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This model yielded a regression line indicating that the average annual rate of telomere shortening (β1) was 139 bp (p <0.0001) and that the difference between the WS and control groups (β2) was −3.6 kbp, the group effect being significant (p = 0.00026).
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However, there was no statistical significant difference between the W-FAM and control mix in terms of the number of cycles to failure resulted from the VECD analysis.
We calculated the free energy difference between the W and CB states.
Here, we define the free energy difference between the W and CB states as ΔE = E W − E CB.
By calculating the free energy difference between the W and CB states, the dependence of wetting behaviors on the periodic nanopatterned geometrical parameters is studied.
This is because the liquid-solid interface energy difference between the W and CB states is smaller than the liquid-vapor interface energy difference between the CB and W states.
Fig. 4 The free energy difference between the W and CB states as the function of hole height H h under different nanohole radii (a).
We also calculated that the free energy difference between the W and CB states under the circumstance of nanohole radii and spacing is under a certain value.
(5) and (10), we can calculate the free energy difference between the W and CB states of a water droplet on a nanohole-patterned surface.
From Fig. 3a, we also note that the free energy difference between the W and CB states will ascend to a maximum value and then descend before the radii reach a critical value.
Figure 4b shows a H h − R h phase diagram for the free energy difference between the W and CB states of a water droplet on a nanohole-patterned surface with the nanohole spacing as 300 nm.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com