Some aspects of the application of VNKh-L-408 inhibitor in an electrostatic field (the kinetics of its evaporation from the surfaces of various metals, the causes of its higher efficiency upon electrostatic application, and the mechanism of its action) are discussed. A technology for electrostatic application of powdered inhibitor to metal surfaces has been developed.
Key words: electrostatic field, kinetics of evaporation, application technology.Received May 24, 2013May 24, . doi: 10.17675/2305May 24, -6894-2013 The method of electrostatic deposition of inhibitors to a metal surface or electrostatic spraying of inhibitors in an enclosure around a metal article to be protected is new [1,2] and unparalleled, so we will discuss it here in more detail. Although this method has been introduced into commercial use, its mechanism is not understood in full; some physicochemical aspects of the process also remain unclear. It is known that if it is possible to seal the space to be protected at least partially is a direct indication that a volatile inhibitor of atmospheric corrosion (VIAC) should be used. Depending on the operating or storage conditions for a metal article, the VIAC vapors propagate within the space by diffusion or by transfer with a gas flow. However, the use of many inhibitors is limited by their low volatility. The electrostatic method allows one to circumvent this problem and use VIACs with low vapor pressures when a metal article is only partially sealed or even not sealed at all.Application of an inhibitor at a concentration of ~10 g/m 2 to a metal surface in an electrostatic field (which corresponds to ~60 g/m 3 of the air volume) ensures higher protection in comparison to its granulated forms (granlin, lingal, and tablin) at the same concentration, or to its application as powder in sachets suspended inside a metal article (the most laborious method) (see Table 2 in [3]). The high efficiency of this method was confirmed by field test data (Table 1).The method essentially involves electrostatic deposition of a VIAC onto a metal surface until a charge density that is optimum for the inhibitor is reached, followed by treatment of the surface with an ionized gas flow produced by corona discharge. This results in a uniform distribution of the inhibitor over the surface (or throughout the space)