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A two-component mixing model, f ss = δ pw ‐ δ sw δ gas ‐ δ sw (5).
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(b) A mass balance model suggests an increasing fraction of secondary sulfate (f SS ) in sites with elevated temperatures.
Thus, the steady-state mean-square behavior is given by E w ̄ ss σ ¯ 2 = E w ̄ ss F ss σ ¯ 2 + b ss T σ ¯, (52).
This gives us the steady-state values for MSD and EMSE as follows: η ss = b ss T I M 2 N 2 − F ss − 1 q η, (54) ζ ss = b ss T I M 2 N 2 − F ss − 1 λ ζ. (55).
Incorporating these two steady-state relations in (33) yields the steady-state weighting matrix as F ss = I M 2 N 2 − I MN ⊙ Λ E D ss − Λ E D ss ⊙ I MN + E D ss ⊙ D ss A G T ⊙ G T, (51).
In the second GLM, G, F, SS, and SE trials were first distinguished.
The differences in the X-ray peaks between RT- and C-SS (d spacing = 1.9 5.2 Å) and F-SS (d spacing = 3.0 Å and 5.2 8.2 Å) were also measured.
The NH stretching (3200 2400 cm−1) of F-SS is also observed at a lower frequency with a broader band than RT-SS and C-SS due to the hydrogen bonding in the β-sheets.
Whereas, F-SS favours β-sheets structure proved by the amide bands shifting to a lower frequency.
Silk sericin (SS) powders were prepared by degumming processes with different storage temperatures before drying into the final powders; defined as RT-SS (room, 25 °C), C-SS (10 °C) and F-SS (freezing, 0 °C), and then fabricated into films and scaffolds by reacting with poly vinyl alcohol) (PVA) in the presence of a new cross-linker (dimethylolurea; DMU).
then f ∈ SS ∗.
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