2017
DOI: 10.1098/rspa.2016.0684
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‘Full fusion’ is not ineluctable during vesicular exocytosis of neurotransmitters by endocrine cells

Abstract: Vesicular exocytosis is an essential and ubiquitous process in neurons and endocrine cells by which neurotransmitters are released in synaptic clefts or extracellular fluids. It involves the fusion of a vesicle loaded with chemical messengers with the cell membrane through a nanometric fusion pore. In endocrine cells, unless it closes after some flickering (‘Kiss-and-Run’ events), this initial pore is supposed to expand exponentially, leading to a full integration of the vesicle membran… Show more

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Cited by 31 publications
(41 citation statements)
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“…The two quantities are proportional through the Faraday law. Herein, the time‐dependent quantity of ROS/RNS, Q in ( t ), present at time t inside the phagolysosome is then formulated as: truenormaldQin(t)normaldt=-k0falsediffρ(t)Qin(t)+normaldQprod(t)normaldt …”
Section: Figurementioning
confidence: 99%
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“…The two quantities are proportional through the Faraday law. Herein, the time‐dependent quantity of ROS/RNS, Q in ( t ), present at time t inside the phagolysosome is then formulated as: truenormaldQin(t)normaldt=-k0falsediffρ(t)Qin(t)+normaldQprod(t)normaldt …”
Section: Figurementioning
confidence: 99%
“…where Q prod ( t ) is a time‐dependent kinetic term accounting for the ROS/RNS production inside the phagolysosome during release; kdiffρ(t) is a pseudo‐rate constant featuring the diffusion‐controlled release out of the phagolysosome pore of time‐dependent radius ρ ( t ) . The current, i ( t ), featuring the ROS/RNS oxidation at the Pt‐NWE surface is then: truei(t)=k0falsediffρ(t)Qin(t) …”
Section: Figurementioning
confidence: 99%
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“…This amounts to assume that the diffusional equivalent of the Newton and Kelvin law of cooling applies, i.e., that diffusional equilibration within each type of nanodomains is much faster than exchanges between adjacent ones. 64,65 This leads at each instant to the fast setting of a quasi-steady state inside each nanodomain, so that f (θ) = [1 − exp(−k f θ)]. 64,65 It follows that to describe the current peak intensity at a given scan rate one may consider that the electrochemical system behaves as if it initially consisted of a single domain containing h A h {1 + γ[1 − exp(−k f RT /Fv)]} oxidizable adsorbed molecules irrespective of the fact that only h A h of them were initially adsorbed onto electroactive nanopatches before the voltammetric scan was initiated.…”
Section: Discussionmentioning
confidence: 99%
“…64,65 This leads at each instant to the fast setting of a quasi-steady state inside each nanodomain, so that f (θ) = [1 − exp(−k f θ)]. 64,65 It follows that to describe the current peak intensity at a given scan rate one may consider that the electrochemical system behaves as if it initially consisted of a single domain containing h A h {1 + γ[1 − exp(−k f RT /Fv)]} oxidizable adsorbed molecules irrespective of the fact that only h A h of them were initially adsorbed onto electroactive nanopatches before the voltammetric scan was initiated. In practice the kinetics of DA non−el ads molecules migration may be more intricate, e.g., involving radial or cylindrical diffusion according to the exact nanodomain shapes and their imbrication onto the electrode surface, 41,66,67 thus leading to more complex formulations of f (θ).…”
Section: Discussionmentioning
confidence: 99%