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A nonlinear model is developed that describes the relative formation dynamics.
Fig. 5 Relative formation energy per Na atom of 1T-Na x MoS2 with respect to 1H-Na x MoS2 as a function of Na concentration.
Relative formation energy calculations, phonon spectrum calculations, as well as finite-temperature molecular dynamics simulations confirm their stability and DFT calculations indicate that they are all semiconductors.
In this method, oil-based mud resistivity, relative oil-based mud permittivity, oil-based mudcake thickness, supply frequency, formation resistivity and relative formation permittivity are all considered synthetically.
The calculated relative formation energy ΔHf α,0) of the neutral transition metal impurities doped in nanowires and bulk are shown in Fig. 2, indicating that the chemical trends of defect energy are similar in the two cases.
Relative formation energy per Na atom of 1T-Na x MoS2 with respect to 1H-Na x MoS2 varies as increasing the Na-adsorption concentration constantly in Fig. 5.
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This procedure also allowed us to normalize the data on the 440 460 signal at 2.5 ns, so as to compare the relative formations of Car* in either lutein- or violaxanthin reconstituted proteins.
The relative clone formation ability was calculated as: relative clone formation ability = (mean experimental clone number/mean control clone number) × 100.
New bone formations (arrows) are observed between the graft materials (stars) and adjacent bones Fig. 4 Relative bone formation.
Figure 2 The calculated relative defect formation energies ΔHf α,0) of the neutral transition metal impurities in ZnO nanowires of different diameters and bulk case.
HA+rhBMP-2 group (35.2 ± 19.7%) showed more relative bone formation compared to the ABB group (28.9 ± 10.3%), but significant difference was not found (p = 0.886) (Fig. 4).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com