ArticleBiophysical journal2006
Subconductance states of Cx30 gap junction channels: data from transfected HeLa cells versus data from a mathematical model.
Article in Biophysical journal, 2006. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 7 papers.
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7 citing papers in PubMed, 12 citations in OpenAlex.
- Membrane voltage multistability in coupled glial cells.bioRxiv : the preprint server for biology · 2026Article
- Gap Junction Channel Regulation: A Tale of Two Gates-Voltage Sensitivity of the Chemical Gate and Chemical Sensitivity of the Fast Voltage Gate.International journal of molecular sciences · 2024Review
- Modeling and analysis of voltage gating of gap junction channels at a single-channel level.Biophysical journal · 2023Article
- Article
- Replacement of a single cysteine in the fourth transmembrane region of zebrafish pannexin 1 alters hemichannel gating behavior.Experimental brain research · 2009Article
- The M34A mutant of Connexin26 reveals active conductance states in pore-suspending membranes.Journal of structural biology · 2009Article
- A stochastic four-state model of contingent gating of gap junction channels containing two "fast" gates sensitive to transjunctional voltage.Biophysical journal · 2009Article
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Authors and funding
3 authors at 2 institutions in 1 country.
Funding
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Abstract
Human HeLa cells expressing mouse connexin30 were used to study the electrical properties of gap junction channel substates. Experiments were performed on cell pairs using a dual voltage-clamp method. Single-channel currents revealed discrete levels attributable to a main state, a residual state, and five substates interposed, suggesting the operation of six subgates provided by the six connexins of a gap junction hemichannel. Substate conductances, gamma(j,substate), were unevenly distributed between the main-state and the residual-state conductance (gamma(j,main state) = 141 pS, gamma(j,residual state) = 21 pS). Activation of the first subgate reduced the channel conductance by approximately 30%, and activation of subsequent subgates resulted in conductance decrements of 10-15% each. Current transitions between the states were fast (<2 ms). Substate events were usually demarcated by transitions from and back to the main state; transitions among substates were rare. Hence, subgates are recruited simultaneously rather than sequentially. The incidence of substate events was larger at larger gradients of V(j). Frequency and duration of substate events increased with increasing number of synchronously activated subgates. Our mathematical model, which describes the operation of gap junction channels, was expanded to include channel substates. Based on the established V(j)-sensitivity of gamma(j,main state) and gamma(j,residual state), the simulation yielded unique functions gamma(j,substate) = f(V(j)) for each substate. Hence, the spacing of subconductance levels between the channel main state and residual state were uneven and characteristic for each V(j).
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