DC Field | Value | Language |
dc.contributor.author | LOPEZ SANCHEZ, ERICK JAVIER | - |
dc.contributor.author | ROMERO SANPEDRO, JUAN MANUEL | - |
dc.coverage.spatial | <dc:creator id="info:eu-repo/dai/mx/cvu/257697">ERICK JAVIER LOPEZ SANCHEZ</dc:creator> | - |
dc.coverage.spatial | <dc:creator id="info:eu-repo/dai/mx/cvu/239423">JUAN MANUEL ROMERO SANPEDRO</dc:creator> | - |
dc.coverage.temporal | <dc:subject>info:eu-repo/classification/cti/1</dc:subject> | - |
dc.date.accessioned | 2021-05-12T19:31:58Z | - |
dc.date.available | 2021-05-12T19:31:58Z | - |
dc.date.issued | 2017 | - |
dc.identifier.citation | arXiv.org Cornell University 2017 | en_US |
dc.identifier.uri | http://ilitia.cua.uam.mx:8080/jspui/handle/123456789/780 | - |
dc.description.abstract | The cable equation describes the voltage in a straight cylindrical cable, this model has been
employed to model electrical potential in dendrites and axons. However, sometimes this equation
might give incorrect predictions for some realistic geometries, in particular when the radius of the
cable changes significantly. Cables with a non constant radius are important for some phenomena, for
example discrete swellings along the axons appear in neurodegenerative diseases such as Alzheimer,
Parkinson, HIV-associated dementia and Multiple Sclerosis. In this paper, using the Frenet-Serret
frame, we propose a generalized cable equation for a general cable geometry. This generalized
equation depends on geometric quantities such as the curvature and torsion of the cable. We show
that when the cable has a constant circular cross-section, the first fundamental form of the cable can
be simplified and the generalized cable equation depends on neither the curvature nor the torsion of
the cable. Additionally, we find an exact solution for an ideal cable which has a particular variable
circular cross-section and zero curvature. For this case we show that when the cross-section of the
cable increases the voltage decreases. Inspired in this ideal case, we rewrite the generalized cable
equation as a diffusion equation with a source term generated by the cable geometry. This source
term depends on the cable cross-section area and its derivates. In addition, we study different cables
with swelling and provide their numerical solutions. The numerical solutions show that when the
cross-section of the cable has abrupt changes, its voltage is smaller than the voltage in the cylindrical
cable. Furthermore, these numerical solutions show that the voltage can be affected by geometrical
inhomogeneities on the cable | en_US |
dc.description.sponsorship | Cornell University | en_US |
dc.language.iso | Inglés | en_US |
dc.publisher | Nueva York : Cornell University | en_US |
dc.rights | https://arxiv.org/pdf/1702.00718.pdf | - |
dc.subject | Biofísica | en_US |
dc.subject | Ecuación del cable | en_US |
dc.subject | Ecuación generalizada | en_US |
dc.subject | Geometría del cable | en_US |
dc.title | Cable equation for general geometry | en_US |
dc.type | Artículo | en_US |
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