We found an increasing rigi<strong>di</strong>ty of micelles rising thetemperature over the percolation line.assigned to the existence of αCD/4MP complexes.Based on the crucial presence of a small amount ofwater, the transition is assigned to a rearrangementof hydrogen bonds, lea<strong>di</strong>ng from a solvated αCD in4MP at lower temperatures to a regular network ofαCD molecules linked by water molecules at highertemperatures. The formed crystalline gel iscomposed of a fairly open regular structure of the4MP-αCD mixtureFig. 5. Here we show the light scattering data on AOTmicroemulsion, obtained by Sopra monochromator inbackscattering configuration (7.1 GHz), with theappropriate fitting function.signal HD-TG (a.u.)pure 4MP solventsound velocity (km/s)1,91,81,71,61,51,44MPαCD-4MPliquidphase1,3-40 -20 0 20 40 60Temperature (°C)solidphaseReferences[1] C.Ziparo, R.Eramo, I.Malfanti, C.M.C.Gambi andR.Torre. “Acoustic phenomena in AOT microemulsionsby frequency and time-resolved opticalspectroscopy”, in preparation.AuthorsR.Eramo (a,b), C.Ziparo (a,d), I.Malfanti (b,c),C.M.C.Gambi (a,c) and R.Torre (a,b,c). (a) INFM-CRS-<strong>Soft</strong> (CNR), Univ. la <strong>Sapienza</strong>. (b) LENS, Univ.<strong>di</strong> Firenze. (c) Dip. <strong>di</strong> <strong>Fisica</strong>, Univ. <strong>di</strong> Firenze.Freezing on heatingUnder the title “Freezing on heating” was recentlyreported the unexpected soli<strong>di</strong>fication upon heatingof a solution of a-cyclodextrine(αCD), 4methylpyri<strong>di</strong>ne (4MP) and water [1]. The solution ishomogeneous and transparent at ambienttemperature, and forms a milky white solid whenheated to temperatures between 45° and 75°. Thisprocess is fully reversible, on cooling the solid meltsand the original homogeneous solution is recovered.The role of water is essential, as demonstrated bythe incomplete soli<strong>di</strong>fication of samples withoutad<strong>di</strong>tion of water (ca. 10mg/ml). A major argumentfor the explanation of the phase transition is thenegative solubility of the αCD in 4MP, that dropsnearly vertically around 75°C, or at lowertemperature when more water is added to thesolution [2]. Diverse experimental techniques havebeen used to characterize the liquid and solid phasesof the mixture, and the mechanisms driving thisunusual phase transition. X-Ray <strong>di</strong>ffraction showedthat the solid phase is crystalline, and undergoesseveral phase transitions between 60 and 100°C.The lowest temperature phase is metastable, but 4other are stable and reversible with large hysteresisin temperature. Two of the transitions are alsoobserved in DSC measurements. Quasi elasticneutron scattering in<strong>di</strong>cates that the dynamics of thecyclodextrine in the solid phase slows down (> 500ps) while a large part of the solvent stays liquid overthe whole temperature range, moving oncharacteristic timescales of ps. In the liquid phase isalso detected a motion slower than the solvent itself,1E-8 1E-7 1E-6 1E-5time (seconds)Fig. 6. HD-TG signal of the pure solvent and of themixture, at room temperature. The right part of thefigure shows the variation of the sound velocity inthe αCD/4MP solution, that tends to join the 4MPbehavior when increases the temperature,extrapolated (solid line) from experimental points(square).αCD molecules, the remaining space being filled with4MP molecules, which remain partially mobile. In atypical solution of 300 mg/ml of αCD in 4MP, withca.10mg/ml of water added, the solid phase isformed of crystallites of 5 to 30 micron length,surrounded by liquid solvent. Acoustic stu<strong>di</strong>es,through Transient Grating spectroscopy, probe<strong>di</strong>rectly the viscoelastic properties of the solution.We therefore started to investigate structuralchanges in the liquid and pre transitional effectsusing this technique. The reorganization of thecomplex αCD/4MP could be responsible for thenegative solubility, by undergoing a change in itsstructure to which TG measurements will besensitive. A first comparison of the propagation ofthe acoustic wave in the pure solvent and αCD/4MPmixture exhibit very <strong>di</strong>fferent behavior of bothsamples at room temperature (see on figure 6),<strong>di</strong>fference that increases when the temperaturedecreases. Using the property that the solid phaseforms slowly (ca. 30 min), pre-transitional effectswere investigated at fixed temperature (following atemperature jump) by measurements at variousincreasing times: no change was observed in thedynamics of the liquid approaching the soli<strong>di</strong>fication.The system transforms <strong>di</strong>rectly from the solvatedαCD in 4MP into the crystalline phase. Preliminarymeasurements have been performed in the hightemperature phase (mixed liquid and solid). Onfigure 6 is shown the behavior of the sound velocityin the pure 4MP and the αCD/4MP solution: the liquidpart of the sample tends to join the pure 4MPbehavior. Surprisingly, the sound wave is notaffected by the solid phase, how can be expectedfrom this me<strong>di</strong>a presenting heterogeneities on themicrometer scale.83SOFT Scientific <strong>Report</strong> 2004-06
