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The air-dried and hand-pestled fine grained fraction (<2 mm) of samples (LEF 1 and 18) was analysed for Ca, Fe, Na, and K concentrations using atomic absorption spectrometry (AAS, Perkin Elmer A-Analyst 300).
The basal 5 mm of samples were cut into 10-μm transverse sections and collected on 3-aminopropyl-triethoxisilan glass slides.
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The highest peak was obtained at 22 keV–125 mAs and 12 mm of sample thickness, with a DGS value around 0.65.
By definition, 1 mM of sample compound is equivalent to 2 mM TEAC.
Figure 13 represents the relation between the turns per meter and the electrical resistance in ohms per 100 mm of yarn samples at 25 °C and 65 % RH for samples A2 to A6.
The results were expressed as mean absorbance (optical density 450 mm) of duplicated samples minus the mean absorbance of the reagent blank divided by the cut-off value.
Fine milling (particle size <0.5 mm) of laboratory samples was performed using a universal cutting mill (Pulverisette 19, Fritsch, Idar-Oberstein, Germany).
We counted positively stained cells within or at the periphery of muscle fibers and calculated the density of positive cells per mm of muscle sample to allow direct comparison between samples.
With this first track, a constant fluence gradient dF/dx along the x-direction within the first 2 mm of the sample is achieved.
The RSM model predicted the 31.5 dB value of the highest absorption with low reflection (8.8 dB) at conditions of 7.7 wt% MWCNTs content, 3 mm of the sample thickness, and 12 GHz of incident EM wave frequency.
The mean third ventricle width of 5.26 ± 1.89 mm of our sample was comparable to, albeit slightly higher than, that of same-age multiple sclerosis patients in previous research (4.10 mm, Benedict et al., 2006 a ).
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