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We have analyzed the role of the phosphatidylinositol-4-phosphate adaptor protein-2 (FAPP2), a component of the apical transport machinery, in cilium formation in polarized Madin-Darby canine kidney (MDCK) cells. We show that ciliogenesis is defective in FAPP2 knockdown cells. Furthermore, by using fluorescence recovery after photobleaching studies of domain connectivity and the generalized polarization spectra of Laurdan, we demonstrate that FAPP2 depletion impairs the formation of condensed apical membrane domains. Laurdan staining also revealed that the ciliary membrane has a highly condensed bilayer domain at its base that could function as a fence to separate the ciliary membrane from the surrounding apical membrane. These results indicate that the compartmentalization of the apical membrane in MDCK cells into the ciliary membrane and the surrounding membrane depends on the balance of raft and nonraft domains.

Although it is well described in model membranes, little is known about phase separation in biological membranes. Here, we provide evidence for a coexistence of at least two different lipid bilayer phases in the apical plasma membrane of epithelial cells. Phase connectivity was assessed by measuring long-range diffusion of several membrane proteins by fluorescence recovery after photobleaching in two polarized epithelial cell lines and one fibroblast cell line. In contrast to the fibroblast plasma membrane, in which all of the proteins diffused with similar characteristics, in the apical membrane of epithelial cells the proteins could be divided into two groups according to their diffusion characteristics. At room temperature ( approximately 25 degrees C), one group showed fast diffusion and complete recovery. The other diffused three to four times slower and, more importantly, displayed only partial recovery. Only the first group comprises proteins that are believed to be associated with lipid rafts. The partial recovery is not caused by topological constraints (microvilli, etc.), cytoskeletal constraints, or protein-protein interactions, because all proteins show 100% recovery in fluorescence recovery after photobleaching experiments at 37 degrees C. In addition, the raft-associated proteins cannot be coclustered by antibodies on the apical membrane at 12 degrees C. The interpretation that best fits these data is that the apical membrane of epithelial cells is a phase-separated system with a continuous (percolating) raft phase <25 degrees C in which isolated domains of the nonraft phase are dispersed, whereas at 37 degrees C the nonraft phase becomes the continuous phase with isolated domains of the raft phase dispersed in it.

The technique of fluorescence recovery after photobleaching was used to investigate the lateral mobility of a fluorescein-labeled amphipathic apolipoprotein, ApoC-III, bound to multibilayers prepared from dipalmitoyl phosphatidylcholine, egg phosphatidylcholine, and a 1:1 (molar ratio) mixture of egg phosphatidylcholine and cholesterol. In dipalmitoyl phosphatidylcholine bilayers the lateral diffusion coefficient (D) for the protein is about 2 x 10(-9) cm(2) sec(-1) at 20 degrees C and about 9 x 10(-8) cm(2) sec(-1) at 45 degrees C. Plots of D versus temperature in this system show a transition between about 30 and 35 degrees C. Arrhenius activation energies for the diffusion in this case between 15 and 30 degrees C and between 35 and 45 degrees C are 28.5 and 7.0 kcal mol(-1), respectively (1 calorie = 4.18 joules). In egg phosphatidylcholine bilayers, D is about 3 x 10(-8) cm(2) sec(-1) at 20 degrees C and the Arrhenius activation energy for diffusion is 8.1 kcal mol(-1) between 15 and 35 degrees C in this system. In bilayers prepared from an equimolar mixture of egg phosphatidylcholine and cholesterol D at 20 degrees C is about 1.4 x 10(-9) cm(2) sec(-1) and the Arrhenius activation energy for the diffusion of the protein in this system between 15 and 35 degrees C is 15.1 kcal mol(-1). Light-scattering and fluorescence-polarization results indicate that binding of this protein does not affect the gel-to-liquid crystalline phase transition of bilayer membranes but does mediate a major, reversible aggregation of the vesicles at about 33 degrees C. These results lend support to the view that ApoC-III resides in the head-group region of the bilayer and suggest that its lateral diffusion coefficient represents an upper bound for integral membrane proteins.

The topographical distributions and mobilities of the murine histocompatibility antigen H-2Kk and of concanavalin A (Con A) binding sites have been studied on a murine lymphoma cell line. The spatial distribution of H-2Kk antigens, the average distance between H-2Kk antigens and Con A binding sites, and the separation of different determinants on the H-2Kk antigen itself were determined by using fluorescence resonance energy-transfer measurements with a dual-laser flow sorter. From the lack of energy transfer between bound monoclonal anti-H-2Kk antibodies conjugated with fluorescein (donor) and rhodamine (acceptor), we conclude that the H-2Kk antigen exists without appreciable clustering on the cell surface. Substantial energy transfer between appropriately labeled Con A and antibodies bound to the H-2Kk antigen shows that the two populations are interspersed. Donor/acceptor pairs of monoclonal antibodies binding to different determinants on the same H-2Kk antigen exhibited a degree of energy transfer indicative of a mean separation of 8.6 nm between the sites. Time-resolved phosphorescence anisotropy measurements with anti-H-2Kk antibodies labeled with eosin or erythrosin yielded rotational mobility information for the antigen-antibody complexes on the cell membrane. The rotational correlation time of 10-20 mus and the finite residual anisotropy are compatible with an uniaxial mode of rotation of monomeric antigen around its transmembrane portion and, thus, provide additional evidence for an unclustered distribution. Capping by rabbit anti-mouse IgG immobilized the antigen-antibody complex. Fluorescence recovery after photobleaching was used to calculate an apparent lateral diffusion coefficient of 5 +/- 3 X 10(-10) cm2 . s-1 for the H-2Kk antigen labeled with fluoresceinated IgG or its corresponding Fab fragment.