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Periodic surface profile

MORPHOLOGIES OF PERIODIC SURFACE PROFILES AND SMALL PARTICLES A SOURCE OF STEP AND STEP INTERACTION ENERGIES... [Pg.41]

Periodic surface profiles on vicinal surfaces have received considerable attention in the past, both from a continuum as well as an atomistic point of view [8-18], Here we describe briefly some recent work for surfaces of miscut a (about 3-10°) based on continuum mechanics specifically designed to take the anisotropy of y(0) into account [18], The approach is based on eq. (1) and the excess chemical potential given by [2]... [Pg.43]

For example, the surface self-diffusion coefficient can be measured by etching a periodic surface profile (e.g., sinusoidal) into a single-crystal surface. The amplitude of the profile is measured as a function of time via the intensity distribution of a laser diffraction pattern generated by the profile itself [52]. The self-diffusion coefficient can be evaluated from the change of the profile amplitude A (/) with time as the surface relaxes into its equilibrium surface structure upon heating ... [Pg.342]

Hager, J. and Spohn, H. (1995), Self-similar morphology and dynamics of periodic surface profiles below the roughening transition. Surface Science 324,... [Pg.784]

The formation of bottom-up block copolymer patterns within or on top-down substrate patterns is the basis for so-called templated self-assembly processes, in which long-range order and orientation of microdomain patterns can be imposed by a template or guide . These top-down templates can take a variety of forms including periodic thickness profiles and chemically patterned surfaces. [Pg.210]

The temperature of the fin base i90 is different from that of the surface where no fins are present, dW2. The heat flux through the fin base into the fin is significantly higher than the flux from the base material, i.e. the wall, into the fluid. The temperature drop which appears underneath the fin causes a periodic temperature profile to develop in the base material. This is shown schematically in Fig. 1.16. As a simplification this complicated temperature change is neglected, such that... [Pg.35]

Fig. 1.16 Periodic temperature profile along the line CD. i9o average temperature of the fin base, W2 average temperature of the surface of the base material between the fins... Fig. 1.16 Periodic temperature profile along the line CD. i9o average temperature of the fin base, W2 average temperature of the surface of the base material between the fins...
In order to fully understand wear in the oral environment, in vivo clinical trials are required. These are necessarily complex studies, run over substantial periods of time to account for the fact that tooth wear is a rather slow process in all but the most extreme conditions. Additional confounding variables, such as diet, illness and environment, are difficult to avoid, which may reduce the power of any study to discriminate between test treatments. A further complication is the requirement to accurately measure minute changes in tooth surface profile on natural teeth. However, a number of studies have been reported and provide valuable information. [Pg.91]

Figure 12-5 is schematic real surface profiles do not have the regular periodicity shown there, nor is the position of the reference line automatically determined. The CLA or the RMS surface roughness is a statistically calculated quantity, to obtain which raw data must be suitably processed. Figure 12-6 shows schematically (with a surface profile of unrealistic ruggedness for convenience in illustrating the point) the kind of problem encountered with a stylus probe instrument. [Pg.313]

Now we consider a strongly nonlinear evolution of ID arrays of islands farther from the instability threshold studied by means of numerical simulations of eq.(5) using a pseudospectral method with periodic boundary conditions. For the parameter values corresponding to region 1 in Fig.3, near the instability threshold, one observes the formation of a sinusoidal surface profile. With the increase of the supercriticality (i.e. with the decrease of g from Qc = 1/4),... [Pg.131]

A technique which has been used to measure surface diffusion rates is scanning Auger electron spectroscopy, which can follow adsorbate diffusion. A particular Auger transition of the adsorbate under investigation is used as a monitor of relative concentration versus distance scanned across the surface. Profiles are recorded after heating periods to observe the change in concentration profile as a function of time and temperature. [Pg.342]

Diffraction grating A structure consisting of a periodic spatial variation of the dielectric constant, conductivity, or surface profile. [Pg.33]

Surface profiles with different periodicities and the same amplitudes yield the same results, althou the effect in use may be somewhat different. [Pg.171]


See other pages where Periodic surface profile is mentioned: [Pg.41]    [Pg.51]    [Pg.629]    [Pg.41]    [Pg.51]    [Pg.629]    [Pg.407]    [Pg.192]    [Pg.197]    [Pg.198]    [Pg.164]    [Pg.306]    [Pg.211]    [Pg.200]    [Pg.131]    [Pg.398]    [Pg.30]    [Pg.391]    [Pg.324]    [Pg.274]    [Pg.63]    [Pg.497]    [Pg.34]    [Pg.3134]    [Pg.171]    [Pg.154]    [Pg.155]    [Pg.407]    [Pg.145]    [Pg.1946]    [Pg.144]    [Pg.219]    [Pg.81]    [Pg.1012]    [Pg.200]    [Pg.198]   
See also in sourсe #XX -- [ Pg.41 , Pg.43 ]




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