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Biophys J, September 2000, p. 1400-1414, Vol. 79, No. 3
Department of Molecular Physiology and Biological Physics, University of Virginia, Charlottesville, Virginia 22908-0736 USA
There is increasing interest in supported membranes as
models of biological membranes and as a physiological matrix for
studying the structure and function of membrane proteins and receptors. A common problem of protein-lipid bilayers that are directly supported on a hydrophilic substrate is nonphysiological interactions of integral
membrane proteins with the solid support to the extent that they will
not diffuse in the plane of the membrane. To alleviate some of these
problems we have developed a new tethered polymer-supported planar
lipid bilayer system, which permitted us to reconstitute integral
membrane proteins in a laterally mobile form. We have supported lipid
bilayers on a newly designed polyethyleneglycol cushion, which provided
a soft support and, for increased stability, covalent linkage of the
membranes to the supporting quartz or glass substrates. The formation
and morphology of the bilayers were followed by total internal
reflection and epifluorescence microscopy, and the lateral diffusion of
the lipids and proteins in the bilayer was monitored by fluorescence
recovery after photobleaching. Uniform bilayers with high lateral lipid
diffusion coefficients (0.8-1.2 × 10
8
cm2/s) were observed when the polymer concentration was
kept slightly below the mushroom-to-brush transition. Cytochrome
b5 and annexin V were used as first test
proteins in this system. When reconstituted in supported bilayers that
were directly supported on quartz, both proteins were largely immobile
with mobile fractions < 25%. However, two populations of
laterally mobile proteins were observed in the polymer-supported
bilayers. Approximately 25% of cytochrome b5 diffused with a diffusion coefficient
of ~ 1 × 10
8 cm2/s, and 50-60%
diffused with a diffusion coefficient of ~2 × 10
10 cm2/s. Similarly, one-third of annexin V
diffused with a diffusion coefficient of ~ 3 × 10
9 cm2/s, and two-thirds diffused with a
diffusion coefficient of ~4 × 10
10
cm2/s. A model for the interaction of these proteins with
the underlying polymer is discussed.
Biophys J, September 2000, p. 1400-1414, Vol. 79, No. 3
© 2000 by the Biophysical Society 0006-3495/00/09/1400/15 $2.00
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