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β2c or β2d as well as β1a, β1c, and β3a induced a minor to moderate increase in single-channel activity with no significant effects detected for closed times.
Analysis with this program included open times, closed times and open probabilities (Po), which were determined by half-amplitude threshold analysis of single-channel recordings as done before [29].
These properties, along with the long open and closed times of LPA-induced channel activity and its attendant [Ca2+]i increase (10-fold higher than elicited by deoxygenation in human SS cells; Figure S2), all differ from the deoxygenation-activated responses reported in the current work.
aMean closed times (1/ k on) are expressed as minutes.
The lack of significant difference in either open or closed times within bursts indicates that the opening/closing kinetics of α1β2γ2 and α3β2γ2 receptors do not differ.
Po is derived from the sum of individual channel opening times (O) and individual closed times (C), thus Po = O/(O + C).
Similar(45)
The channel exhibited closed dwell-time distributions that fitted well to a two-component probability density function; τ1 closed = 3 ± 1 ms and τ2 closed = 57 ± 15 ms. The two time constants differ in duration by > 10-fold, a property of a bursting channel, where τ1 closed is the closed time within a burst, and τ2 closed is the closed time between bursts.
In an asymmetric bilayer, the channel exhibited characteristic bursting pattern with two closed time distributions, τ1 closed = 5 ± 1 ms, τ2 closed = 47 ± 9 ms, and an open time distribution τ open = 13 ± 4 ms. The significant difference in τ open (13 ± 4 ms vs 55 ± 9 ms) suggests that mPiezo1 remains open for longer times in the presence of Yoda1.
As detailed in Materials and methods, the critical end-burst closed time was calculated from the analysis of closed time distributions.
Q: "I am sorry, I am sorry, during closed time — ah, downtime — do stores remain open?" A: "I would say probably half remain open year-round and the others actually close.
Barrow's history of 20th-century cosmologies takes us from steady-state to big bang theories, universes that create themselves in closed time loops, bouncing or eternally inflating universes, and "kinky", "deviant" or "Mixmaster" universes – the zoo of possible solutions to Einstein's equations is populated by strange fauna indeed.
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