , 2018, NeuroImage.

[18]  J. G. Webster,et al.  Analysis and Control of the Current Distribution under Circular Dispersive Electrodes , 1982, IEEE Transactions on Biomedical Engineering.

[19]  Jiping He,et al.  Paresthesia thresholds in spinal cord stimulation: a comparison of theoretical results with clinical data , 1993 .

[20]  K. Rijkers,et al.  Morphology of the human cervical vagus nerve: implications for vagus nerve stimulation treatment , 2016, Acta neurologica Scandinavica.

[21]  Marom Bikson,et al.  High‐Resolution Multi‐Scale Computational Model for Non‐Invasive Cervical Vagus Nerve Stimulation , 2018, Neuromodulation : journal of the International Neuromodulation Society.

[22]  C. McIntyre,et al.  Tissue and electrode capacitance reduce neural activation volumes during deep brain stimulation , 2005, Clinical Neurophysiology.

[23]  Nathan D. Crosby,et al.  Modulation of activity and conduction in single dorsal column axons by kilohertz-frequency spinal cord stimulation. , 2017, Journal of neurophysiology.

[24]  David R. Wozny,et al.  The electrical conductivity of human cerebrospinal fluid at body temperature , 1997, IEEE Transactions on Biomedical Engineering.

[25]  K. Foster,et al.  Dielectric Permittivity and Electrical Conductivity of Fluid Saturated Bone , 1983, IEEE Transactions on Biomedical Engineering.

[26]  W M Grill,et al.  Modeling the response of small myelinated axons in a compound nerve to kilohertz frequency signals , 2017, Journal of neural engineering.

[27]  Wenwei Yu,et al.  Influence of Different Geometric Representations of the Volume Conductor on Nerve Activation during Electrical Stimulation , 2014, Comput. Math. Methods Medicine.

[28]  C. McIntyre,et al.  Role of Soft-Tissue Heterogeneity in Computational Models of Deep Brain Stimulation , 2017, Brain Stimulation.

[29]  J. Newman Current Distribution on a Rotating Disk below the Limiting Current , 1966 .

[30]  C. McIntyre,et al.  Modeling the excitability of mammalian nerve fibers: influence of afterpotentials on the recovery cycle. , 2002, Journal of neurophysiology.

[31]  Warren M. Grill,et al.  Evaluation of Intradural Stimulation Efficiency and Selectivity in a Computational Model of Spinal Cord Stimulation , 2014, PloS one.

[32]  J. Newman Resistance for Flow of Current to a Disk , 1966 .