Sentence examples for the preferred particle from inspiring English sources

A Box-Behnken design was used to determine the preparation parameters that would achieve the preferred particle size and high encapsulation efficiency.

Various formulations and process parameters were identified and optimized to obtain the preferred particle size, entrapment, and polydispersibility of the VEGF-NPs system.

We identified and optimized various formulations and process parameters to get the preferred particle size, entrapment, and polydispersibility of the VEGF-NPs, and incorporated the VEGF-NPs into the (poly ethylene oxide -poly(proxide -polyde)-propylenelene oxide -poly ethylene127 toxide -poly ethylenered VEGF-NPs thermoxidesitive gel system.

The reconstructed density shows some distortion in the direction normal to the plane of the preferred particle orientation, due to the missing data for orientations at >45° tilt.

This resolution limit can be attributed to preferred particle orientation on the cryo-EM grid, continuous conformational variations, and/or subtle structural heterogeneity in TRiC, which have been found in cryo-EM studies of group II chaperonins (Clare et al, 2008; Zhang et al, 2011).

This has allowed us to identify a preferred particle morphology for efficient desilication.

This resulted in preferred particle orientations, which facilitated sorting of subpopulations, and enabled us to take advantage of random conical tilt (Radermacher et al, 1987).

The flowline density is the density of flowlines per grid cell, where flowlines are particle trajectories calculated by modelling the preferred path of particles starting at each grid cell and moving down slope under the effect of gravity58.

The TEM-measured width (wTEM) was converted to the width of the Oil-type faces (w{011}) to account for the preferred orientation of particles on the grid, and a specific surface area was calculated for each particle measured using the density of goethite (4.26 g/cm3) from Cornell and Schwertmann,[3]w{011}, LTEM, and θ (the angle between the 011-type faces).

The preferred menu of particles predicted by this model, in its simplest and most symmetrical form, is one in which all particles are exactly the same and have zero mass.

A specific response of the drawn films to an external magnetic stimulus was also visualized, and it was reasonably attributed to an effect of the magneto-anisotropy coming from the preferred orientation of the particle aggregates.