Shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulation
Axonal stimulation with electric currents is an effective method for controlling neural activity. An electric field parallel to the axon is widely accepted as the predominant component in the activation of an axon. However, recent studies indicate that the transverse component to the axolemma is als...
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| Format: | Article |
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PeerJ Inc.
2018-12-01
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| Online Access: | https://peerj.com/articles/6020.pdf |
| _version_ | 1797423894177513472 |
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| author | Hui Ye Jeffrey Ng |
| author_facet | Hui Ye Jeffrey Ng |
| author_sort | Hui Ye |
| collection | DOAJ |
| description | Axonal stimulation with electric currents is an effective method for controlling neural activity. An electric field parallel to the axon is widely accepted as the predominant component in the activation of an axon. However, recent studies indicate that the transverse component to the axolemma is also effective in depolarizing the axon. To quantitatively investigate the amount of axolemma polarization induced by a transverse electric field, we computed the transmembrane potential (Vm) for a conductive body that represents an unmyelinated axon (or the bare axon between the myelin sheath in a myelinated axon). We also computed the transmembrane potential of the sheath-covered axonal segment in a myelinated axon. We then systematically analyzed the biophysical factors that affect axonal polarization under transverse electric stimulation for both the bare and sheath-covered axons. Geometrical patterns of polarization of both axon types were dependent on field properties (magnitude and field orientation to the axon). Polarization of both axons was also dependent on their axolemma radii and electrical conductivities. The myelin provided a significant “shielding effect” against the transverse electric fields, preventing excessive axolemma depolarization. Demyelination could allow for prominent axolemma depolarization in the transverse electric field, via a significant increase in myelin conductivity. This shifts the voltage drop of the myelin sheath to the axolemma. Pathological changes at a cellular level should be considered when electric fields are used for the treatment of demyelination diseases. The calculated term for membrane polarization (Vm) could be used to modify the current cable equation that describes axon excitation by an external electric field to account for the activating effects of both parallel and transverse fields surrounding the target axon. |
| first_indexed | 2024-03-09T07:53:19Z |
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| id | doaj.art-27c68af71ef9429cbc0662bffc94c167 |
| institution | Directory Open Access Journal |
| issn | 2167-8359 |
| language | English |
| last_indexed | 2024-03-09T07:53:19Z |
| publishDate | 2018-12-01 |
| publisher | PeerJ Inc. |
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| spelling | doaj.art-27c68af71ef9429cbc0662bffc94c1672023-12-03T01:19:49ZengPeerJ Inc.PeerJ2167-83592018-12-016e602010.7717/peerj.6020Shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulationHui YeJeffrey NgAxonal stimulation with electric currents is an effective method for controlling neural activity. An electric field parallel to the axon is widely accepted as the predominant component in the activation of an axon. However, recent studies indicate that the transverse component to the axolemma is also effective in depolarizing the axon. To quantitatively investigate the amount of axolemma polarization induced by a transverse electric field, we computed the transmembrane potential (Vm) for a conductive body that represents an unmyelinated axon (or the bare axon between the myelin sheath in a myelinated axon). We also computed the transmembrane potential of the sheath-covered axonal segment in a myelinated axon. We then systematically analyzed the biophysical factors that affect axonal polarization under transverse electric stimulation for both the bare and sheath-covered axons. Geometrical patterns of polarization of both axon types were dependent on field properties (magnitude and field orientation to the axon). Polarization of both axons was also dependent on their axolemma radii and electrical conductivities. The myelin provided a significant “shielding effect” against the transverse electric fields, preventing excessive axolemma depolarization. Demyelination could allow for prominent axolemma depolarization in the transverse electric field, via a significant increase in myelin conductivity. This shifts the voltage drop of the myelin sheath to the axolemma. Pathological changes at a cellular level should be considered when electric fields are used for the treatment of demyelination diseases. The calculated term for membrane polarization (Vm) could be used to modify the current cable equation that describes axon excitation by an external electric field to account for the activating effects of both parallel and transverse fields surrounding the target axon.https://peerj.com/articles/6020.pdfTransverse fieldAxonShielding effectMyelinCable equationElectric stimulation |
| spellingShingle | Hui Ye Jeffrey Ng Shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulation PeerJ Transverse field Axon Shielding effect Myelin Cable equation Electric stimulation |
| title | Shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulation |
| title_full | Shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulation |
| title_fullStr | Shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulation |
| title_full_unstemmed | Shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulation |
| title_short | Shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulation |
| title_sort | shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulation |
| topic | Transverse field Axon Shielding effect Myelin Cable equation Electric stimulation |
| url | https://peerj.com/articles/6020.pdf |
| work_keys_str_mv | AT huiye shieldingeffectsofmyelinsheathonaxolemmadepolarizationundertransverseelectricfieldstimulation AT jeffreyng shieldingeffectsofmyelinsheathonaxolemmadepolarizationundertransverseelectricfieldstimulation |