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Therefore, the effect of these variables on Density is weak and can be neglected.
This shows that the coupling impedance in the lower plasma density is weak and growth rate remains constant in this limit.
Because the electron density is weak and the coordination distance of >2.8 Å is longer than would be expected for Na+, we interpret this density as a water molecule.
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Although the dynamic mechanism can affect the ionospheric electron density, it mainly transports the ion and electron, and its influence on the total electron density is weak.
First, we consider the plasma density is weak.
Third, the variability in the exponent β suggests that the negative dependence of reproductive investment on parasite density is weak or may be confounded by other factors such as immune responses.
While electron density is weaker in this region of the Sir3 BAH-NCP structure, it appears that multiple arginines (R28, R29, R30, R32, and R34) line the acidic patch groove to make charged interactions with the NCP surface.
Electron density for the basic segment is weak, and somewhat divergent among the four copies in the tetramer.
We expect that the sheet current densities are weak or absent where there are no currents (e.g. in non-polar regions) and not wildly fluctuating.
But it is a crucial problem due to the fact that practically all-protective measurements like e.g. the choice of the cement, increased density of material and others are weak and insufficient.
The study of the influence of different kinetic parameters temparature, surface roughness, etc) on the methanol electrooxidation showed, in particular, that the current densities are weaker for electrodes having a large active surface.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com