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Elastic Properties of Natural Sea Surface Films Incorporated with Solid Dust Particles: Model Baltic Sea Studies

DOI: 10.1155/2012/638240

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Abstract:

Floating dust-originated solid particles at air-water interfaces will interact with one another and disturb the smoothness of such a composite surface affecting its dilational elasticity. To quantify the effect, surface pressure ( ) versus film area ( ) isotherm, and stress-relaxation ( -time) measurements were performed for monoparticulate layers of the model hydrophobic material (of μm-diameter and differentiated hydrophobicity corresponding to the water contact angles (CA) ranging from 60 to 140°) deposited at surfaces of surfactant-containing original seawater and were studied with a Langmuir trough system. The composite surface dilational modulus predicted from the theoretical approach, in which natural dust load signatures (particle number flux, daily deposition rate, and diameter spectra) originated from in situ field studies performed along Baltic Sea near-shore line stations, agreed well with the direct experimentally derived data. The presence of seawater surfactants affected wettability of the solid material which was evaluated with different CA techniques applicable to powdered samples. Surface energetics of the particle-subphase interactions was expressed in terms of the particle removal energy, contact cross-sectional areas, collapse energies, and so forth. The hydrophobic particles incorporation at a sea surface film structure increased the elasticity modulus by a factor (1.29–1.58). The particle-covered seawater revealed a viscoelastic behavior with the characteristic relaxation times ranging from 2.6 to 68.5?sec. 1. Introduction The atmospheric transport and deposition of mineral particles strongly influence the physics and chemistry of the marine atmosphere, and the biogeochemical cycles in seawater. So far, our emphasis has been closed on the multicomponent character of natural surfactant films, and the consequent complexities involved in any attempt to predict the interfacial viscoelastic properties playing a crucial role in modeling of physical systems with surface film-mediated interfaces. A variation in the surface rheological parameters of the natural surfactant seawater films has been conceived as a different in source of surfactant materials and in physical dynamics reflecting organic matter migration, degradation, and spatial-temporal dynamics in natural waters [1]. In nearly all cases, uniform, homogeneous surfaces have been studied. However, in “real” systems, in technology, biology, and oceanography, surfaces are very often non-uniform. For instance, a flat surface containing a surfactant monolayer which has undergone a

