Equations of motion of an oblong aerosol particle in the neighbourhood of a cylinder placed crosswise to the main direction of carrier-gas flow are presented.
Silicon and metal nanowires, nanotubes, and nanorods which enable solar cells in decoupling light absorption from the direction of carrier transport have been studied by many researchers [3 6].
Nanowire, nanotube, and nanorod morphology provides direct conduction paths for electrons from the point of injection to the collection electrode and allows for the decoupling of light absorption from the direction of carrier transport along the longitudinal direction only, while the weblike and network structure of nanofibers has inherent anisotropy with a large variety of morphology.
The model predicts that as the spiral angle of the annular gratings increases, the probability that the traveling wave arrives from the direction of carrier grating motion must decrease.
At greater stimulus speeds, traveling wave arrival times encroach on the limits posed by the observer's reaction time, as the traveling waves become increasingly propelled in the direction of carrier grating motion.
The positive correlation between arrival time difference and stimulus motion is significant (Spearman's ρ 0.39, p = 0.01), as is the ratio between arrival times of traveling waves in the direction of carrier grating motion and those moving against it (p<0.05, t-test).
The goal of the in silico optimization was to find the possible directions of carrier modification in order to maximize FPF.
When stimulus speed is increased even further (to, say, 75°/s), this causes the motion direction of the carrier grating to fully dominate the traveling wave arrival direction.
These data show that traveling waves in binocular rivalry indeed tend to move faster in the direction of the carrier's motion when compared to the opposite direction (that of the mask stimulus' motion).
The data in figure 3 imply that when stimulus motion exceeds ∼±40°/s, the 50% point of the CCW probability is shifted spatially to the ±90° point, indicating that the speed of the traveling wave in the direction of the carrier grating is threefold the speed in the opposite direction.
