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The Emergence of Competition Between Model Protocells

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Science  03 Sep 2004:
Vol. 305, Issue 5689, pp. 1474-1476
DOI: 10.1126/science.1100757

Abstract

The transition from independent molecular entities to cellular structures with integrated behaviors was a crucial aspect of the origin of life. We show that simple physical principles can mediate a coordinated interaction between genome and compartment boundary, independent of any genomic functions beyond self-replication. RNA, encapsulated in fatty acid vesicles, exerts an osmotic pressure on the vesicle membrane that drives the uptake of additional membrane components, leading to membrane growth at the expense of relaxed vesicles, which shrink. Thus, more efficient RNA replication could cause faster cell growth, leading to the emergence of Darwinian evolution at the cellular level.

A simple model of a primitive cell involves a self-replicating genome, such as an RNA polymerase ribozyme (a “replicase”), and an encapsulating membrane that can grow and divide (1) (supporting online text). Genomic influence over vesicle growth has been assumed to require a second RNA function, such as a ribozyme that would synthesize membrane components (2). Although such molecules presumably evolved at some point, we wondered whether the transition to a unified cell might have been facilitated by simpler physical mechanisms for coupling genomic properties and membrane behavior.

We sought to detect the emergence of an adaptive cellular-level trait based on the physical properties of a model prebiotic vesicle system containing encapsulated nucleic acids. Counterions associated with RNA encapsulated by a semipermeable membrane exert osmotic pressure on the membrane, which is counterbalanced by membrane tension. RNA replication would convert freely diffusing nucleic acid monomers into large impermeable macromolecules, increasing the concentration of trapped counterions. The resulting increase in osmotic pressure and membrane tension would create a driving force for an increase in membrane area, thereby coupling RNA replication to membrane growth (supporting online text).

We tested whether fatty acid vesicles (35) (supporting online text) osmotically stressed by encapsulated contents would increase in membrane area at the expense of unstressed vesicles. An initial concern was that fatty acid membranes might be too structurally weak to maintain a substantial osmotic gradient. We therefore determined the maximum sustainable membrane tension of oleate (C18:1) vesicles under osmotic stress. Oleate vesicles (100-nm diameter) encapsulating 1 M sucrose were diluted into hypotonic buffers (6). Applied gradients ≥0.7 M caused transient membrane rupture and release of solutes, detectable by size-exclusion chromatography, followed by membrane resealing at a maximal sustainable membrane tension (τ*oleate). After accounting for vesicle swelling from the extruded nonspherical shape to a spherical shape (7, 8) and the partial loss of encapsulated solutes, we estimate that τ*oleate is 10 dyn/cm, or 4 atm. A similar experiment with 100 nm POPC (1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine) vesicles showed that τ*POPC is 25 dyn/cm (supporting online text). These measurements fall within the range previously reported for phospholipid membranes (3 to 40 dyn/cm) (911). Thus, fatty acids, though chemically simple, can indeed form surprisingly strong membranes under osmotic stress.

We then performed competition experiments between swollen and isotonic vesicles. Low-osmolarity (isotonic) oleate vesicles were prepared in buffer without sucrose. High-osmolarity (swollen) vesicles were prepared by encapsulating sufficient osmolyte (e.g., 1 M sucrose) to generate the maximal sustainable membrane tension upon dilution into buffer. The two vesicle preparations were mixed in a stopped-flow device, and membrane surface areas of the swollen and isotonic vesicles were monitored in separate experiments using a fluorescence resonance energy transfer (FRET)–based assay (6). We observed that the membrane area of swollen oleate vesicles increased and the membrane area of isotonic vesicles decreased in parallel by ∼25% when mixed in a 1:1 ratio (Fig. 1, A to D), following first-order kinetics (koleate ∼ 0.1 s–1). Vesicle fusion, which would result in FRET decreases for both vesicle populations, does not explain the observed changes. No pronounced changes in FRET were seen upon mixing vesicles of equal osmolarity or mixing vesicles with buffer alone. Similar experiments with POPC vesicles showed no changes in FRET over several hours (Fig. 1, E and F), as expected from the very low vesicle-vesicle exchange rates of phospholipids (12, 13).

