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The solubility was seen to decrease with increasing CaO mol%, for all the glasses investigated, and all the compositions showed a gradual decrease in pH with time, and this was accounted for by the release of Na+ and Ca2+ ions into solution.
The concentration of the solution was kept at 0.05 mol l−1 for all the experiments.
The transition into the Henry's law region occurs over a range of loadings near 0.01 mol kg−1 for all temperatures.
Lipid concentrations (mol%) for all samples were compiled into two different profile matrices.
Since the Pareto front represents the outer bound of performance, in Figures 4 and 5 we used Y tot = 29,469 mol./cell for all cells; the results do not change significantly if the next higher or lower levels of Y tot are used instead.
Maximal areal productivities for all systems were obtained above 30 mol m−2 day−1.
The ɛmeas values for all liposome suspensions were ∼32,000 M−1 cm−1 at 1 mol % of Py-met-chol and were little different at a probe mole fraction of 5 mol %.
The same sample preparation method was used for all concentrations of RB which ranged from 10−7 to 10−11 mol L−1.
Using AFM, the Young's modulus for all nanoparticles was determined; values ranged from 18 ± 4 kPa (1.7% mol cross-linker) to 39 ± 43 kPa (15% mol cross-linker).
For all systems (54 to 180 atoms), the energy barriers were approximately 40 kcal mol-1 (n = 54) to 400 kcal mol-1 (n = 180), indicating a clear length dependence on the unfolding energy.
Under the CIRA/sodalime-filtered xenon arc conditions most likely to be representative of outdoor exposure, the Ea for gloss loss was ≤5 kcal/mol for all samples tested.
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