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Suraj Chandra Sharma

Publications and source records attributed to Suraj Chandra Sharma.

3 recordsLinked to original sources

Viscoelastic micellar solutions in nonionic fluorinated surfactant systems.

The formation and rheological behavior of a viscoelastic wormlike micellar solution in an aqueous solution of a nonionic fluorinated surfactant, perfluoroalkyl sulfonamide ethoxylate, of structure C8F17SO2N(C3H7)(CH2CH2O)10H was studied. Temperature-induced viscosity growth is observed even at low-surfactant concentration (approximately 1 wt %), and viscosity reaches the maximum at a temperature T(eta)-max. Upon successive increases in the temperature, the viscosity decreases, and ultimately a phase separation occurs. Small-angle X-ray scattering (SAXS) measurements confirm the presence of cylindrical aggregates at low temperature, which undergo continuous one-dimensional growth with increasing temperature, and ultimately, an indication of a slight lamellarlike structural pattern is observed, which probably comes from the formation of micellar joints or branching. Such changes in the microstructure result in a decrease in the viscosity and stress-relaxation time, while the network structure is retained; the trends in the evolution of shear modulus (Go) and relaxation time (tauR) with temperature are in agreement with this. With increased surfactant concentration, the temperature corresponding to the viscosity maximum (T eta-max) in the temperature-viscosity curve shifts to lower values, and the viscosity at temperatures below or around T eta-max increases sharply. A viscoelastic solution with Maxwellian-type dynamic rheological behavior at low-shear frequency is formed, which is typical of entangled wormlike micelles. Rheological parameters, eta(o) and Go, show scaling relationships with the surfactant concentrations with exponents slightly greater than the values predicted by the living-polymer model, but the exponent of tauR is in agreement with the theory. Dynamic light-scattering measurements indicate the presence of fast relaxation modes, associated with micelles, and medium and slow modes, associated with transient networks. The disappearance of the slow mode and the predominance of the medium mode as the temperature increases support the conclusions derived from SAXS and rheometry.

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Aqueous foam stabilized by dispersed surfactant solid and lamellar liquid crystalline phase.

Foaming properties of dilute aqueous solutions of pentaglycerol monostearate (C(18)G(5)) and pentaglycerol monooleate (C(18:1)G(5)) have been studied at 25 degrees C. The aqueous C(18)G(5) system formed highly persistent foams, which did not rupture for several days. Foamability and foam stability were increased on increasing the surfactant concentration in both C(18)G(5) and C(18:1)G(5) systems. The C(18:1)G(5)/water system showed lower foam stability compared to the C(18)G(5)/water system. Aqueous phase behavior of the C(18)G(5) and C(18:1)G(5) systems showed the dispersion of alpha-solid and L(alpha) phase respectively in water rich region at 25 degrees C. Stable foam in the C(18)G(5)/water system was mainly due to the finely dispersed small surfactant solid particles. The average particles diameter of alpha-solid and L(alpha) dispersion is found less than 1 mum and it decreases with increasing surfactant concentration. There is no appreciable difference in the particle size of the alpha-solid and L(alpha) dispersion; however, the foam stability differs largely. Foam stabilized by lamellar liquid crystal dispersion in C(18:1)G(5)/water system, is less stable compared to the foam stabilized by the surfactant solid dispersion in C(18)G(5)/water system. The foamability and foam stability of the surfactant systems show poor correlation with the dynamic surface tension properties.

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Phase behavior and preparation of mesoporous silica in aqueous mixtures of fluorinated surfactant and hydrophobic fluorinated polymer.

The phase behavior and formation of self-assemblies in the ternary water/fluorinated surfactant (C(8)F(17)EO(10))/hydrophobic fluorinated polymer (C(3)F(6)O)(n)COOH system and the application of those assemblies in the preparation of mesostructured silica have been investigated by means of phase study, small angle X-ray scattering, and rheology. Hexagonal (H(1)), bicontinuous cubic (V(1)) with Ia3d symmetry, and polymer rich lamellar (L(alpha)(')) are observed in the ternary diagram. C(8)F(17)EO(10) molecules are dissolved in polymer rich aggregates, whereas (C(3)F(6)O)(n)COOH molecules are practically insoluble in the surfactant lamellar phase due to packing restrictions. Hence, two types of lamellar phases exist: one with surfactant rich (L(alpha)) and the other with polymer rich (L(alpha)(')) in the water/C(8)F(17)EO(10)/(C(3)F(6)O)(n)COOH system. As suggested by rheological measurements, worm-like micelles are present in C(8)F(17)EO(10) aqueous solutions but a rod-sphere transition takes place by solubilization of (C(3)F(6)O)(n)COOH. C(8)F(17)EO(10) acts as a structure directing agent for the preparation of hexagonal mesoporous silica by the precipitation method. The addition of (C(3)F(6)O)(n)COOH induces the formation of larger but disordered pores.

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