Scientific <strong>Report</strong> – Non Equilibrium Dynamics and ComplexityReferences[1] M. Plazanet, C. Floare, M.R. Johnson, R.Schweins, H.P. Trommsdorff, J. Chem. Phys. 121,5031 (2004).[2] M.Plazanet, M.Dean, M.Merlini, A.Hüller,H.Emerich, C. Meneghini, M.R. Johnson andH.P.Trommsdorff, “Heat induced crystallization andcomplex phase behavior of α-cyclodextrin solutions”,JACS, submitted.AuthorsM.Plazanet (a,b), P.Bartolini (a,b), A.Taschin (a,b)and R. Torre (a,b,c).(a) INFM-CRS-<strong>Soft</strong> (CNR), Univ.la <strong>Sapienza</strong>.(b) LENS , Univ. <strong>di</strong> Firenze. (c) Dip. <strong>di</strong> <strong>Fisica</strong>, Univ. <strong>di</strong>Firenze.Aqueous micellar solutionsA new Dielectric Spectroscopy technique wasdeveloped in the frequency range 30 MHz - 3 GHz.The complex permittivity of liquids is measured intransmission lines by a Vector Network Analyzer by<strong>di</strong>fferential methods. Two coaxial line cells weredone, <strong>di</strong>ffering for the length, and measured emptyand filled by the sample.This method gives "absolute measurements". Nocalibration by standard liquids is required. The cellshave to be machined with precision of 0.05 mm.Aqueous micellar solutions have been stu<strong>di</strong>ed atconstant temperature and pressure. The so<strong>di</strong>umdodecyl sulphate micellar solutions in the range 30mM - 520 mM were stu<strong>di</strong>ed by three models, SingleDebye, Cole-Cole and Double Debye. The Cole-Coleand Double Debye models lead to know therelaxation time and the <strong>di</strong>electric constant stepamplitude of the relaxation processes of the system.Two processes related to the micelle and to theinterfacial water have been shown with stepamplitudes from 10 to 30 vs. concentration andrelaxation times from 800 ps to 500 ps for themicelles, and step amplitudes from 1 to 12 vs.concentration and relaxation times practicallyconstant 110 ps for the interfacial water. The resultshave been tested by the Grosse's model for the<strong>di</strong>electric constant and by the Kallay's model for theconductivity, taking into account the parametersobtained by small-angle neutron scattering, SANS,ra<strong>di</strong>us of the micelle, interfacial layer, fractionalionization and aggregation number.We are working on new fluorinated compounds bySolexis-Solvay that lead to ionic micellar solutions inwater. SANS measurements have been performed todefine the microstructure of the system as a functionof the surfactant counterion. Shape and <strong>di</strong>mension ofthe micelles as well as the parameters of theinteraction potential between micelles have beenevaluated for the ammonium, potassium, lithium,cesium and <strong>di</strong>ethanol ammonium, having <strong>di</strong>fferentvolumes.The micelles interaction is due to hard sphere plusrepulsive Coulomb screened potential: Debye'slength and contact potential. As a function ofconcentration, temperature and counterion, themicelles can be spherical or ellipsoidal.Increasing the surfactant concentration, the micellegrow changes vs the volume increase, i.e. themicelle ionization degree decreases and the axialratio increase from 1.6 to 4.2 whereas the interfacialFig.7. The real and imaginary parts of the complex<strong>di</strong>electric constant for water and so<strong>di</strong>um dodecylsulphate aqueous micellar solutions at <strong>di</strong>fferentsurfactant concentrations.layer is constant 0.4 nm. The detailed structure isknown for the micelles, included the area per polarhead. These results are very important for manyapplications. Since 2004, the study of a portion of agiant multidomain protein from vertebrate muscles insolution, the β-connectin, is performed by DynamicLight Scattering (DLS). We are comparing AtomicForce Measurements on single molecule performedby a CNR - ISC group with DLS resultsReferencesLeandro Lanzi, M.Carla', C.M.C.Gambi and LeonardoLanzi, J. of Non – Cryst. Solids 351, 2864 (2005).C.M.C. Gambi, R. Giordano, A. Chittofrati, R. Pieri, P.Baglioni; and Teixeira J.J. Phys.Chem. B 109, 8592(2005).AuthorsL.Lanzi (a,b), S.Marchetti (a,b) and C.M.C.Gambi(a,b).(a) INFM-CRS-<strong>Soft</strong> Matter (CNR), Univ. la <strong>Sapienza</strong>.(b) Dip. <strong>di</strong> <strong>Fisica</strong>, Univ. <strong>di</strong> Firenze.SOFT Scientific <strong>Report</strong> 2004-0684
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