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Langmuir monolayers of C17, C19, and C21 fatty acids ... - UNAM

Langmuir monolayers of C17, C19, and C21 fatty acids ... - UNAM

Langmuir monolayers of C17, C19, and C21 fatty acids ... - UNAM

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7026 J. Chem. Phys., Vol. 110, No. 14, 8 April 1999 S. Ramos <strong>and</strong> R. Castillo<br />

FIG. 6. Phases observed with the BAM close to the L 2 – CS <strong>and</strong> L 2 – CS<br />

phase transitions. L 2 phase as seen just below the transition, upper panel,<br />

<strong>and</strong> CS phase just above the transition, medium panel (T4.9 °C <strong>and</strong> <br />

18.6 mN/m. In the lower panel, we show L 2 phase just starting the<br />

transformation to CS phase (T2.2 °C <strong>and</strong> 19.0 mN/m. Here, there is<br />

a light-gray needle-shaped structure, which suddenly appeared in the lower<br />

left part <strong>of</strong> the field <strong>of</strong> view, in the gray area.<br />

can be seen disappearing steadily from one phase (L 2 ) to the<br />

other (Ov), decompressing the monolayer. All our observations<br />

are consistent with a first-order transition, in agreement<br />

with the observations <strong>of</strong> Rivière et al. In C 21 , one part <strong>of</strong> the<br />

L 2 – Ov boundary must be almost vertical since, it was impossible<br />

for us to catch more experimental points for this<br />

phase transition close to 37 °C. See Fig. 3.<br />

The transition from L 2 – L 2 was observed with the BAM<br />

in C 19 <strong>and</strong> C 21 . This transition is characterized by a change<br />

FIG. 7. Phases observed with the BAM close to the L 2 – Ov phase transition<br />

at T22.8 °C <strong>and</strong> 19.4– 19.7 mN/m. a L 2 phase slightly below<br />

the phase transition; b When L 2 phase is compressed, the Ov phase appears;<br />

c Decompressing the monolayer, L 2 phase is recovered with almost<br />

the same domains.<br />

<strong>of</strong> domain shapes. The contrast between domains is low but<br />

clearly visible, as well as the phase transition. These features<br />

can be seen in Fig. 8. The low level <strong>of</strong> contrast is due to the<br />

same degree <strong>of</strong> anisotropy in both phases. We can see how<br />

rapid domains grow, decompressing the monolayer. We classify<br />

the transition as first order, however, the lack <strong>of</strong> contrast<br />

between domains does not allow to see the growing <strong>of</strong> domains<br />

as clearly as in other cases previously mentioned.<br />

Compressing the L 2 phase <strong>of</strong> C 21 <strong>fatty</strong> acid, at low temperature,<br />

allowed us to reach the outst<strong>and</strong>ing phase transition<br />

Downloaded 26 Feb 2003 to 132.248.7.15. Redistribution subject to AIP license or copyright, see http://ojps.aip.org/jcpo/jcpcr.jsp

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