The Movement of Goods Around the Cell

By Patricia Bassereau and Bruno Goud The Movement of Goods Around the Cell A biologist and a physicist collaborate on a decade-long exploration of the physical parameters of membrane traffic in eukaryotic cells. 3-D reconstruction of confocal images showing membrane tubes pulled from a giant unilamellar vesicle by kinesin motors along microtubules. The tube diameter is about 100 nm and the vesicle diameter about 15 μm.Courtesy of Cécile Leduc In proka

By | April 1, 2011

The Movement of Goods
Around the Cell

A biologist and a physicist collaborate on a decade-long exploration of the physical parameters of membrane traffic
in eukaryotic cells.

3-D reconstruction of confocal images showing membrane tubes pulled from a giant unilamellar vesicle by kinesin motors along microtubules. The tube diameter is about 100 nm and the vesicle diameter about 15 μm.
Courtesy of Cécile Leduc

In prokaryotic cells, simple diffusion is largely responsible for getting nutrients to where they need to be and for removing waste products. But eukaryotes, which are much more complex, require a specialized mass-transit system. This system consists of membrane-bound structures called transport carriers that ferry cargo into, out of, and around the cell. Over the past decade, our interest has centered on this system, particularly on the interplay between the biophysical properties of the membranes and the way in which these properties are exploited by specific biological molecules to construct and direct this transport system. It is an ideal topic for collaboration between a biologist and a physicist.

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The other of us (Patricia) was trained as an experimental physicist in soft matter and had worked initially on the physical aspects of liquid crystals. The intrinsic nonequilibrium nature of biological membranes captured Patricia’s interest, leading her to study, in collaboration with Jacques Prost, the fluctuations of model lipid membranes in the presence of membrane proteins. Patricia had already known of Bruno’s findings on Rab6-decorated membrane tubules before we met.

Video: Bruno Goud and Patricia Bassereau talk about their fruitful collaboration exploring the physics of membrane trafficking in a Skype interview.

Assays and models

Almost immediately, we agreed on our joint goal: we would develop an in vitro assay that mimics the initial steps of intracellular transport. In particular, we would concentrate on the creation of the tubular carriers and the membrane deformation involved in their formation. We recruited a student, Aurélien Roux, to work with us. Aurélien, who now has his own lab in the biochemistry department of the University of Geneva, would generate tubular carriers by attaching biotinylated kinesin motor proteins to biotinylated lipid membranes using 100-nm polystyrene beads coated with streptavidin. The membranes known as giant unilamellar vesicles (GUVs) provide a simplified model of a cell membrane lipid bilayer. (See figure 1, below.) When incubated with microtubules and ATP in small chambers, GUVs did indeed give rise to membrane tubes and to complex tubular networks that could be visualized by confocal microscopy.2 (See photomicrograph on opposite page.) This experiment was the first demonstration that the force generated by kinesins was sufficient to pull a membrane tube from a membrane reservoir. Remarkably, as shown by transmission electron microscopy, the tubes that were pulled from GUVs made of egg phosphatidylcholine (EPC) had a constant diameter of 40±10 nm, a value close to that estimated for tubular transport carriers operating, for example, between the Golgi and the plasma membrane in vivo.

3 For these experiments, kinesins tagged with streptavidin were directly attached to the lipid membrane of GUVs via biotinylated lipids, following a method developed by the team of Marileen Dogterom in the Netherlands.4 (See figure 1.) In parallel, colleagues in the physics department had started to work on theoretical aspects of the physics of membrane tubes, to identify the forces and parameters involved in tube formation by molecular motors. Their analysis of the dynamics of motors on both vesicle and tube surfaces fitted Cécile’s experimental observations. Together, these studies identified the initial minimal surface density of motor proteins on the vesicle required to form membrane tubes, and, conversely, a maximum membrane tension above which motors cannot pull tubes.3 These model findings suggest that intracellular-membrane transport might be switched on and off in cells by regulating the number of available motors, the number of potential motor attachment sites (proteins or lipids) on the membrane, or the tension of the membrane. Cécile is now a researcher at the Centre de Physique Moleculaire Optique et Hertzienne in Bordeaux.

Getting physical

Using this minimal model, we also set out to investigate physical parameters involved in the early steps of intracellular transport, including membrane curvature, membrane bending rigidity, and membrane tension.

