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Resistance water phase

The fluid is formulated from a premium mineral od-base stock that is blended with the required additive to provide antiwear, mst and corrosion resistance, oxidation stabdity, and resistance to bacteria or fungus. The formulated base stock is then emulsified with ca 40% water by volume to the desired viscosity. Unlike od-in-water emulsions the viscosity of this type of fluid is dependent on both the water content, the viscosity of the od, and the type of emulsifier utilized. If the water content of the invert emulsion decreases as a result of evaporation, the viscosity decreases likewise, an increase in water content causes an increase in the apparent viscosity of the invert emulsion at water contents near 50% by volume the fluid may become a viscous gel. A hydrauHc system using a water-in-od emulsion should be kept above the freezing point of water if the water phase does not contain an antifreeze. Even if freezing does not occur at low temperatures, the emulsion may thicken, or break apart with subsequent dysfunction of the hydrauHc system. [Pg.263]

Equation (4.20) expresses that the total resistance to mass transfer across the air-water boundary is equal to the sum of the resistances across the liquid film and the gas film. The importance of the magnitude of Henry s constant is, in this respect, evident. For high values of HA, e.g., exemplified by 02, the resistance mainly exists in the water film, and turbulence in a sewer will, therefore, enhance the water-air transfer process. The importance of turbulence in the water phase is reduced for odorous components with a relatively low HA value, and turbulence in the air phase will correspondingly increase the release rate (Table 4.1). As seen from Equations (4.20) and (4.21), these facts also depend on the k1A/k2A ratio that varies according to system characteristics. [Pg.76]

To transfer ozone to a water phase very often fine bubble columns or stirred or agitated tank reactors are applied. The bubbles in these reactors are small. The value of m for ozone is relatively high. Furthermore the diffusion coefficient of ozone in the gas phase is very high compared with the diffusion coefficient of ozone in the water phase. These three reasons lead to the conclusion that in bubble columns and stirred tank reactors the resistance to mass transfer in the gas phase can be neglected. Equation (20) can than be simplified to ... [Pg.267]

The air phase resistance is estimated to be 27 times the water phase resistance in equation (E8.5.3). Thus, the results that we get assuming the water phase resistance to be zero are close to those that we would get assuming that they will be 1/27 the total resistance. This indicates that toxaphene is a gas-phase (nonvolatile) controlled compound, as long as Kq/Kl is equal to 150. A diagram of the assumed concentration profiles is given in Figure E8.5.2. [Pg.210]

The viscosity of the external or oil phase plays a dual role. In an oil having a high viscosity (a high resistance to flow), a given amount of agitation will not break up the water phase Into droplets as numerous or fine as would be the case with a lower-viscosity oil. [Pg.134]

An important performance characteristic of passive samplers that operate in the TWA regime is the diffusion barrier that is inserted between the sampled medium and the sorption phase. This barrier is intended to control the rate of mass transfer of analyte molecules to the sorption phase. It is also used to define the selectivity of the sampler and prevent certain classes (e.g., polar or nonpolar compounds) of analytes, molecular sizes, or species from being sequestered. The resistance to mass transfer in a passive sampler is, however, seldom caused by a single barrier (e.g., a polymeric membrane), but equals the sum of the resistances posed by the individual media (e.g., aqueous boundary layer, biofilm, and membrane) through which analyte diffuses from the bulk water phase to the sorption phase.19 The individual resistances are equal to the reciprocal value of their respective mass transfer coefficients and are additive. They are directly proportional to the thickness of the barrier... [Pg.45]

The value of KA may depend primarily on kA or on k%, depending on whether m is very large or very small. For example, if acetic acid (C) is being extracted from x -hexane (A) by water (B), the distribution ratio m is very large and from Eq. (9) we see that KA kA. In this case the extraction rate is controlled by the -hexane phase resistance. Conversely, if the solute (e.g., benzoic acid) is much less soluble in the water than in the n-hexane, then Ka = kw/tri and the extraction rate is controlled by water phase resistance. [Pg.485]

This effect of physically shielding unstable perfume components from contact with the water phase may perhaps be provided also by the stable components of the perfume compound itself, provided that the latter are present in sufficient excess. This would account for Paul Jellinek s observation (1954, p. 116) that "the presence of a soap-resistant aromatic delays the decomposition of compounds which are unstable to alkali, and may prevent it altogether," and for the common observation that unstable but powerful perfumery materials such as methyl heptine and octine carbonates which are normally used at very low levels exhibit better stability in practice than tests of their stability in pure form would have indicated. [Pg.169]

Emulsion Capacity and Stability. A 0.5 g sample of the freeze-dried protein fraction was redissolved in a minimum of 0.3 M citrate-phosphate buffer at pH 7.0 and mixed thoroughly with 50 ml of 1 M NaCl for 1 min in a Sorvall Omnimixer at 1000 rpm in a one pint Mason jar set in a water bath (20°C). Crisco oil (50 ml) was added to the jar and an emulsion formed by mixing at 500 rpm with simultaneous addition of oil at the rate of 1 ml/min until the emulsion broke. The endpoint was determined by monitoring electrical resistance with an ohmeter. As the emulsion broke a sharp increase (l KS2 to 35- 0 KSi) was noted. Emulsion capacity was expressed as the total volume of oil required to reach the inversion point per mg protein. This method is similar to that used by Carpenter and Saffle (8) for sausage emulsions. To establish emulsion stability the same procedure was used except that 100 ml of oil was added and a stable emulsion formed by blending at 1000 rpm for 1 min. A 100 ml aliquot was transferred to a graduate cylinder and allowed to stand at room temperature. Observations were made of the volume of the oil, emulsion and water phases at 30, 60, 90 and 180 min. [Pg.151]

