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Point and Surface Tension

Similar considerations apply to the surface tension of solids. Although surface tension between solids and gases has never been accurately measured, there can be no doubt of its [Pg.376]


When different chemical and biochemical materials are introduced into water, there is a rise in the boiling point and viscosity and a decrease in the freezing point and surface tension. Solubility increases with increasing temperature as the heat introduced reduces water-water hydrogen bond attractions and facilitates solute hydration. [Pg.6]

A setting of 380 K is generally high enough for aqueous solutions in tube wall atomization, whereas about 520 to 570 K is needed in probe atomization. The time necessary varies according to the sample size. As an empirical rule, a time in seconds up to 2 times the sample size in fx should be used. Thus, 20 /Jil of aqueous sample in tube wall atomization needs 30 to 40 s at 380 K to dry. With solvents other than water, the drying temperature and time necessary will obviously be different due to the different boiling points and surface tension. [Pg.88]

Water has an unusually high normal boiling point and surface tension. Additionally it expands on freezing. [Pg.555]

Relationships between molecular polarizabilities and the densities, boiling points, and surface tensions of M(C2H5)4 compounds (M = C to Pb) have been discussed [12]. [Pg.56]

MAH Mahajan, S., Shaheen, A., Banipal, T.S., and Mahajan, R.K., Cloud point and surface tension studies of triblock copolymer-ionic surfactant mixed systems in the presence of amino adds or dipeptides and electrolytes, J. Chem. Eng. Data, 55, 3995,2010. [Pg.559]

Katti, P. K. Chaudhri, M. M. Boiling points and surface tensions of mixtures of benzyl acetate wifli dioxane, aniline, and meta-cresol. J. Chem. Eng. Data 1964, 9, 128-130. [Pg.1468]

When a surface of a liquid is expanded, more molecules are brought from the interior of the liquid to the surface. The quantity of work required to bring more molecules to the surface depends on the sfrength of the attractive forces between the molecules and, consequently, on the energy of cohesion. Hence, a correlation, albeit with many exceptions, exists between the boiling point and surface tension [3]. [Pg.104]

Chitosan TFA-DCM Effect of various solvents with the co-system of TFA-DCM most adequate due to low boiling point and surface tension. Antimicrobial test. [157]... [Pg.713]

Surface waves at an interface between two innniscible fluids involve effects due to gravity (g) and surface tension (a) forces. (In this section, o denotes surface tension and a denotes the stress tensor. The two should not be coiifiised with one another.) In a hydrodynamic approach, the interface is treated as a sharp boundary and the two bulk phases as incompressible. The Navier-Stokes equations for the two bulk phases (balance of macroscopic forces is the mgredient) along with the boundary condition at the interface (surface tension o enters here) are solved for possible hamionic oscillations of the interface of the fomi, exp [-(iu + s)t + i V-.r], where m is the frequency, is the damping coefficient, s tlie 2-d wavevector of the periodic oscillation and. ra 2-d vector parallel to the surface. For a liquid-vapour interface which we consider, away from the critical point, the vapour density is negligible compared to the liquid density and one obtains the hydrodynamic dispersion relation for surface waves + s>tf. The temi gq in the dispersion relation arises from... [Pg.725]

Revised material in Section 5 includes an extensive tabulation of binary and ternary azeotropes comprising approximately 850 entries. Over 975 compounds have values listed for viscosity, dielectric constant, dipole moment, and surface tension. Whenever possible, data for viscosity and dielectric constant are provided at two temperatures to permit interpolation for intermediate temperatures and also to permit limited extrapolation of the data. The dipole moments are often listed for different physical states. Values for surface tension can be calculated over a range of temperatures from two constants that can be fitted into a linear equation. Also extensively revised and expanded are the properties of combustible mixtures in air. A table of triple points has been added. [Pg.1287]

Properties. The physical properties of aHphatic fluorine compounds containing chlorine are similar to those of the PECs or HECs (3,5). They usually have high densities and low boiling points, viscosities, and surface tensions. The irregularity in the boiling points of the fluorinated methanes, however, does not appear in the chlorofluorocarbons. Their boiling points consistently increase with the number of chlorines present. The properties of some CECs and HCECs are shown in Tables 3 and 4. [Pg.284]

