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Shielding surface

Deposits cause corrosion both directly and indirectly. If deposits contain corrosive substances, attack is direct interaction with the aggressive deposit causes wastage. Shielding of surfaces below deposits produces indirect attack corrosion occurs as a consequence of surface shielding provided by the deposit. Both direct and indirect attack may involve concentration cell corrosion, but indirect attack almost always involves this form of corrosion. [Pg.67]

Slime is a network of secreted strands (extracellular polymers) intermixed with bacteria, water, gases, and extraneous matter. Slime layers occlude surfaces—the biological mat tends to form on and stick to surfaces. Surface shielding is further accelerated by the gathering of dirt, silt, sand, and other materials into the layer. Slime layers produce a stagnant zone next to surfaces that retards convective oxygen transport and increases diffusion distances. These properties naturally promote oxygen concentration cell formation. [Pg.124]

The primary difference between these types of metal wastage and oxygen corrosion is that these are all indirect forms of attack, induced by surface shielding (areas of metal surface under deposits or foulants, or cracks and gaps in the metal that are close to a shielding surface). [Pg.246]

All the various forms of concentration cell corrosion described are types of indirect attack induced by the effects of surface shielding, although not all concentration cell corrosion mechanisms involve the presence of oxygen. [Pg.248]

Several of these problems can be solved by polyplex modification with polyethylene glycol (PEG). PEGylation has been broadly explored for surface shielding ( stealthing ) of many liposomal and nanoparticulate carriers. In the case of cationic polymers, Plank et al. [62] demonstrated that complement activation can be reduced when the polymers are PEGylated. Such a modification can be... [Pg.4]

Polyplex surface shielding solves several crucial problems, but may also create new problems. Shielding can strongly reduce the efficiency of subsequent cellular steps of the delivery process [68, 69], and also can negatively alter other polyplex characteristics. For pDNA/PEI polyplexes with optimum medium size of PEI, PEG was found to reduce the polyplex stability in vivo [64, 65, 81]. For a discussion of these aspects see Sect. 3.1. [Pg.5]

The following sections discuss how polymers and polyplexes can be chemically designed to be bioresponsive in three key delivery functions (1) polyplex surface shielding, (2) interaction with lipid bilayers, and (3) polyplex stability. [Pg.10]

Kircheis, R., Blessing, T., Brunner, S., Wightman, L., Wagner, E. (2001). Tumor targeting with surface-shielded ligand-polycation DNA complexes. J. Control Release, 72, 165-170. [Pg.370]

A uniphase, buried-channel charge transfer device is disclosed in US-A-4229752 wherein a portion of each cell includes an inversion layer, or "virtual electrode" at the semiconductor surface, shielding that region from any gate-induced change in potential. [Pg.3]

While the theoretical treatment appears simpler than that of the feedback amperometric mode, in practice quantitative agreement between theoretical and experimental concentration profiles is more difficult because the tip travels through the diffusion layer due to the substrate activity. Thus, the tip introduces convection within the substrate diffusion layer while shielding the substrate from the bulk. In the amperometric mode diffusion is restricted to the tip-substrate gap and thus shielding and convection are not a problem. On the whole, the fit between experimental and theoretical concentration profiles works well when the tip is at least one tip radius away from the surface. Shielding dominates at closer tip-substrate distances where the tip significantly affects the concentration profile and the fit is very poor. [Pg.430]

Surface Shield. pCymaX] Mold sealers and release agents. [Pg.360]

Assumed Ne/ °Ne too high, see text Lunar surface, shielding depth 500 g/cm ... [Pg.769]

The addition of Ca-ions affects the behavior of C-1 gelatin more than P-1, shifting the adsorption maxima of both gelatins to the acid side. The surface areas occupied per molecule at the I.E.P are twice as large with as without Ca-ions. Since the Ar s stay about the same, Ca-ions attached to the gelatin reduce coil contraction or interpenetration. Surface shielding by adsorbed... [Pg.275]

