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Set a "closed" time for the kitchen.
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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.
24 In brief, at 10 years of age, these measures included: time to cross a 2 m balance beam, walking heel-to-toe; heel-to-toe balance on a beam, eyes open and closed (time balance maintained up to a maximum of 20 s); and standing on one leg, eyes open and closed (time balance maintained up to a maximum of 20 s).
Data for in-use open container stability does not have to be collected at a closed container time of interest to estimate in-use degradation at this time point as long as this point is within the range of the experiment.
Let's try to set up a paradoxical situation using the little closed time loop above.
It should be noted that both graphs are linked because each couple (MFI and NV) corresponded to a single couple (mean burst size and mean closed time).
As detailed in Materials and methods, the critical end-burst closed time was calculated from the analysis of closed time distributions.
However, mean closed time was lower in induced tgind β2a suggesting that a portion of overexpressed β2a exerts functional action similar to the recombinant channel data presented.
To define the end-burst critical closed times, the closed time distributions were constructed and fitted with four or five exponential components (confidence interval 95%).
One could consider unbinding from the fully-bound open state but such transition would affect open and closed time distributions.
The closed time distributions determined for currents measured in patches from VB and RT areas could be fitted with at least three exponential components (not shown).
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