There are three types of Hquid content in a packed bed (/) in a submerged bed, there is Hquid filling the larger channels, pores, and interstitial spaces (2) in a drained bed, there is Hquid held by capillary action and surface tension at points of particle contact, or near-contact, as weU as a zone saturated with Hquid corresponding to a capillary height in the bed at the Hquid discharge face of the cake and (3) essentially undrainable Hquid exists within the body of each particle or in fine, deep pores without free access to the surface except perhaps by diffusion or compaction. [Pg.399]

Liquid Metal Sources. The source feed is a metal of low melting point - Ga and In are commonly employed. It is introduced as a liquid film flowing over a needle towards the tip whose radius is relatively blunt (10 pm). The electrostatic and surface tension forces form the liquid into a sharp point known as the Taylor cone. Here the high electric field is sufficient to allow an electron to tunnel from the atom to the surface, leaving the atom ionized. [Pg.74]

Heretofore, ionic liquids incorporating the 1,3-dialkylimidazolium cation have been preferred as they interact weakly with the anions and are more thermally stable than the quaternary ammonium cations. Recently, the physical properties of 1,2,3,4-tetraalkylimidazolium- and 1,3-dialkylimidazolium-containing ionic liquids in combination with various hydrophobic and hydrophilic anions have been systematically investigated (36,41). The melting point, thermal stability, density, viscosity, and other physical properties have been correlated with alkyl chain length of the imidazolium cation and the nature of the anion. The anion mainly determines water miscibility and has the most dramatic effect on the properties. An increase in the alkyl chain length of the cations from butyl to octyl, for example, increases the hydrophobicity and viscosity of the ionic liquid, whereas densities and surface tension values decrease, as expected. [Pg.161]

A return to a more rational expression of the relation between drop weight and surface tension has been made by Iredale Phil. Mag. XLV. 1088, 1923). This expression rests upon the fact that different liquids may form drops of similar shape from tubes of different diameters. From this and from the assumption that rupture occurs at the point of maximum concavity the equation... [Pg.14]

Mixed surfactant systems are of importance from a fundamental and practical point of view. Therefore, many recent papers have reported on the micellar properties of mixed surfactant solutions. For example, Tokiwa et al. have measured the NMF spectra W Ingram has measured surface tension ( 5). Previously, we have reported the solution properties of anionic-nonlonlc surfactant mixed systems from the point of view of electrical (., 7) and surface tension measurements (8-10), and investigated the mixed micelle formation. [Pg.68]

Figure 1. Mixed cmc s and surface tensions at the cmc for mixtures of C qPO and SDS in 1 mM Na2C0T (at 24°C). The plotted points are experimental results, the solid lines the prediction of the nonideal model for 8 = -3 7 and 8 = -3.5 respectively, and the dashed lines the prediction for ideal mixing in the pseudo-phase. Figure 1. Mixed cmc s and surface tensions at the cmc for mixtures of C qPO and SDS in 1 mM Na2C0T (at 24°C). The plotted points are experimental results, the solid lines the prediction of the nonideal model for 8 = -3 7 and 8 = -3.5 respectively, and the dashed lines the prediction for ideal mixing in the pseudo-phase.
The conditions for synergism in surface tension reduction efficiency, mixed micelle formation, and Surface tension reduction effectiveness in aqueous solution have been derived mathematically together with the properties of the surfactant mixture at the point of maximum synergism. This treatment has been extended to liquid-liquid (aqueous solution/hydrocarbon) systems at low surfactant concentrations.) The effect of chemical structure and molecular environment on the value of B is demonstrated and discussed. [Pg.144]

Joyce (29) developed the wax method of spray-particle-size measurement to a high degree of perfection during 1942 to 1946. His technique is based upon the observation that paraffin wax, when heated to a suitable temperature level above its melting point, corresponds closely, in the significant characteristics of viscosity and surface tension, with jet fuel. [Pg.158]


See other pages where Point and Surface Tension is mentioned: [Pg.165]    [Pg.476]    [Pg.376]    [Pg.377]    [Pg.338]    [Pg.165]    [Pg.476]    [Pg.376]    [Pg.377]    [Pg.338]    [Pg.51]    [Pg.296]    [Pg.491]    [Pg.1899]    [Pg.35]    [Pg.35]    [Pg.521]    [Pg.599]    [Pg.61]    [Pg.74]    [Pg.385]    [Pg.55]    [Pg.22]    [Pg.32]    [Pg.48]    [Pg.199]    [Pg.62]    [Pg.491]    [Pg.95]    [Pg.296]   


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