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The Brink's hypothesis used in previous calculations can at times lead to erroneous results.
We have calculated the electronegativity of the atoms of 103 elements of the periodic table using the ansatz suggested by Gordy by carefully allaying the dimensional mismatch seemingly prevalent in previous calculations.
Instead of bending downward above ρ0 as in previous calculations, the energy per particle of pure neutron matter ¯¯¯En kn) and the asymmetry energy A kf) now grow monotonically with density.
Differences in ocean NPP estimates in (16) and those in Fig. 1 and Table 1 result from (i) addition of Arctic and Antarctic monthly ice masks, (ii) correction of a rounding error in previous calculations of pixel area, and (iii) changes in the designation of the seasons to correspond with (3).
In previous calculations we report drastic geometric effects in the electronic structure of QD super-crystals, as the shape changes in 3D semiconductors, while in 2D the dielectric function peaks correspond to the predicted dipole transitions energies [J.F. Nossa, A.S. Camacho, J.L. Carrillo, Rev. Mex. Fis. 53 (7) (2007) 123].
The changes of individual TE transport coefficients are consistent with the tendencies found in previous calculations of Si NW [4], nanoporous Si [5], and Si NW computed here (not shown).
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As this prediction model only included genetic risk factors, we expect an improvement of the performance of advanced AMD risk assessment with additional environmental and demographic factors in prospective studies as in our previous calculations (18, 19).
However, the domain size used in the previous calculations was too small for heat conduction, so that the calculated results are domain dependent and the dendrite could not grow freely.
In order to assess this effect within the population, the proportion of products susceptible to the virus in Equation 2 (PProd_sus) has been varied from 10%, the value used in all previous calculations, to 60%.
The comparison of three sets of numerical results indicates that the stream function-vorticity solution using the approximate boundary conditions reported in the previous calculations predicts a longer flame length and a broader flame shape.
Thinking about the mass differences between Ga and Mn atoms, the obtained results show that it would be difficult to obtain a 'two-mode' behavior as that verified in our previous calculations for the Al x Ga1−xN alloys[20].
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