In dead end filtration mode, we found that, depending on the transmembrane pressure, four particle transmission regimes could be distinguished.
From SEM measurements developed in STEM-HAADF mode, we found that nanoparticles are near sized to those values fixed experimentally also confirmed by AFM observations.
By application of slightly acidic polar organic mobile phases as preferred elution mode, we found that certain amounts of aprotic acetonitrile in protic methanol substantially increased enantioselectivity and resolution of amino acids in a structure-dependent manner.
For switching the computer to standby mode we found an effect of time, F (1, 85) = 5.17, p < .05, ηp = .06, but no effects of category, number of persons per office or their interactions.
For switching the computer to sleep mode, we found a marginal effect of time, F (1,82) = 2.91, p < .10, ηp = .03, such that during the course of our study, participants showed an overall positive effect: they were quicker to switch their computer to sleep mode (M = 6.0 before intervention versus M = 5.6 after intervention).
In this mode, we found Control-FREEC called on average 55 % more copy-number altered events than ENVE, but did not match ENVE's sensitivity in detecting sCNAs in three of the four comparisons across the AA and TCGA WES datasets (Additional file 2: Figure S4A,B).
Using only the rigid body modes, we find the classical theory and using the deformation normal modes, a high order theory is constructed.
In order to identify the appropriate modes, we find roots of the transfer function of the full system, (lambda_{1},ldots,lambda_{M}) (with corresponding poles (p_{1},ldots,p_{M})).
By analyzing the pressure field of defect modes, we found the waves are localized in the bend-shaped linear defect.
Out of the two modes, we found only fast mode to get reflected only when certain condition for the propagation angle is satisfied.
