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To determine the probability of spheres making contact with the loukoumasome by chance, we estimated the proportional volume of cytoplasm occupied by a 1 micron-thick layer coating the outside of the loukoumasomal torus.
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The random distribution of 200-nm spheres in 10 × 10 × 1 μm3 volume is simulated by assuming the probability profile of sphere-to-sphere overlap to show exponential decay, the exponent of which is assumed following the Hertzian model of elastic potential energy for contact of two identical elastic spheres at a given overlap displacement [47].
It was found that the formation probability of PEDOT hollow spheres depended on the concentration of PVP.
High probability of overlapping in action spheres of two technologies might lead to poor operating efficiency during gel injection.
By choosing N max r) large enough such that the probability of any premature termination of the sphere decoder is asymptotically no larger than (text {SNR}^{-d^_{n_{t},n_{r},K}(r)}), the overall error probability at most (2 cdot text {SNR}^{-d^_{n_{t},n_{r},K}(r)}), thereby achieving the same diversity (d^_{n_{t},n_{r},K}(r)).
Dalton had pictured atoms as spheres and compound atoms as characteristic arrangements of spheres.
Stimuli consisted of spheres, cubes, and tetrahedrons.
The formation of spheres were observed 10 15 days later.
Furthermore, the number of spheres was more significantly different in the secondary spheres than in the primary spheres.
After filtration and dissociation of spheres, another 10 days were needed for generation of secondary spheres.
Therefore, we could not distinguish between sphere size and number of spheres.
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