1970
DOI: 10.1016/0001-6160(70)90006-4
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Decoration criteria for surface steps

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Cited by 70 publications
(67 citation statements)
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“…On the left-hand side of the top pore there is a narrow wedge, a wedge with a large value of α. In the section on heterogeneous nucleation we found that the nucleation barrier tends to zero as θ − α tends to zero and so wedges with large values of α have small nucleation barriers, see [13]. Thus on increasing the supersaturation nucleation will occur in the narrow wedge with α > 45 • before it occurs in the corners with α = 45 • .…”
Section: Nucleation At Phase Transitions In Porous Mediamentioning
confidence: 89%
“…On the left-hand side of the top pore there is a narrow wedge, a wedge with a large value of α. In the section on heterogeneous nucleation we found that the nucleation barrier tends to zero as θ − α tends to zero and so wedges with large values of α have small nucleation barriers, see [13]. Thus on increasing the supersaturation nucleation will occur in the narrow wedge with α > 45 • before it occurs in the corners with α = 45 • .…”
Section: Nucleation At Phase Transitions In Porous Mediamentioning
confidence: 89%
“…cosθ`1 4 cos 3 θ˙ (9) while the heterogeneous nucleation energy barrier in a wedge [79] with a characteristic length greater than the critical radius R˚is: ( 10) where θ is the contact angle of the nucleus at the surface, α is the angle of the wedge, and cos Figure 12a). The Equation (10) is valid for p180´αq {2 ď θ ď p180`αq {2 and 0 ď α ď 180˝.…”
Section: R˚" 2γmentioning
confidence: 99%
“…This behaviour is well described by classical nucleation theory 121 . The classical nucleation theory prediction for the nucleation barrier in a wedge is that the barrier has the form ∆F * (θ, β) 154 . Here θ is the contact angle the interface between the nucleus and the bulk phase makes with a flat surface.…”
Section: Wedgesmentioning
confidence: 99%