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Exact(21)
The asymptotic values (a, i.e., saturated value) of the properties of the volume fraction, specific surface area, and cube-counting fractal dimension of the glass bead samples were greater than those for the silica gel samples primarily because of the intrinsic differences in the porous networks and local distribution of the pore size and connectivity.
For pyrite (FeS2 s)), the estimated saturation indices at 25°C (1 bar) in all the samples were greater than zero, sometimes by several orders of magnitude (Figure 4b).
The forward and backward peak current densities (If and Ib) of the MP/TiO2 samples were greater than NW + MP/TiO2, which was in turn higher than NW/TiO2 samples.
In contrast, the M s values calculated from the hysteresis loops measured at 10 K for these samples were greater than 0.80 Am2/kg (Fig. 3c f, Table 2).
Sample sizes vary in some cases, where there was insufficient sample to measure multiple steroids (e.g., some blood samples were greater than others, and could be assayed for more steroids).
The RNA Integrity Number (RIN) values of all the samples were greater than 6.
Similar(39)
Another obvious evidence for the exchange coupling is that the ratio Mr/Ms in the well-processed samples is greater than 0.828.
If the most similar distance samples are greater than 0.1, the repair effect is relatively poor.
This showed that the variation between the samples was greater than any changes induced by the exposure to X-rays.
It shows that the Si/Al ratios of the modified samples are greater than that of CUSY.
RNA integrity number of all the samples was greater than 7.0 and met the criterion for the subsequent microarray analysis.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com