References

[1]  Z. A. Mazurek, J. S. Pogorzelski, and K. Boniewicz-Szmyt, “Evolution of natural sea surface film structure as a tool for organic matter dynamics tracing,” Journal of Marine Systems, vol. 74, pp. S52–S64, 2008.
[2]  S. J. Pogorzelski and A. D. Kogut, “Structural and thermodynamic signatures of marine microlayer surfactant films,” Journal of Sea Research, vol. 49, no. 4, pp. 347–356, 2003.
[3]  J. Lucassen, “Dynamic dilational properties of composite surfaces,” Colloids and Surfaces, vol. 65, no. 2-3, pp. 139–149, 1992.
[4]  Z. Hórv?lgyi, M. Máté, A. Dániel, and J. Szalma, “Wetting behaviour of silanized glass microspheres at water-air interfaces: a Wilhelmy film balance study,” Colloids and Surfaces A, vol. 156, no. 1–3, pp. 501–507, 1999.
[5]  A. W. Adamson and A. Gast, Physical Chemistry of Surfaces, John Wiley & Sons, New York, NY, USA, 2nd edition, 1997.
[6]  E. Kim, D. Kalman, and T. Larson, “Dry deposition of large, airborne particles onto a surrogate surface,” Atmospheric Environment, vol. 34, no. 15, pp. 2387–2397, 2000.
[7]  Z. G. Cui, B. P. Binks, and J. H. Clint, “Determination of contact angles on microporous particles using the thin-layer wicking technique,” Langmuir, vol. 21, no. 18, pp. 8319–8325, 2005.
[8]  A. W. Adamson, Physical Chemistry of Surfaces, John Wiley & Sons, New York, NY, USA, 8th edition, 1982.
[9]  T. Kato, K. Iriyama, and T. Araki, “The time of observation of π-A isotherms III. Studies on the morphology of arachidic acid monolayers, observed by transmission electron microscopy of replica samples of one-layer Langmuir-Blodgett films using plasma-polymerization,” Thin Solid Films, vol. 210-211, no. 1, pp. 79–81, 1992.
[10]  F. Ravera, M. Ferrari, E. Santini, and L. Liggieri, “Influence of surface processes on the dilational visco-elasticity of surfactant solutions,” Advances in Colloid and Interface Science, vol. 117, no. 1–3, pp. 75–100, 2005.
[11]  J. van Hunsel and P. Joos, “Study of the dynamic interfacial tension at the oil/water interface,” Colloid & Polymer Science, vol. 267, no. 11, pp. 1026–1035, 1989.
[12]  M. R. Rodríguez Ni?o, P. J. Wilde, D. C. Clark, and J. M. Rodríguez Patino, “Surface dilational properties of protein and lipid films at the air-water interface,” Langmuir, vol. 14, no. 8, pp. 2160–2166, 1998.
[13]  Y. Jayalakshmi, L. Ozanne, and D. Langevin, “Viscoelasticity of Surfactant Monolayers,” Journal of Colloid And Interface Science, vol. 170, no. 2, pp. 358–366, 1995.
[14]  J. H. Clint and S. E. Taylor, “Particle size and interparticle forces of overbased detergents: a Langmuir trough study,” Colloids and Surfaces, vol. 65, no. 1, pp. 61–67, 1992.
[15]  M. Máté, J. H. Fendler, J. J. Ramsden, J. Szalma, and Z. Hórv?lgyi, “Eliminating surface pressure gradient effects in contact angle determination of nano- and microparticles using a film balance,” Langmuir, vol. 14, no. 22, pp. 6501–6504, 1998.
[16]  B. S. Murray, “Equilibrium and dynamic surface pressure-area measurements on protein films at air-water and oil-water interfaces,” Colloids and Surfaces A, vol. 125, no. 1, pp. 73–83, 1997.
[17]  M. A. Rodríguez-Valverde, M. A. Cabrerizo-Vílchez, P. Rosales-López, A. Páez-Dueas, and R. Hidalgo-álvarez, “Contact angle measurements on two (wood and stone) non-ideal surfaces,” Colloids and Surfaces A, vol. 206, no. 1–3, pp. 485–495, 2002.
[18]  C. J. van Oss, R. F. Giese, Z. Li et al., “Determination of contact angles and pore sizes of porous media by column and thin layer wicking,” Journal of Adhesion Science and Technology, vol. 6, pp. 413–428, 1992.
[19]  W. Wu, R. F. Giese, and C. J. Van Oss, “Change in surface properties of solids caused by grinding,” Powder Technology, vol. 89, no. 2, pp. 129–132, 1996.
[20]  G. Tolnai, A. Agod, M. Kabai-Faix, A. L. Kovács, J. J. Ramsden, and Z. Hórv?lgyi, “Evidence for secondary minimum flocculation of St?ber silica nanoparticles at the air-water interface: film balance investigations and computer simulations,” Journal of Physical Chemistry B, vol. 107, no. 40, pp. 11109–11116, 2003.
[21]  A. Ulman, An Introduction to Ultrathin Organic Films, Academic Press, Boston, Mass, USA, 1991.
[22]  S. Yariv, “Wettability of clay minerals,” in Modern Approaches to Wettability: Theory and Applications, M. E. Schrader and G. Loeb, Eds., pp. 279–326, Plenum Press, New York, NY, USA, 1992.
[23]  S. Caquineau, A. Gaudichet, L. Gomes, M. C. Magonthier, and B. Chatenet, “Saharan dust: clay ratio as a relevant tracer to assess the origin of soil-derived aerosols,” Geophysical Research Letters, vol. 25, no. 7, pp. 983–986, 1998.
[24]  A. Avila, I. Queralt-Mitjans, and M. Alarcón, “Mineralogical composition of African dust delivered by red rains over northeastern Spain,” Journal of Geophysical Research D, vol. 102, no. 18, pp. 21977–21996, 1997.
[25]  J. Keller and R. Lamprecht, “Road dust as an indicator for air pollution transport and deposition: an application of SPOT imagery,” Remote Sensing of Environment, vol. 54, no. 1, pp. 1–12, 1995.
[26]  H. W. Vallack and D. E. Shillito, “Suggested guidelines for deposited ambient dust,” Atmospheric Environment, vol. 32, no. 16, pp. 2737–2744, 1998.
[27]  B. Forster, X. Baide, and S. Xingwai, “Modelling suspended particle distribution in near coastal waters using satellite remotely-sensed data,” International Journal of Remote Sensing, vol. 15, no. 6, pp. 1207–1219, 1994.
[28]  P. Gentien, M. Lunven, M. Leha?tre, and J. L. Duvent, “In-situ depth profiling of particle sizes,” Deep-Sea Research I, vol. 42, no. 8, pp. 1297–1312, 1995.
[29]  S. Chen and D. Eisma, “Fractal geometry of in situ flocs in the estuarine and coastal environments,” Netherlands Journal of Sea Research, vol. 32, no. 2, pp. 173–182, 1995.
[30]  D. J. Law, A. J. Bale, and S. E. Jones, “Adaptation of focused beam reflectance measurement to in-situ particle sizing in estuaries and coastal waters,” Marine Geology, vol. 140, no. 1-2, pp. 47–59, 1997.
[31]  R. Arimoto, B. J. Ray, N. F. Lewis, U. Tomza, and R. A. Duce, “Mass-particle size distributions of atmospheric dust and the dry deposition of dust to the remote ocean,” Journal of Geophysical Research D, vol. 102, no. 13, pp. 15867–15874, 1997.
[32]  S. A. Slinn and W. G. N. Slinn, “Predictions for particle deposition on natural waters,” Atmospheric Environment A, vol. 14, no. 9, pp. 1013–1016, 1980.
[33]  H. Sievering, “Small-particle dry deposition on natural waters: how large the uncertainty?” Atmospheric Environment, vol. 18, no. 10, pp. 2271–2272, 1984.
[34]  W. Alpers and H. Huhnerfuss, “The damping of ocean waves by surface films: a new look at an old problem,” Journal of Geophysical Research, vol. 94, pp. 6251–6265, 1989.
[35]  G. Franceschetti, A. Iodice, D. Riccio, G. Ruello, and R. Siviero, “SAR raw signal simulation of oil slicks in ocean environments,” IEEE Transactions on Geoscience and Remote Sensing, vol. 40, no. 9, pp. 1935–1949, 2002.

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