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The significant relationships between the surface charges, wettability and fineness of LFs show that impurities like clays are key factors in the flow of LF suspensions.
However, no correlation was found between the surface charges of bacterial cultures and their adhesion inhibition by the biosurfactant (corresponding correlation coefficients for resting and growing cells are 0.15 and −0.26).
Probably due to chemical interactions between the surface charges of the two surfactants and the synergetic effect, the enhancement in oil recovery was greater when the two surfactants were used as a mixture, rather than alone.
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This fact can be explained by the competition between the surface charge and solution chemistry as two important factors.
Hence, a good correlation is found between the surface charge of the bitumen droplet as measured by zeta potential and the work of adhesion at water bitumen interface.
One can then use the bi-orthogonality between the surface charge distribution, σ(r), and the surface dipole distribution, τ(r), to derive, a n m = Λ 2 π ∑ β, k a β k ∫ τ α m r n ^ ⋅ ∫ σ β k r β r − r β r − r β 3 d S β dS = Λ 2 π ∑ β, k K αβ mk a β k (24).
We predict no notable differences between the surface charge characteristics of CENP-V and the GFA- Pn domains (data not shown).
Given the previously demonstrated relationship between the surface charge density and solution substrate interfacial energy, these results indicate that the variation in interfacial energy observed here is due to the differences in protein surface charge density, which impacts the affinity of the substrates for the aqueous solution (i.e., the hydrophilicity).
As Figure 5c shows, the zeta potential exhibits an inverse linear relationship between the surface charge density and the interfacial energy, with the large negative zeta potential of fetuin A leading to the lowest value of α and the small zeta potential of OPN giving the largest value of α.
Especially, no correlation between the functionalization and/or the surface charge (ζ-potential), as well as the hydrodynamic diameter, was found for fluidic or immobilized MNP.
where t is the transport number of Cl− in a solution, k is the shape coefficient (k = 2.8 for pores between globules), η is the surface charge density and C is the average value of concentrations of the solutions from two sides of the membranes.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com