Fig. 1.

Stopped-flow mixing of isotonic and swollen oleate vesicles (1:1 molar ratio) in 0.2 M bicine, pH 8.5. Relative surface area was measured by the FRET assay; membrane growth decreases probe density, causing the FRET signal to decrease. Isotonic vesicles, labeled with FRET dyes, were mixed with unlabeled isotonic (A) or swollen (B) vesicles. The solid line indicates a single exponential decay curve fit with rate constant k = 0.09 s–1. Swollen vesicles, labeled with FRET dyes, were mixed with unlabeled swollen (C) or isotonic (D) vesicles. The solid line indicates the single exponential curve fit (k = 0.08 s–1). Isotonic (E) or swollen (F) POPC vesicles, labeled with FRET dyes, were mixed with unlabeled isotonic (open circles) or swollen (solid circles) POPCvesicles.

The above results show that vesicles with high internal osmotic pressure can acquire membrane from isotonic vesicles. These isotonic vesicles can lose membrane until they become spherical, but further membrane loss requires a volume decrease and concomitant concentration of their impermeable contents. The resulting osmotic gradient should eventually limit the redistribution of fatty acid. Indeed, as more swollen vesicles were added to a fixed number of initially isotonic vesicles, membrane loss reached a plateau (Fig. 2A). The maximum observed membrane loss from initially isotonic vesicles (∼35%) was somewhat larger than the estimated membrane loss necessary to adopt a spherical shape (∼27%; supporting online text), indicating that initially isotonic vesicles lost membrane until they also built up some osmotic gradient. Conversely, swollen vesicles, in the presence of excess isotonic vesicles, should grow until the membrane tension reaches zero, which we calculated should occur after a 35% surface area increase; the maximum observed increase was ∼35%.

Fig. 2.

(A) Change in surface area of isotonic vesicles mixed with different ratios of swollen vesicles, measured by FRET assay. Error bars indicate 95% confidence intervals for at least three trials. Time scale of intervesicular exchange of R18 in oleate (B) or MA:GMM (C) vesicles, measured by fluorescence dequenching. (B) Solid line indicates the single exponential curve fit (k = 3.1 min–1). (C) Solid line indicates a single exponential curve fit (k = 0.06 min–1).

To examine the mechanism of fatty acid transfer among vesicles, we tested the role of vesicle-vesicle collisions by varying the concentration of vesicles, but no rate changes were observed. Because the initial rate of uptake of fatty acid from micelles into vesicles can be quite fast compared with the observed rate of exchange (14), fatty acid adsorption is unlikely to be rate-limiting. We also tested the role of fatty acid desorption from vesicles, which becomes faster as chain length decreases (15). Myristoleate vesicles (C14:1) showed faster exchange (kmyristoleate ∼ 0.6 s–1). Exchange rates were also slower than fatty acid flip-flop rates (16). These observations indicate that exchange may be rate-limited by desorption, consistent with previous results on phospholipid transfer among liposomes (12, 17).

Having established that encapsulated osmolytes could drive vesicle growth at the expense of isotonic vesicles, we turned to vesicles that were osmotically swollen by encapsulated nucleic acids. Efforts to encapsulate high concentrations of nucleic acids (>0.1 M nucleotide monophosphate equivalents) in pure fatty acid vesicles caused visible aggregation and contents leakage. Because the addition of glycerol monoesters to fatty acid membranes has been reported to increase vesicle stability in the presence of high salt concentrations (18), we encapsulated nucleic acids in myristoleate:glycerol monomyristoleate (MA: GMM = 2:1) vesicles, which were stable (supporting online text).

