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Surface thickness dependence

Examination of oven-aged samples has demonstrated that substantial degradation is limited to the outer surface (34), ie, the oxidation process is diffusion limited. Consistent with this conclusion is the observation that oxidation rates are dependent on sample thickness (32). Impact property measurements by high speed puncture tests have shown that the critical thickness of the degraded layer at which surface fracture changes from ductile to brittle is about 0.2 mm. Removal of the degraded layer restores ductiHty (34). Effects of embrittled surface thickness on impact have been studied using ABS coated with styrene—acrylonitrile copolymer (35). [Pg.203]

A web of molten plastic is pulled from the die into the nip between the top and middle roUs. At the nip, there is a very small rolling bank of melt. Pressure between the roUs is adjusted to produce sheet of the proper thickness and surface appearance. The necessary amount of pressure depends on the viscosity. For a given width, thickness depends on the balance between extmder output rate and the take-off rate of the pull roUs. A change in either the extmder screw speed or the puU-roU speed affects thickness. A constant thickness across the sheet requires a constant thickness of melt from the die. The die is equipped with bolts for adjusting the die-gap opening and with an adjustable choker bar or dam located inside the die a few centimeters behind the die opening. The choker bar restricts flow in the center of the die, helping to maintain a uniform flow rate across the entire die width. [Pg.140]

The attack of most glasses in water and acid is diffusion controlled and the thickness of the porous layer formed on the glass surface consequently depends on the square root of the time. There is ample evidence that the diffusion of alkali ions and basic oxides is thermally activated, suggesting that diffusion occurs either through small pores or through a compact body. The reacted zone is porous and can be further modified by attack and dissolution, if alkali is still present, or by further polymerisation. Consolidation of the structure generally requires thermal treatment. [Pg.880]

Unsuitable position of the reference electrode resulting in inclusion of a high ohmic potential drop between reference and working electrode. Moreover, when extended surfaces are used over which the mass transfer boundary layer thickness depends on position, a suitable number of independent reference electrodes should be used to measure local overpotentials on electrically isolated segments of the working electrode. [Pg.252]

Place several layers of filter paper on a smooth, hard surface, and place a blotting membrane on top (see Fig. 1). Depending on the size of the tissue, use a single- or double-edged razor blade to cut a tissue section 0.2-2.0 mm thick, depending on the particular tissue sample. It is necessary... [Pg.114]

The diffusion boundary layer thickness depends on D, and consequently the viscosity of the medium, r, and the geometry of the microorganism. In the absence of flow, the diffusion boundary layer of large or planar surfaces (n> > (5) can be defined by [40,43] ... [Pg.453]

Unlike the bulk morphology, block copolymer thin films are often characterized by thickness-dependent highly oriented domains, as a result of surface and interfacial energy minimization [115,116]. For example, in the simplest composition-symmetric (ID lamellae) coil-coil thin films, the overall trend when t>Lo is for the lamellae to be oriented parallel to the plane of the film [115]. Under symmetric boundary conditions, frustration cannot be avoided if t is not commensurate with L0 in a confined film and the lamellar period deviates from the bulk value by compressing the chain conformation [117]. Under asymmetric boundary conditions, an incomplete top layer composed of islands and holes of height Lo forms as in the incommensurate case [118]. However, it has also been observed that microdomains can reorient such that they are perpendicular to the surface [ 119], or they can take mixed orientations to relieve the constraint [66]. [Pg.204]

Stevenson [99] conducted the first polycondensation experiments with thin polymer melt films of 0.07-5 mm thickness. The experiments were performed on metal surfaces at temperatures between 265 and 285 °C under vacuum. He varied the kind of metal and observed that the behaviour of the polycondensation rate with decreasing film thickness depended on the metal being used. He concluded that the reaction rate increased only on metals soluble in the polymerizing melts... [Pg.75]

Polypyrrol is a polymeric support that can be used in immobilization of ONDs to surfaces. The generation of polypyrrol films can be by electrochemical co-polymerization of pyrrole and pyrrole-modified ONDs onto platinum electrodes. The polymer forms a black and insoluble film that is electrically conducting and whose thickness depends on the current used during the polymerization process (Fig. 14). The final surface density of the OND can be controlled by the ratio of pyrrole/OND being polymerized [53-55]. [Pg.93]

The heat flux transferred back from the gas phase to the burning surface is dependent on the temperature gradient in the gas phase, which is inversely proportional to the thickness of the reaction zone in the gas phase. Since the reaction in the gas phase is complete at the upper end of the bluish flame, the heat flux defined by Am conforms to the proportionality relationship Am l/6g p0- . The observed pressure dependence of the burning rate, is caused by the pressure depend-... [Pg.185]

The effect of aluminium on the surface area of goethite depends on the level of Al in the system and on the source of iron. Other conditions being equal, Al reduces both the rate of growth and the crystal size its effect on surface area depends on which of these two effects predominates. The surface area (EGME) of goethite grown from ferrihydrite in 0.3 M KOH at 25 °C dropped from 52 to 26 m g as the extent of Al substitution rose from 0 to 0.16 mol mol (Schulze and Schwertmann, 1987). This effect was attributed to an increase in crystal thickness along the [001] direction... [Pg.102]

Compared with the AP decomposition flame thickness, the fuel-oxidant redox flame extends a much greater distance from the propellant surface and depends on the rate of both chemical reaction and diffusional mixing. [Pg.258]


See other pages where Surface thickness dependence is mentioned: [Pg.696]    [Pg.157]    [Pg.155]    [Pg.255]    [Pg.528]    [Pg.227]    [Pg.469]    [Pg.422]    [Pg.275]    [Pg.129]    [Pg.61]    [Pg.379]    [Pg.229]    [Pg.230]    [Pg.106]    [Pg.199]    [Pg.203]    [Pg.627]    [Pg.405]    [Pg.435]    [Pg.160]    [Pg.119]    [Pg.604]    [Pg.166]    [Pg.237]    [Pg.134]    [Pg.124]    [Pg.59]    [Pg.596]    [Pg.69]    [Pg.73]    [Pg.74]    [Pg.100]    [Pg.186]    [Pg.90]    [Pg.120]    [Pg.528]    [Pg.14]   
See also in sourсe #XX -- [ Pg.152 ]




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Surface dependence

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