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This encouraging behavior is attributed in part to the improved oxidation resistance of the BN at high energy levels and the ability of the BN to facilitate formation of a stable wear film at lower energy levels.
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The difference in scaling behavior is attributed to differences in flame structure.
This behavior is attributed to difference in adopted conduction pathways of protons and methanol molecules.
The reason for the better high-voltage cycling behavior is attributed to reduction in the side reactions that cause increase of the cell resistance during cycling.
This sliding behavior is attributed to differences in the third body formation (i.e. carbon based transfer- and tribo-film) and velocity accommodation modes, which are analyzed ex situ by means of X-ray photoelectron spectroscopy (XPS), micro-Raman spectroscopy and atomic force microscopy.
Such behavior is attributed to systematic variations in domain wall motion in relation to stress and λS.
The different behavior is attributed to the difference in spatial distributions of the interacting sites in the complexes.
This behavior is attributed to an increase in the crack nucleation probability with increasing sample size.
This behavior is attributed to the difference in morphology, with larger flexibility of the twisted and branched structure of G. lucidum, which make the failure more progressive and, therefore, smoother.
This behavior is attributed to the increase in stacking fault energy with the increase of Al content and stability of austenite, which depends on the local chemical variation.
This behavior is attributed to the differences in lamellar morphology (length scales ∼100 Å), especially the contribution of the amorphous regions, which determine the bulk properties.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com