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CuDB enables reduction in fabrication process steps, can obtain higher interconnect density and enhanced thermal conductivity.
Hence, three successive steps can obtain the curve points: Up-sampling of the B-Spline coefficients; Averaging by (n + 1) moving average filters of size h; Filtering by a unit B-Spline kernel of degree n.
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This step can obtain the member sequences with quite stable secondary structures and decrease inaccuracy from secondary structure prediction software.
After above steps, we can obtain the calibration parameters matrix.
Following similar steps we can obtain the other three families of statement (4.2 - 4.4 4.2 - 4.4
Finally, through the above steps, we can obtain a sample of 21 × 21 × 4.
By the method of steps, we can obtain the expression of the (ii -solution on [ 0, 1 ] correspondii -solutionnitial condition φ ( t ).
Following the method of steps, we can obtain the expression of the (i -solution on [ 0, 1 ], whi -solutionesented in Figure 5. Figure 5 (i)-sonution to ( 5.8 ) ( λ = 1 ).
Repeating this operation, after a finite number of steps, we can obtain a graph (G^) that is a disjoint union of a connected component (G_{1} ) induced by (V (C) cup V (H _{1} )) and some acyclic graphs.
When we adopt the fully discrete CNFVE formulation to solve the 2D Sobolev equations at (t=2~mbox{s}), as soon as we perform 200 steps, we can obtain the numerical solution with accuracy 10−4 with respect to the norm (|cdot|_{1}) in (H_{0}^{1}(Omega)) (see Figure 2) such that the accumulation of truncation errors in the computational process is very slow (see the dotted line of Figure 4).
In the next step, one can obtain the reservoir fluid composition using phase behavior studies.
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