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Important differences with colloidal interactions in a bulk suspension arise due to the discontinuity in solvent properties at the interface.
This bulk suspension was mixed thoroughly using a magnetic stirrer bar then dispensed aseptically into 30 ml aliquots into flasks using a sterile Eppendorf Multipipette unit.
In this paper, we develop a multidimensional theory of the macroscopic mechanics of strongly flocculated colloidal suspensions to describe suspension transport, deformation and separation in terms of the bulk suspension velocity field and local average solids volume fraction alone.
The dimensionless permeate flux, ν−w (φb), depends only on the particle volume fraction in the bulk suspension, φb, and is given by ν−w = 0.0581φb−13 when the suspension is dilute (φb < 0.10).
The MNP-adsorbed HLM biomaterial (denoted as MNPamine/HLM) was magnetically separated from the bulk suspension of HLM, washed twice in phosphate buffer (pH 7.0), and adsorbed onto polished edge-plane pyrolytic graphite (EPG) electrodes.
The resulting permeate flux is vw(x) = τw(a4/3x 13νt-w/μ0, where x is filter entra4/3x 13νt-w/μ0 whereshear stress exerted on the boundary layer by the tangentisl filterf bulk suspentrancehrough the filter channel, a is the particle radius, and μ0 is the characteristic viscosity.
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For bulk suspensions that are salt-free, the only ions present are those from the charging process of the particles, which are counter-ions formed at the fluid-particle interface.
Theoretical and experimental results clearly show that, under confinement, the microstructure (ordering) of the suspension, the phase coexistence, the internal architecture of the particles (for the case of polymers and similar kind of soft colloids) and the effective depletion interaction arising in colloid polymer mixtures strongly differ from the ones observed in free bulk suspensions.
By directly visualizing transport into GUVs, the approach offers a high level of certainty and integrity compared to experiments on bulk suspensions of smaller vesicles.
Because of its electroactive nature, serotonin can be detected at the single-platelet and bulk-suspension level, making it an ideal a marker of δ-granule secretion.
Polymerization on an industrial scale is conducted using five basic methods: bulk, solution, suspension, emulsion, and gas-phase.
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