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Original

Potential Use of Fluorocarbons in Lung Surfactant Therapy

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Pages 211-220 | Published online: 11 Jul 2009

Figures & data

Figure 1 Compression isotherm (surface pressure (π)/molecular area (σ)) of DPPC measured at 26°C under an atmosphere of N2 (dashed line) and N2 saturated with PFOB (solid line). Fluorescence images of a) the DPPC monolayer at 15 mN m−1, showing the crystalline domains and b) the DPPC monolayer in contact with gPFOB (30 mN m−1).

Figure 1 Compression isotherm (surface pressure (π)/molecular area (σ)) of DPPC measured at 26°C under an atmosphere of N2 (dashed line) and N2 saturated with PFOB (solid line). Fluorescence images of a) the DPPC monolayer at 15 mN m−1, showing the crystalline domains and b) the DPPC monolayer in contact with gPFOB (30 mN m−1).

Figure 2 Fluorescence images of a DPPC monolayer compressed at 13 mN m−1 under N2 (upper image). At time t, the atmosphere of N2 above the monolayer started to be saturated with gPFOB. One can see that the LC domains progressively disappear with time. After 7 min, the monolayer is totally homogenous and fluid.

Figure 2 Fluorescence images of a DPPC monolayer compressed at 13 mN m−1 under N2 (upper image). At time t, the atmosphere of N2 above the monolayer started to be saturated with gPFOB. One can see that the LC domains progressively disappear with time. After 7 min, the monolayer is totally homogenous and fluid.

Figure 3 Diffracted intensity of the grazing X rays, I/I0, as a function of the in-plane scattering wave vector, qxy. When compressed at 20 mN m−1, the DPPC monolayer shows the two Bragg peaks characteristic of the tilted LC phase at 1.42 and 1.51 Å−1 (a). When He is saturated with gPFOB the peaks disappear rapidly (b), demonstrating the dissolution of the crystalline LC domains and the rapid re-spreading of the DPPC molecules.

Figure 3 Diffracted intensity of the grazing X rays, I/I0, as a function of the in-plane scattering wave vector, qxy. When compressed at 20 mN m−1, the DPPC monolayer shows the two Bragg peaks characteristic of the tilted LC phase at 1.42 and 1.51 Å−1 (a). When He is saturated with gPFOB the peaks disappear rapidly (b), demonstrating the dissolution of the crystalline LC domains and the rapid re-spreading of the DPPC molecules.

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