In principle, cathodic protection can be applied to a bare metal however, the external current demand for snch protection is usually very large and uneconomical. Protection of metals from corrosion may also be achieved by coating the surface. The coating thus applied to the metal surface shields it from the corrosive environment. However, flaws are inherent in coatings, which increase both in size and number with the service life of the coated structure. [Pg.434]

Method numbers 2 and 3 are based on the assumption that the metal/liquid interphase and thus the polarization impedance is invariable. This is not always the case. Measuring on dry samples for instance implies poor control of the contact electrolyte. Also a sample may contain local regions of reduced conductivity near the electrode surface. The currents are then canalized with uneven current density at the metal surface (shielding effect). Electrode polarization impedance, in particular at low frequencies, is then dependent on the degree of shielding. An example of method 4 is Krizaj and Pecar (2012), who described such a method for removing the contribution from electrode polarization impedance on measured impedance data of a suspension of microcapsules. [Pg.241]

Surface veils are lightweight thin surfacing materials usually constructed from swirl mats either in glass or from a synthetic fibre. Their main use is to act as a decorative surface, shielding from view the texture of the underlying structural reinforcement. But they also may be used in conjunction with gel coats for added support. C-glass surface veils are... [Pg.309]

This silicate morphology may act as an cfBcient barrier to oxygen diffusion towards the bulk of the polymer. Surface polymer molecules trapped within the silicate are thus brought to a close contact with oxygen to produce the thermally and oxidative stable charred material providing a new char-layered silicate nanocomposite acting as an effective surface shield... [Pg.41]

PAMAM G4 labeled by ferrocenyl groups was also immobilized on the surface of a gold electrode covered by a monolayer of DTSP [26] or MUA activated by EDAC and pentafluorophenol [27]. This PAMAM G4 ferrocene conjugate mono-layer was biotinylated. The bioelectrocatalytic oxidation of glucose by GOx appeared to be inhibited by addition of avidin or by a monoclonal antibiotin antibody because of surface shielding (Fig. 6.5). [Pg.189]

Giant liposomes with 5 mol % of (PEG-DSPE) were used to test whether the fusion pulse width thresholds were shifted by the surface shielding polymers. Figure 16.6 shows the fusion threshold of liposomes with added PEG-DSPE. The surface shielding offered by the PEG moiety increases the energy barrier for electrofusion. As a result, the pulse widths required to fuse these surface-modified giant liposomes... [Pg.238]

The permeability of a system represents the amount of gas passing through a material specimen with cross-sectional area A and thickness d in a specific unit of time t. The process involves two basic mechanisms, namely, thermodynamic solubility of the permeant in the surface of the films and kinetic diffusion of the permeating molecules across the film to the other surface (Shields, 2008 Gonzo et al., 2006 Robeson, 2003 Kamal and Jinnah, 1984). Thus, permeability can be expressed as a product of solubility constant S and diffusion coefficient D, P = S x D. [Pg.172]


See other pages where Shielding surface is mentioned: [Pg.297]    [Pg.264]    [Pg.818]    [Pg.958]    [Pg.189]    [Pg.309]    [Pg.6]    [Pg.11]    [Pg.12]    [Pg.701]    [Pg.232]    [Pg.74]    [Pg.264]    [Pg.225]    [Pg.245]    [Pg.98]    [Pg.165]    [Pg.292]    [Pg.1026]    [Pg.623]    [Pg.851]    [Pg.242]    [Pg.102]    [Pg.125]    [Pg.159]   
See also in sourсe #XX -- [ Pg.124 ]

See also in sourсe #XX -- [ Pg.97 ]




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Anisotropic shielding surfaces

Intermolecular shielding surfaces

Iso-chemical shielding surfaces

Nuclear shielding surfaces

Shielding Surfaces and Rovibrational Averaging

Shielding hyper-surfaces

Shielding surface rovibrational averaging

Shielding surface temperature dependence

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