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Mesostructured fluids: supra aggregates made of interdigitated reverse micelles

Identifieur interne : 000949 ( Istex/Corpus ); précédent : 000948; suivant : 000950

Mesostructured fluids: supra aggregates made of interdigitated reverse micelles

Auteurs : A. Filankembo ; P. André ; I. Lisiecki ; C. Petit ; T. Gulik-Krzywicki ; B. W. Ninham ; M. P. Pileni

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RBID : ISTEX:32088867E661DDD3A86EAA3D3E34FD2E9CF0750B

English descriptors

Abstract

Abstract: In this paper we describe in detail the phase diagram Cu(AOT)2–water–isooctane in the oil rich region. The phase diagram is very rich. All the phases described are thermodynamically stable. In this paper we concentrate in the isotropic region obtained at rather large water content (29
Url:
DOI: 10.1016/S0927-7757(00)00513-6

Links to Exploration step

ISTEX:32088867E661DDD3A86EAA3D3E34FD2E9CF0750B

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<div type="abstract" xml:lang="en">Abstract: In this paper we describe in detail the phase diagram Cu(AOT)2–water–isooctane in the oil rich region. The phase diagram is very rich. All the phases described are thermodynamically stable. In this paper we concentrate in the isotropic region obtained at rather large water content (29</div>
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<abstract>Abstract: In this paper we describe in detail the phase diagram Cu(AOT)2–water–isooctane in the oil rich region. The phase diagram is very rich. All the phases described are thermodynamically stable. In this paper we concentrate in the isotropic region obtained at rather large water content (29>w=[H2O]/[AOT]>40). A transition from interconnected cylinder to reverse micelles is observed. At high surfactant concentration the system does not have enough oil to solvate the surfactant alkyl chains and large aggregates made of interdigitated reverse micelles are surrounded by isolated water in oil droplets.</abstract>
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<note type="content">Fig. 1: Phase diagram of Cu(AOT)2 in isooctane solution.</note>
<note type="content">Fig. 2: (A) The FFEM pattern of phase Vb1 at [Cu(AOT)]0=4.2·10−1 M, w=21. (B) The FFEM patterns of phase Vb2 at [Cu(AOT)]0=4.2·10−1 M, w=21.</note>
<note type="content">Fig. 3: Phase diagram of Cu(AOT)2 in isooctane solution containing 2% in mass of sodium derivative.</note>
<note type="content">Fig. 4: Variation of conductivity of 5×10−2 M Cu(AOT)2 in isooctane solution forming phase with increasing water content.</note>
<note type="content">Fig. 5: The FFEM patterns of phase VII obtained at w=40 at [Cu(AOT)2]0=1.2×10−1 M (A, B) and [Cu(AOT)2]0=4.2×10−1 M (C, D).</note>
<note type="content">Fig. 6: Variation of the conductivity with polar volume fraction at w=30 (A), w=36 (B). Comparison in the log scale of conductivity at w=30 and w=36 (C).</note>
<note type="content">Fig. 7: Cartoon of interdigitated reverse micelles.</note>
<note type="content">Table 1: Summary of the phase diagram of Cu(AOT)2/water/isooctane in the oil rich region</note>
<note type="content">Table 2: Water content, w; head polar group area σ; shape of the objects cylinders (c); spheres (s); length of the cylinders, Lc; width of the cylinders, lc; polar radius of spherical droplet, Rs·κ the conductivity; surfactant, φS; water, φW, and oil, φO, volume fractions measureda</note>
<note type="content">Table 3: Water content, w, head polar area, σ, shape of the objects cylinders (c), spheres (s), width of the cylinders, lc, polar radius of spherical droplet, Rs. Surfactant, φS, water, φW, and oil, φO, volume fractions measureda</note>
<note type="content">Table 4: Calculated surfactant and water volume fractions for a set of water content, w, in various structuresa</note>
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<abstract lang="en">Abstract: In this paper we describe in detail the phase diagram Cu(AOT)2–water–isooctane in the oil rich region. The phase diagram is very rich. All the phases described are thermodynamically stable. In this paper we concentrate in the isotropic region obtained at rather large water content (29</abstract>
<note type="content">Fig. 1: Phase diagram of Cu(AOT)2 in isooctane solution.</note>
<note type="content">Fig. 2: (A) The FFEM pattern of phase Vb1 at [Cu(AOT)]0=4.2·10−1 M, w=21. (B) The FFEM patterns of phase Vb2 at [Cu(AOT)]0=4.2·10−1 M, w=21.</note>
<note type="content">Fig. 3: Phase diagram of Cu(AOT)2 in isooctane solution containing 2% in mass of sodium derivative.</note>
<note type="content">Fig. 4: Variation of conductivity of 5×10−2 M Cu(AOT)2 in isooctane solution forming phase with increasing water content.</note>
<note type="content">Fig. 5: The FFEM patterns of phase VII obtained at w=40 at [Cu(AOT)2]0=1.2×10−1 M (A, B) and [Cu(AOT)2]0=4.2×10−1 M (C, D).</note>
<note type="content">Fig. 6: Variation of the conductivity with polar volume fraction at w=30 (A), w=36 (B). Comparison in the log scale of conductivity at w=30 and w=36 (C).</note>
<note type="content">Fig. 7: Cartoon of interdigitated reverse micelles.</note>
<note type="content">Table 1: Summary of the phase diagram of Cu(AOT)2/water/isooctane in the oil rich region</note>
<note type="content">Table 2: Water content, w; head polar group area σ; shape of the objects cylinders (c); spheres (s); length of the cylinders, Lc; width of the cylinders, lc; polar radius of spherical droplet, Rs·κ the conductivity; surfactant, φS; water, φW, and oil, φO, volume fractions measureda</note>
<note type="content">Table 3: Water content, w, head polar area, σ, shape of the objects cylinders (c), spheres (s), width of the cylinders, lc, polar radius of spherical droplet, Rs. Surfactant, φS, water, φW, and oil, φO, volume fractions measureda</note>
<note type="content">Table 4: Calculated surfactant and water volume fractions for a set of water content, w, in various structuresa</note>
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