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Using the procedure discussed in this paper one can obtain a reduced order dynamic model, eliminate position vector gradients that introduce high frequencies to the solution of some problems, achieve the continuity of the remaining gradients at the nodal points, and obtain a formulation that automatically satisfies the principle of work and energy.
The values of k 1 and k 2 were estimated using the procedure discussed in Sect. 2.
The samples from acid-hydrolyzed DNA from blood and plants were spiked with 1 μmol L−1 for each G, A, C, and T, and analysis was carried out using the procedure discussed in the GC-FID portion.
We calculated the FAB, TCD, and CL at each location using the procedure discussed previously in Section 2. While moving the MPDC towards the RotA source (moving from L1 to L2, L3, and L4) and determining the electrogram characteristics at each location along the movement path, the variations in TCD and CL were examined.
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Point estimates for these odds ratios were used for our base case analysis, with 95% confidence intervals used for sensitivity analysis, using the procedures discussed below.
We were able to decoupled the DAE system into 4, 028 differential equations and 154 algebraic equations using the procedure we discussed in Section 3.2.1, i.e. n 10 = 4028, k 1 = 35 and k 0 = 119.
We decoupled the DAE system into 5, 727 differential equations and 34, 639 algebraic equations using the procedure we discussed in Section 3.1, i.e. n 0 = 5, 727 and k 0 = 34, 639.
The procedure discussed will be used in a forthcoming work for developing a methodology of designing the required height for a packed absorber for selective removal of H2S.
The gaps in SS ionosonde observations are filled up using the cloning procedure discussed in Gulyaeva et al. (2008).
The procedure discussed in the methodology is used to determine the extreme solutions.
The procedure discussed here are just guidelines.
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