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Using this equation [45], we weight the instantaneous rate of accretion, so that the steeper portion the curve, is most influential when accounting for overall carbon.
Tidal rivers in coastal deltas are dynamic in terms of variations in settings (e.g. Well 1995); changes of courses (e.g., Zhang et al. 2010), rate of accretion and erosion (e.g., Rogers et al. 2013) and the amount of water discharge/intake over short period.
In most galaxies, Wang et al. report, the rate of accretion of the supermassive black hole is slow, but the Milky Way seems to be an important exception.
At this stage the rate of accretion is proportional to R2, which is derived from the geometrical cross-section of an oligarch.
The actual evolutionary process during this accretion stage remains uncertain, as it can depend both on the rate of accretion and the transfer of angular momentum to the white dwarf companion.
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OIS 5e, 5c and 5a were marked by low rates of accretion, more extensive bioturbation and limited leaching.
However, the relationship between cecal digesta weight and DNA damage appeared to plateau at relatively moderate cecal digesta weights with higher rates of accretion not affecting the level of DNA damage.
This wide range of variation in rupture behavior is likely to be caused by variations in the nature of subduction due to plate age, convergence rate, amount of accretion sediments, geometrical irregularities including seamounts, overriding plates and back-arc activity.
We estimated the weighted average rate of carbon accretion as: frac{{Ab_{1} }}{{2b_{2} + 2}}.
However, topographic attributes play a deterministic role in the rate of C accretion in degraded sloping lands.
We show that a high rate of disk accretion onto the white dwarf surface resulted in temporary screening of its magnetic field and spin-up of the white dwarf to its present spin period.
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