Because of the small diameter of actual transport carriers inside cells (typically 40–100 nm), they represent highly curved structures in comparison with the membrane from which they originate, which can be viewed as “flat.” During the early stages of vesicle formation from cell organelles, membrane proteins and lipids are sorted, ensuring efficient and accurate transport between cell compartments and the maintenance of homeostasis in organelle membranes. By 2004, the sorting of proteins had already been well described, but lipid sorting was much less clearly understood. To investigate constraints on lipid sorting, we pulled tubes from GUVs that were prepared from ternary mixtures of brain sphingomyelin, cholesterol, and dioleoylphosphatidylcholine (DOPC), representing the three major lipid components of the external leaflet of the plasma membrane. Depending on the relative proportion of the three lipids, they either mix to form a single homogeneous phase, or they demix and preferentially segregate in different phases. In the latter case, two phases coexist, a liquid disordered phase enriched in DOPC, and a liquid ordered phase enriched in cholesterol and sphingomyelin. The disordered phase is so called because the lipid tails in these patches of membrane have kinks and are disorganized so they do not pack together as closely as in the ordered phase.

The force required to pull a tube is proportional to the bending rigidity and the tension of the membrane.5 Using optical tweezers coupled to a micropipette system, we measured the bending rigidity of the ordered and disordered phases. (See figure 2.) Membranes in ordered phase are about twice as rigid as membranes in the more loosely packed disordered phase.6 Given this, we predicted that lipids of the ordered phase should be excluded from tube formation, to reduce the energy cost needed to bend the membrane into tubes. This is exactly what we observed. In phase-separated vesicles, tubes were preferentially pulled out from the disordered phase; when pulled from homogeneous vesicles, the tubes were enriched in lipids of the disordered phase (DOPC). These experiments provided the first direct demonstration that lipid sorting can occur during the formation of highly curved membrane tubes.6 There are two hypotheses to explain lipid sorting during vesicle formation: either the vesicle is formed from domains of the donor membrane where the lipids are already segregated, or lipid sorting occurs at the same time as the vesicle forms. Our in vitro experiments support the latter hypothesis, namely the dynamic sorting of lipids.

7 Our theoretician colleagues developed a model based on membrane elasticity and nonideal solution theory (in which forces between the solution components are not equal) to explain Benoît’s results. This model posits that the sorting of lipids between tube and vesicle is determined by a trade-off between mixing entropy and bending energy. The exclusion of lipids that have a tendency to form more rigid membranes lowers the energy required to form a curved membrane, and thus a thin tube. However, due to the small size of the lipid molecules, this effect is dominant over lipid mixing entropy only for compositions close to phase separation.7

Lipid-manipulating proteins

Because the tool set available to biologists to study cellular function have been predominantly biochemical techniques, the story of how cells work is dominated by protein interactions. Recently, researchers have begun to appreciate that physical properties play a much bigger role in cellular activities than was previously suspected. In fact, it is the ways in which a cell takes advantage of physical and biochemical properties together that has interested us most.

Aurélien had also observed that when phase separation of lipids occurs in the tubes, fission events take place at the boundary between ordered and disordered domains.6 It turns out that these observations are consistent with a theoretical analysis in which membrane rupture was predicted to originate from the difference in surface energy between the two phases, caused by their different composition. Much as nonmiscible liquids minimize their surface of contact, the lipids in bidimensional lipid domains minimize the length of their contact, resulting in a constricting force called line tension.8 Since the lipids in cell membranes are likely close to phase separation, these results raised the interesting prospect that the role of the numerous proteins implicated in sorting and fission events in vivo could be to trigger phase separation in membrane lipids, either by clustering specific lipids or by inducing membrane tubulation.9

Mechanoenzymes, including dynamin, are known to contribute to membrane fission. Dynamin is a large GTPase that polymerizes into a helical collar at the neck of endocytic buds, and induces the formation of endocytic vesicles through neck fission. Our work on line tension–induced membrane fission motivated us to explore the role of membrane curvature in the helical assembly of dynamin. Using a combination of confocal microscopy and optical tweezers, we discovered that membrane curvature triggers dynamin assembly, and thus the precise timing of the detachment of endocytic vesicles from the membrane.10

The functions of proteins that sense or induce membrane curvature have received considerable attention recently because of the importance of these phenomena during the formation of vesicles and tubular carriers involved in intracellular transport. During formation, vesicles and tubules are surrounded by coat proteins, such as the COPI coatomer, which are recruited to the site by activated coat-recruitment proteins such as Arf1 (ADP-ribosylation factor), a small G protein that binds to Golgi membranes as the first step in coat assembly. Several proteins involved in vesicle formation, including the ArfGAP1 protein, contain a lipid-binding structural motif, named ALPS, that senses membrane curvature.

