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From these computations, the transient structure of the flamelet, including ignition, is obtained.
The observed U-OH2 bond lengths for aqueous U IV are 2.41 ± 0.02 Å [41, 67], and there are 9 U-O(H2) bonds averaging 2.47 Å from these computations (Table 1).
But although accurate atomic data are obtained from these computations, they are traditionally carried out in jj-coupling and, hence, do often not allow for a simple LSJ classification of the atomic levels as needed by experiment.
From these computations, we characterized the criticality of proteins and our results were consistent with published experiments.
The salient observations from these computations were: 1) the vRBCs all exhibited comparatively similar patterns of variation from the responses of nRBC (unlike the G6PD variants considered above), and 2) the changes between high and low energy load in the variants were all similar to the changes observed for the nRBC.
Similar(55)
The fluid velocity, temperature, the local skin-friction coefficient and the local Nusselt and Sherwood numbers are determined from these numerical computations.
Apart from these parameter computations on sustained vowels, using complete speech utterances cepstral peak prominence measures and speaking rates were computed and analysed.
First, the simplest and often-used approach is just to ignore the missings and exclude these from the computations.
While these computations are far from easy our framework shows how to perform such an analysis.
It will follow from the computations that the free entropy dimension and free Hausdorff dimension of these sets is r.
From the computations we can guess that (a_{n+1}=C_{n}), (ngeq1).
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CEO of Professional Science Editing for Scientists @ prosciediting.com