
I. The Molecular Design of Life 12. Lipids and Cell Membranes
12.6. Lipids and Many Membrane Proteins Diffuse Rapidly in the Plane of the
Membrane
Biological membranes are not rigid, static structures. On the contrary, lipids and many membrane proteins are constantly
in lateral motion, a process called lateral diffusion. The rapid lateral movement of membrane proteins has been
visualized by means of fluorescence microscopy through the use of the technique of fluorescence recovery after
photobleaching (FRAP; Figure 12.29). First, a cell-surface component is specifically labeled with a fluorescent
chromophore. A small region of the cell surface (~3 µm
2
) is viewed through a fluorescence microscope. The fluorescent
molecules in this region are then destroyed (bleached) by a very intense light pulse from a laser. The fluorescence of this
region is subsequently monitored as a function of time by using a light level sufficiently low to prevent further
bleaching. If the labeled component is mobile, bleached molecules leave and unbleached molecules enter the illuminated
region, which results in an increase in the fluorescence intensity. The rate of recovery of fluorescence depends on the
lateral mobility of the fluorescence-labeled component, which can be expressed in terms of a diffusion coefficient, D.
The average distance s traversed in time t depends on D according to the expression
The diffusion coefficient of lipids in a variety of membranes is about 1 µ m
2
s
-1
. Thus, a phospholipid molecule diffuses
an average distance of 2 µ m in 1 s. This rate means that a lipid molecule can travel from one end of a bacterium to the
other in a second. The magnitude of the observed diffusion coefficient indicates that the viscosity of the membrane is
about 100 times that of water, rather like that of olive oil.
In contrast, proteins vary markedly in their lateral mobility. Some proteins are nearly as mobile as lipids, whereas others
are virtually immobile. For example, the photoreceptor protein rhodopsin (Section 32.3.1), a very mobile protein, has a
diffusion coefficient of 0.4 µm
2
s
-1
. The rapid movement of rhodopsin is essential for fast signaling. At the other
extreme is fibronectin, a peripheral glycoprotein that interacts with the extracellular matrix. For fibronectin, D is less
than 10
-4
µm
2
s
-1
. Fibronectin has a very low mobility because it is anchored to actin filaments on the inside of the
plasma membrane through integrin, a transmembrane protein that links the extracellular matrix to the cytoskeleton.
12.6.1. The Fluid Mosaic Model Allows Lateral Movement but Not Rotation Through
the Membrane
On the basis of the dynamic properties of proteins in membranes, S. Jonathan Singer and Garth Nicolson proposed the
concept of a fluid mosaic model for the overall organization of biological membranes in 1972 (Figure 12.30). The
essence of their model is that membranes are two-dimensional solutions of oriented lipids and globular proteins. The
lipid bilayer has a dual role: it is both a solvent for integral membrane proteins and a permeability barrier. Membrane
proteins are free to diffuse laterally in the lipid matrix unless restricted by special interactions.
Although the lateral diffusion of membrane components can be rapid, the spontaneous rotation of lipids from one face of
a membrane to the other is a very slow process. The transition of a molecule from one membrane surface to the other is
called transverse diffusion or flip-flop (Figure 12.31) The flip-flop of phospholipid molecules in phosphatidyl choline
vesicles has been directly measured by electron spin resonance techniques, which show that a phospholipid molecule flip-
flops once in several hours. Thus, a phospholipid molecule takes about 10
9
times as long to flip-flop across a membrane
as it takes to diffuse a distance of 50 Å in the lateral direction. The free-energy barriers to flip-flopping are even larger
for protein molecules than for lipids because proteins have more extensive polar regions. In fact, the flip-flop of a protein
molecule has not been observed. Hence, membrane asymmetry can be preserved for long periods.
12.6.2. Membrane Fluidity Is Controlled by Fatty Acid Composition and Cholesterol