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The latter are translated into physicochemical properties and the corresponding boundary values for each property are defined.
The velocity field, pressure field and fluid pathlines are calculated in the three-dimensional, axi-symmetric flow domain for prescribed boundary values for the velocity components at inlet.
The range of values of scalar fields in turbulent flows is bounded by their boundary values, for passive scalars, and by a combination of boundary values, reaction rates, phase changes, etc., for active scalars.
In this paper, we compare 3 algorithms: (1) quasi-Monte Carlo; (2) Schervish's MULNOR; and (3) a bivariate version of Armitage's recursive formula proposed by Jennison and Turnbull, for calculating boundary values for the L-region bivariate design which takes account of the correlation between the outcomes.
We show that, although the most direct analogue of the scalar theorem on the existence of boundary values for pseudocontinuable functions with respect to Clark measures fails in the non-scalar situation, suitable vector-valued versions of such results can be found.
Recently, the genuine degenerate situation with zero boundary values for (1.7) has been discussed by Lei and Zheng [15].
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We used the 27% boundary value for the upper and lower group determination following (Kelley 1939).
It is worthwhile to point out that rigorously, ν = 0 is a boundary value for the Gamma distribution.
The initial boundary value for the Schrödinger equation in cylinders with base containing conical points was established in [1].
The first for loop is used to find the boundary value for each monitoring nodes that violate local constraints, its time complexity is a.
The upper boundary value for shedding rate, ksh,p of 0.4 h−1, was chosen based on in vitro measurement of the shedding rate.
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