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At high water saturations, the saturation exponent becomes a strongly increasing function of the fraction of oil-wet pores when the value of this parameter exceeds the percolation threshold of the lattice network and oil percolates spontaneously through network joining clusters of oil-wet pores.
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The phenomenon appears above a threshold of lattice mismatch (≈2%) between the film and substrate.
The percolation threshold of a 3D lattice is significantly less than pc(2) and determined to be pc(3) = 0.0977 ± 0.0008.
Beyond a certain threshold, they affect the lattice structure leading to remarkable flexibility in engineering many physical and mechanical properties of the polymer.
At each corner of the lattice there is a galaxy.
Plots made use of the lattice, ggplot2 and RBGL packages.
At the fourth level of the lattice, we discover a first potential concept contained in a formal concept containing 9 objects and 9 attributes one of which has a 75% ratio, i.e., satisfying our pruning threshold.
The set of all these matrices constitute the lattice group of the lattice: The lattice group provides an integral representation of the point group and these are related via the equation and moreover the following hold (Pitteri & Zanzotto, 2002 ▶): We notice that a change of basis in the lattice leaves the point group invariant, whereas the corresponding lattice groups are conjugated in.
For instance, merohedral twins are characterized by and having the same lattice; coincidence grain boundaries are twins by reticular merohedry with a grain boundary index being the order of the lattice of in the lattice of.
As the lattices do not overlap perfectly (see below), refinement of the lattice parameters was done using reflections from one twin domain only, rejecting all overlapped lattice nodes (l = 3 n).
A closer look at the lattice parameters a, b, c, and β reveals a prominent decrease of the lattice parameter b (–2.6 %) in contrast to the lattice parameters a (+0.9 %) and c (–0.8 %).
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