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The results indicate that the orientation and stretch, as well as the tube survival probability, have strong dependence on the chain contour variable, especially in the high-shear-rate region.
Within the research for apedal, contour variable locomotion systems, the influence of an alternating magnetic field on the shape of the free surface of a magnetizable fluid (magnetic fluid) is studied.
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There was a strong linear correlation among shore parallel and cross-contour variable values, and this result gives confidence in the use of a depth contour-based survey to characterize the nearshore comprehensively and explore potential linkages to landscape variability.
Based on a modified expression of the rate of the convective constraint release, we present a new contour-variable model of constitutive equations in which the non-uniform segmental stretch and the non-Gaussian chain statistical treatment of the single chain are considered to describe the polymer chain dynamics and the rheological behavior of an entangled system composed of linear polymer chains.
τ is the Keldysh contour time variable, and T C is the time ordering along the Keldysh contour.
A friction stir welding (FSW) tool geometry, consisting of a shoulderless conical probe, is investigated for application to closed contour welding, variable thickness welding, and open-loop control welding.
This paper addresses the problem of B-spline surface interpolation of scattered points for a hull form design, which are not arbitrarily scattered, but can be arranged in a series of contours permitting variable number of points in the contours.
To correct this shortcoming of DF-type interface solutions for unconfined aquifers, we here adapt the outflow gap estimate of an analytical 2-D interface solution for infinitely thick aquifers to fit the 50%-salinity contour of variable-density solutions for finite-depth aquifers.
We further improve the accuracy of the interface toe location predicted with depth-integrated DF interface solutions by ∼20% (relative to the 50%-salinity contour of variable-density solutions) by combining the outflow-gap adjusted aquifer depth at the sea with a transverse-dispersion adjusted density ratio (Pool and Carrera, 2011), appropriately modified for unconfined flow.
The program equally subdivided the contour curves into variable length vectors.
However, the mean widening for progress variable contours of premixed turbulent flames in comparison with corresponding values of unstrained premixed laminar flames was insignificant, implying that the influence of turbulent eddies on the flame front broadening is negligible.
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CEO of Professional Science Editing for Scientists @ prosciediting.com