The primary variable that determines whether the controlling resistance is in the liquid or gas film is the H or Henry constant. As shown in Figure 5.15, and as is apparent from equation 39, for small values of H the water phase film controls the transfer, and for high values of H the transfer is controlled by the air phase film. Gas transfer conditions that are liquid film controlled sometimes are expressed in terms of thickness, Zw, of the water film. As indicated by equation 38, this can be done from a measured value of (or K,o,) and the diffusion coefficient of the substance Zw decreases with the extent of turbulence (current velocity, wind speed, etc.). Typical values for are in the range of micrometers for seawater, a few hundred micrometers in lakes and up to 1 nun in small wind-sheltered water bodies (Brezonik, 1994). [Pg.243]

If the emulsion polymerization product is retained in the water phase for use it is referred to as a PTEE dispersion. The very strong C-E bonds, plus the strengthening effect of these on the C-C bonds confers extraordinarily stable properties to this polymer. The chemical inertness, excellent electrical resistance, high-heat resistance, nonstick properties, and low coefficient of friction combine to make PTFE one of the highest performance commercial vinyl plastics produced (Table 23.3). [Pg.749]

The ability of an oil to remain liquid during refrigerator storage is determined by the cold test analysis crystallization resistance is measured as the time in hours before the oil appears cloudy at 32°F (CPC). Standardized AOCS Method Cc 11-53 requires that dry filtered oil be placed in a sealed 4-ounce bottle and submerged in an ice bath. A go-no-go examination for clarity after 5 hours is stipulated by the Official AOCS Method however, most laboratories practice the alternative procedure which continues the clarity examination until a cloud appears. The cold test procedure was developed to evaluate cottonseed oil for the production of mayonnaise and salad dressings. Oil that solidifies at refrigerator temperatures will cause an emulsion-break with a resultant separation of the oil and water phases. Currently, the cold test is also utilized to ensure that bottled oils for retail sale will not develop an unattractive appearance on the grocery shelf. [Pg.209]

Zi) Assuming that the water-air interface is at the same temperature as the bulk of the water (water-phase resistance to heat transfer negligible), calculate the driving force at the top and at the bottom of the tower. Using an average — Jf,... [Pg.765]

The coefficients for the water phase, k , the organic phase, /c , and the membrane, o/z, are generally about the same magnitude, but if the distribution coefficient m is large, most of the resistance is in the water phase. Here m is the ratio of the solute concentration in the organic phase to that in the water phase. [Pg.863]

If the distribution coefficient for the solute strongly favors the water phase m 1), the organic phase has the controlling resistance, and a hydrophilic membrane might be selected to make the membrane resistance smaller. [Pg.864]

The ice/water interface will advance into the bulk water phase but as the thickness of the ice layer increases with the associated increase in thermal resistance, the rate of heat removal will fall. In turn this vnll represent an exponentially decreasing rate of growth of the ice layer. [Pg.138]

Fig. 3. Schematic of the surface renewal model of gas exchange (shown, water side resistance dominant). In this model, gas diffuses across the air-water interface and establishes a gradient. Tm-bulence eddies periodically mix the gradient into the bulk water phase. Solid lines show gas concentration with distance from the interface and correspond to times, to to which represent increasing times between renewal events. The concentration of dissolved gas is C, and subscripts a and w refer to air (at equilibrium) and water, respectively. Note that the shorter the sm face renewal time, the higher the gas transfer, because transfer Orem s on average along a stronger gradient... Fig. 3. Schematic of the surface renewal model of gas exchange (shown, water side resistance dominant). In this model, gas diffuses across the air-water interface and establishes a gradient. Tm-bulence eddies periodically mix the gradient into the bulk water phase. Solid lines show gas concentration with distance from the interface and correspond to times, to to which represent increasing times between renewal events. The concentration of dissolved gas is C, and subscripts a and w refer to air (at equilibrium) and water, respectively. Note that the shorter the sm face renewal time, the higher the gas transfer, because transfer Orem s on average along a stronger gradient...

See other pages where Resistance water phase is mentioned: [Pg.879]    [Pg.152]    [Pg.53]    [Pg.217]    [Pg.223]    [Pg.247]    [Pg.153]    [Pg.173]    [Pg.108]    [Pg.291]    [Pg.375]    [Pg.102]    [Pg.331]    [Pg.539]    [Pg.379]    [Pg.53]    [Pg.825]    [Pg.328]    [Pg.210]    [Pg.78]    [Pg.153]    [Pg.402]    [Pg.132]    [Pg.538]    [Pg.879]    [Pg.216]    [Pg.864]    [Pg.870]    [Pg.329]    [Pg.233]    [Pg.35]    [Pg.91]    [Pg.242]   
See also in sourсe #XX -- [ Pg.210 ]




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