11 This more hydro- phobic nature likely explains the extreme sensitivity of proteins with ALPS motifs to membrane curvature. ArfGAP1 is a GTPase-activating protein (GAP) that stimulates the hydrolysis of GTP bound to Arf1. In its GTP conformation, Arf1 binds strongly to membranes, where it promotes the assembly of the COPI coat on the surface of transport vesicles operating between Golgi and ER. (See figure 3.) The rate of ArfGAP1–induced GTP hydrolysis is dramatically higher—by about 50 times—on Arf1 bound to small (highly curved) liposomes (35 nm) than on Arf1 bound to larger (flatter) liposomes (150 nm).12

Our assay system was ideal for studying the spatial distribution of proteins between curved and noncurved membrane regions. Ernesto Ambroggio, a postdoc, worked with Benoît to compare the sensitivity to curvature of Arf1 and ArfGAP1. Arf1 bound almost equally well to the GUV membrane and to a tube pulled with kinesin motors or optical tweezers. Thus, Arf1 binding is, at most, only weakly sensitive to membrane curvature. In contrast, ArfGAP1 did not bind to the GUV at all. A curvature threshold was found for its binding to the membrane tubes: almost no binding was detected on tubes with a radius above 35±5 nm, while below this critical radius, ArfGAP1 density on the membrane increased linearly.13

13 Taken together, these finding suggest that membrane fission is the triggering event for coat disassembly. When the neck of the COPI-coated vesicle is cut, the dissociation of Arf1 from the membrane after GTP hydrolysis is no longer compensated for by Arf1 diffusion. As a result, the coat should readily disassemble. (See figure 3.)

Recently, Benoît has used a similar approach to study amphiphysin, a protein with a crescent-shaped binding domain that is involved in the generation of clathrin-coated vesicles. He showed that this protein has a dual behavior: at low concentration, its levels in membranes depend on membrane curvature—reminiscent of ArfGAP1—but it cannot deform the membrane. At high concentration, amphiphysin constricts a membrane tube, independently of the membrane tension (Sorre et al., submitted).


Our collaboration, combining biophysics and cell biology, and illuminated by our interactions with theoretical physicists, has been particularly fruitful and gratifying over the past 10 years. Right now we are planning to deepen our partnership still further with an ambitious project aimed at understanding how different classes of actin-based motors of the myosin family function in membrane trafficking and membrane dynamics. This project will exploit the minimal in vitro system developed in our laboratories.

Over the last decade we have challenged one another and generated reciprocal interests: Bruno has become more receptive to and interested in physics concepts, and Patricia continues to explore projects more related to cell biology. Based on the results of our cross-disciplinary collaboration, we advise others to embrace the approach. The challenges and rewards of considering alternative perspectives will add exciting new dimensions to your research design and experimentation.

Patricia Bassereau and F1000 Member References:

1. J. White et al., “Rab6 coordinates a novel Golgi to ER retrograde transport pathway in live Cells,” J Cell Biol, 147:743-760, 1999.
2. A. Roux et al., “A minimal system allowing tubulation with molecular motors pulling on giant liposomes,” PNAS, 99:5394-99, 2002.
3. C. Leduc et al., “Cooperative extraction of membrane nanotubes by molecular motors,” PNAS, 101:17096-101, 2004.
4. G. Koster et al., “Membrane tube formation from giant vesicles by dynamic association of motor proteins”, PNAS, 100:15583-88, 2003.
5. I. Derenyi et al., “Formation and interaction of membrane tubes,” Phys Rev Lett, 88:238101-1-4, 2002.
6. A. Roux et al., “Role of curvature and phase transition in lipid sorting and fission,” EMBO J, 24:1537-45, 2005. Free F1000 Evaluation
7. B. Sorre et al., “Curvature-driven lipid sorting needs proximity to a demixing point and is aided by proteins, PNAS, 106:5622-26, 2009.
8. J. Allain et al., “Fission of a multiphase membrane tube,” Phys Rev Lett, 93:158104, 2004.
9. V. I. Slepvev, P. De Camilli, “Accessory factors in clathrin-dependent synaptic vesicle Endocytosis,” Nat Rev Neurosci, 1:161-72, 2000.
10. A. Roux et al., “Membrane curvature controls dynamin polymerization,” PNAS, 107:4141-46, 2010.
11. G. Drin et al., “A general amphipathic α-helical motif for sensing membrane Curvature,” Nat Struct Mol Biol, 14:138-46, 2007. Free F1000 Evaluation
12. E. Ambroggio et al., “ArfGAP1 generates an Arf1 gradient on continuous lipid membranes displaying flat and curved regions,” EMBO J, 29:292-303, 2010. Free F1000 Evaluation
13. J. Bigay et al., “Lipid packing sensed by ArfGAP1 couples COPI coat disassembly to membrane bilayer curvature,” Nature, 426:563-66, 2003. Free F1000 Evaluation

This article is adapted from a review in F1000 Biology Reports, DOI:10.3410/B3-7 (open access at For citation purposes, please refer to that version.

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