TY - CHAP

T1 - Multiscale analysis of myelinated axons

AU - Jerez-Hanckes, Carlos

AU - Martínez, Isabel A.

AU - Pettersson, Irina

AU - Rybalko, Volodymyr

N1 - Funding Information:
Acknowledgments This research was funded by the Swedish Foundation for International Cooperation in Research and Higher Education STINT CS2018-7908, Fondecyt Regular 1171491, and Conicyt-PFCHA/Doctorado Nacional/2018-21181809, whose support is warmly appreciated.
Publisher Copyright:
© 2021, The Author(s), under exclusive license to Springer Nature Switzerland AG.

PY - 2021

Y1 - 2021

N2 - We consider a three-dimensional model for a myelinated neuron, which includes Hodgkin–Huxley ordinary differential equations to represent membrane dynamics at Ranvier nodes (unmyelinated areas). Assuming a periodic microstructure with alternating myelinated and unmyelinated parts, we use homogenization methods to derive a one-dimensional nonlinear cable equation describing the potential propagation along the neuron. Since the resistivity of intracellular and extracellular domains is much smaller than the myelin resistivity, we assume this last one to be a perfect insulator and impose homogeneous Neumann boundary conditions on the myelin boundary. In contrast to the case when the conductivity of the myelin is nonzero, no additional terms appear in the one-dimensional limit equation, and the model geometry affects the limit solution implicitly through an auxiliary cell problem used to compute the effective coefficient. We present numerical examples revealing the forecasted dependence of the effective coefficient on the size of the Ranvier node.

AB - We consider a three-dimensional model for a myelinated neuron, which includes Hodgkin–Huxley ordinary differential equations to represent membrane dynamics at Ranvier nodes (unmyelinated areas). Assuming a periodic microstructure with alternating myelinated and unmyelinated parts, we use homogenization methods to derive a one-dimensional nonlinear cable equation describing the potential propagation along the neuron. Since the resistivity of intracellular and extracellular domains is much smaller than the myelin resistivity, we assume this last one to be a perfect insulator and impose homogeneous Neumann boundary conditions on the myelin boundary. In contrast to the case when the conductivity of the myelin is nonzero, no additional terms appear in the one-dimensional limit equation, and the model geometry affects the limit solution implicitly through an auxiliary cell problem used to compute the effective coefficient. We present numerical examples revealing the forecasted dependence of the effective coefficient on the size of the Ranvier node.

UR - http://www.scopus.com/inward/record.url?scp=85100969030&partnerID=8YFLogxK

U2 - 10.1007/978-3-030-62030-1_2

DO - 10.1007/978-3-030-62030-1_2

M3 - Chapter

AN - SCOPUS:85100969030

T3 - SEMA SIMAI Springer Series

SP - 17

EP - 35

BT - SEMA SIMAI Springer Series

PB - Springer Science and Business Media Deutschland GmbH

ER -