Buckled surface

Buckled surface models for the two other copper sulfur phases were proposed that rationalised the STM, LEED and SEXAFS data (Figure 10.5). Note that the local adsorption site of the sulfur adatoms in both the p(3 x 2) and p(5 x 2) structures is the four-fold hollow in agreement with the SEXAFS18 measurements but looking at the structure from above with the STM, the periodicity of the structure suggests a variety of different adsorption sites. 

Harrison C, Stafford CM, Zhang WH, Karim A (2004) Sinusoidal phase grating created by a tunably buckled surface. Appl Phys Lett 85 4016—4018... 

C. Harrison, C. M. Stafford, W. Zhang, and A. Karim, Sinusoidal phase grating created by a tun-ably buckled surface. Appl. Phys. Lett. 85, 4016 (2004). 

In all boron three-dimensional (3D) structures, most of the atoms are members of the almost regular atomic triangles and form 6 bonds (five intra- and one inter-icosahedral bonds). This circumstance leads to the possibility to synthesize bare boron structures with triangular two-dimensional (2D) lattices, e.g., nanotubular boron in the form of cylindrically rolled fiat or buckling surfaces (Boustani et al. 1999). 

Bending and Forming Pipe may be bent to any radius for which the bend-arc surface will be free of cracks and substantially free of buckles. The use of bends which are creased or corrugated is permitted. Bending may be by any hot or cold method permissible within the radii and material characteristics of the pipe being bent. 

The plate buckling equations inherently cannot be derived from the equilibrium of a differential element. Instead, the buckling problem represents the departure from the equilibrium state when that state becomes unstable because the in-plane load is too high. The departure from the equilibrium state is accompanied by waves or buckles in the surface of the plate. That is, the plate cannot remain flat when the... 

The reverse-buckling disk, without knives but wth a pre-scored disk surface, offers some features that do not depend on the knives being in place because the thickness of the metal disk dome along the score line determines the bursting pressure of the disk. 

Fig. 1.82 Oxidation of a convex surface by cation diffusion the compressive stress in the initially formed oxide may lead to (a) failure by buckling or to (b) void precipitation...

Flame Cleaning Now little used as a preparatory method, flame cleaning is a process whereby an intensely hot oxyacetylene flame is played on the surface of the steel. In theory, differential expansion causes millscale to detach. In practice, there is evidence that the treatment may not remove thin, tightly adhering millscale. Also, steel less them 5 mm thick can buckle. Finally, the process can burn in chemicals deposited on the surface, causing premature paint failure. 

Stuart and Hlady [37] found that unintentional lateral forces influenced their measurements of adhesion between surface-bound protein molecules and colloid probe-bound ligands. They noted a greatly exaggerated separation distance and a stick-shp behavior in their adhesion curves, which they attribute to roUiug and buckling of the cantilever under the influence of lateral forces as the sample was retracted with the probe stuck to it. 

An example of a structural effect is on the gold (111) surface where there is an in-plane tangential surface pressure (, , 35) On extended surfaces, a hill-and-valley roughening occurs to accommodate the expansion, as described earlier. In contrast, small particles accommodate the pressure by a surface buckle ( ). We would expect similar behaviour when there is chemisorption involving interactions between the adsorbed molecules. 

FIGURE 27.8 Specular reflectivity for a clean Au(lOO) surface in vacuum at 310 K ( ). The solid line is calculated for an ideally terminated lattice. The dashed line is a fit to the data with a reconstmcted surface with a 25% increase in the surface density combined with a surface relaxation that increases the space between the top and next layers by 19%. In addition, the data indicate that the top layer is buckled or cormgated with a buckling amplitude of 20%. (From Gibbs et al., 1988, with permission from the American Physical Society.)... 

A line profile analysis of the saturated acetylide surface reveals the buckled nature of the overlayer with a periodicity of seven protrusions or 14 lattice units along the < 110 > axis. The nominal 14 units actually match 13 lattice units therefore to accommodate seven protrusions on 13 lattice units with equal spacing would result in surface buckling (Figure 5.13). The distance between two terminal silver atoms is 5.37 A, which is 2% shorter than that in silver acetylide based on the assumption of covalent radii. 

Figure 5.13 High-resolution image of a surface-saturated acetylide overlayer at 300 K. Below the image is a cross-section along the line A. Note the buckling of the adlayer. (Reproduced from Ref. 40).

The c(4 x 2)-2CO structure observed20 at Ni(lll) at room temperature has CO occupying both fee and hep threefold hollow adsorption sites with a surface coverage of 0.5 ML. So as to maximise the 0-0 distance, the molecular axis is tilted away from the surface normal towards atop positions. Corrugation of the adlayer is attributed to a CO-induced buckling of the surface nickel atoms, which is manifested by height differences between adjacent CO molecules (Figure 8.6). 

Phenyl iodide dissociates at Cu(110) to form a c(2 x 2) iodine layer, accompanied by coupling of phenyl groups which desorb as biphenyl but with evidence that some phenyl groups remain at the surface stabilised as chains at step-edges and on terraces as paired chains . Chemisorption of HC1 at Cu(110) is corrosive , with evidence for surface buckling. 

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