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The variations of grain size with pressure on compression and decompression at room temperature are illustrated in Fig. 8 for nano-Ni.
Open image in new window Figure 5 Variations of grain size and surface roughness as a function of argon gas flow.
The variations of grain size or particle size (nm) and dislocation density of semiconducting thin films with different substrate temperatures are shown in Fig. 6.
Figure 8 The variations of grain size with pressure on compression (upper panel) and decompression (lower panel) at room temperature for nano-Ni.
From analogy with fluvial compound channels, and fluvial theory, this reversal in secondary flow cell orientation is also expected to influence the spatial variations of grain size in submarine channel 'point-bar' deposits.
The variations of grain wear, grinding force and force ratio, and pile-up ratio were investigated under the conditions of undeformed chip thickness (UCT) ranging from 0.2 to 1 µm.
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The basic design parameter selected for optimization of these cells is the epitaxial layer thickness, through variation of grain size and grain boundary recombination velocity.
Variation of grain size fractions revealed that the pore geometry had a significant impact on gas release.
The lower coefficient of variation of grain size distribution suggesting a more homogeneous grain structure, was found to result in the lower fractal dimension of MRBC for the specimens with a similar grain boundary character distribution (GBCD).
Upon decompression, the variation of grain size of the samples (lower panel of Fig. 8) shows a similar but reversible trend as observed during compression, with the grain size reverting back to the starting values on fully releasing the pressure.
Predictions are made for the variation of grain size with refiner addition level, solute content in the melt and cooling rate.
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