Show simple item record

dc.contributor.authorKelley, Craig
dc.contributor.authorNewton, Adam J H
dc.contributor.authorHrabetova, Sabina
dc.contributor.authorMcDougal, Robert A
dc.contributor.authorLytton, William W
dc.date.accessioned2022-08-30T15:28:02Z
dc.date.available2022-08-30T15:28:02Z
dc.date.issued2022-08-18
dc.identifier.citationKelley C, Newton AJH, Hrabetova S, McDougal RA, Lytton WW. Multiscale Computer Modeling of Spreading Depolarization in Brain Slices. eNeuro. 2022 Aug 18;9(4):ENEURO.0082-22.2022. doi: 10.1523/ENEURO.0082-22.2022. PMID: 35927026; PMCID: PMC9410770.en_US
dc.identifier.eissn2373-2822
dc.identifier.doi10.1523/ENEURO.0082-22.2022
dc.identifier.pmid35927026
dc.identifier.urihttp://hdl.handle.net/20.500.12648/7519
dc.description.abstractSpreading depolarization (SD) is a slow-moving wave of neuronal depolarization accompanied by a breakdown of ion concentration homeostasis, followed by long periods of neuronal silence (spreading depression), and is associated with several neurologic conditions. We developed multiscale (ions to tissue slice) computer models of SD in brain slices using the NEURON simulator: 36,000 neurons (two voltage-gated ion channels; three leak channels; three ion exchangers/pumps) in the extracellular space (ECS) of a slice (1 mm sides, varying thicknesses) with ion (K+, Cl-, Na+) and O2 diffusion and equilibration with a surrounding bath. Glia and neurons cleared K+ from the ECS via Na+/K+ pumps. SD propagated through the slices at realistic speeds of 2-4 mm/min, which increased by as much as 50% in models incorporating the effects of hypoxia or propionate. In both cases, the speedup was mediated principally by ECS shrinkage. Our model allows us to make testable predictions, including the following: (1) SD can be inhibited by enlarging ECS volume; (2) SD velocity will be greater in areas with greater neuronal density, total neuronal volume, or larger/more dendrites; (3) SD is all-or-none: initiating K+ bolus properties have little impact on SD speed; (4) Slice thickness influences SD because of relative hypoxia in the slice core, exacerbated by SD in a pathologic cycle; and (5) SD and high neuronal spike rates will be observed in the core of the slice. Cells in the periphery of the slice near an oxygenated bath will resist SD.en_US
dc.language.isoenen_US
dc.relation.urlhttps://www.eneuro.org/content/9/4/ENEURO.0082-22.2022.longen_US
dc.rightsCopyright © 2022 Kelley et al.
dc.rightsAttribution 4.0 International*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.subjectNEURONen_US
dc.subjectextracellular spaceen_US
dc.subjecthypoxiaen_US
dc.subjectreaction-diffusionen_US
dc.subjectspreading depolarizationen_US
dc.subjectspreading depressionen_US
dc.titleMultiscale Computer Modeling of Spreading Depolarization in Brain Slices.en_US
dc.typeArticle/Reviewen_US
dc.source.journaltitleeNeuroen_US
dc.source.volume9
dc.source.issue4
dc.source.countryUnited States
dc.source.countryUnited States
dc.description.versionVoRen_US
refterms.dateFOA2022-08-30T15:28:02Z
dc.description.institutionSUNY Downstateen_US
dc.description.departmentBiomedical engineeringen_US
dc.description.degreelevelN/Aen_US
dc.identifier.journaleNeuro


Files in this item

Thumbnail
Name:
ENEURO.0082-22.2022.full.pdf
Size:
2.553Mb
Format:
PDF

This item appears in the following Collection(s)

Show simple item record

Copyright © 2022 Kelley et al.
Except where otherwise noted, this item's license is described as Copyright © 2022 Kelley et al.