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Nuclei are relatively dark and can be modeled as small elliptical areas in the stained images.
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These are latent defects that affect circuit reliability and can be modeled as small-delay defects.
The waves are modeled as small perturbations of isothermal steady states of the system.
The M = 7 ~ 8 asperities are modeled as smaller fracture energy areas whose nucleation size is smaller than the asperity size.
Thus, the power consumed in beyond ATIM window can be modeled as {small{begin{aligned} E_{legacy_beyondATIM} =& P_{rx} times T_{rx_data} + P_{tx} times T_{tx_data} & + P_{idle} times (T_{beyond}-T_{rx_data}-T_{tx_data}).
In the lattice calculations, a boron burnable particle is modeled as a small sphere located at the center of a concentric spherical cell, surrounded by the effective fuel particle zone and fuel-free graphite zone with the same volumetric ratios as in the real fuel pebble.
Assuming that the pool of M2 is homogeneous, we attribute a stronger influence of R1 on R2 relative to R3. Intuitively, a stronger influence is modeled as a smaller edge weight (shorter path distance), whereas a weaker influence is modeled as a larger edge weight (longer path distance).
While the large-scale pathloss and the shadow fading are modeled as position-dependent trace, the small-scale fading is modeled as a time-dependent trace.
Regional ecosystems are modeled as statistical aggregates of dynamically driven small-scale ecosystems.
Macro cells and small cells are modeled as independent homogeneous PPPs, and they are cooperative to cache contents based on the popularity ranking.
In this approach the ice field is modeled as a viscous fluid for very small strain rates and is assumed to flow plastically otherwise.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com