Initial competition experiments with MA:GMM vesicles were done using vesicles containing 0.2 M uridine 5′-monophosphate (5′-UMP) (∼0.6 osmolar) (supporting online text). Growth of swollen vesicles and shrinkage of isotonic vesicles were observed as before (Table 1). The rate of exchange was substantially slower (kMA:GMM ∼ 0.1 min–1), consistent with the expected slower desorption rate from the more stable membranes. We confirmed that the difference between koleate and kMA:GMM quantitatively reflected the difference between the rate of lipid exchange in oleate versus that in MA:GMM vesicles using a self-quenching fluorescent fatty acid, octadecyl rhodamine B (R18) (6). Dilution of R18 among vesicles was detected as an increase in fluorescence (Fig. 2, B and C). The rate constant of R18 transfer in oleate vesicles (kR18oleate) was 3.0 min–1, whereas kR18MA:GMM was 0.06 min–1 (supporting online text). The fluorescence of R18-labeled vesicles did not change after mixing with buffer alone. These rate constants are in good agreement with the corresponding rate constants of osmotically driven lipid exchange.

Table 1.

Intervesicle competition reactions using RNA osmolytes.

Osmolyte FRET-labeled vesicles (low or high osmolarity) % surface area change k (min-1)
5′-UMP Low -45 0.05
High +36 0.02
Oligoribo-nucleotidesView inline Low -64 0.03
High +51 0.02
tRNA Low -23 0.1
High +21 0.1
  • View inline* Vesicles swollen by oligomers appeared to exchange more membrane than vesicles swollen by other osmolytes, an effect possibly due to salts or other minor components of bulk yeast RNA.

  • Membrane transfer to swollen vesicles was also observed when the osmolyte was a heterogeneous mixture of RNA oligomers obtained by alkaline hydrolysis of bulk RNA (93 mg/ml; ∼0.29 M nucleotide equivalents), which were 1 to 40 nucleotides in length as estimated by high-performance liquid chromatography. Finally, we observed membrane transfer using vesicles osmotically swollen by tRNA (83 mg/ml; ∼0.26 M nucleotide equivalents), which has a length (72 to 95 bases) comparable to that of many ribozymes (19) (Fig. 3) (supporting online text).

    Fig. 3.

    Intervesicle competition using tRNA to swell MA:GMM vesicles. Isotonic (A) or swollen (B) vesicles were labeled with FRET dyes and mixed with unlabeled swollen vesicles pressurized by tRNA (open circles), isotonic vesicles (solid circles), or buffer only (triangles). (A) Solid line indicates a single exponential curve fit (k = 0.09 min–1). (B) Solid line indicates a single exponential curve fit (k = 0.1 min–1).

    The concentrations of nucleic acids that produce this effect are biologically reasonable. In general, the concentration of genomic nucleic acid in a unicellular organism increases as the size of the organism decreases. For one of the smallest bacteria, Mycoplasma genitalium (∼300 nm in diameter), the concentration of DNA alone is 100 mg/ml (0.32 M nucleotide equivalents) (20). In a larger bacterium, Escherichia coli, the concentration of DNA is 13 mg/ml, and the combined concentration of DNA and RNA is ∼130 mg/ml (0.4 M nucleotide equivalents) (21). The RNA concentrations used in our osmotically driven growth experiments fell within this range.

    Our results show that osmotically swollen fatty acid vesicles can grow at the expense of relaxed (isotonic) vesicles. We have attempted to model the behavior of a primitive cell in which an RNA genome encodes functional RNA, but the same principles would apply given any other charged genetic polymer. In contrast, a neutral polymer such as PNA (peptide nucleic acid), having no associated counterions, would be a much less effective osmolyte, a difference that may have influenced the natural selection of the genetic material itself. We suggest that the phenomenon of osmotically driven, competitive vesicle growth could have played an important role in the emergence of Darwinian evolution during the origin of cellular life (supporting online text). The present results suggest that simple physical principles may allow a direct connection between genome and membrane. RNA replicating within vesicles could confer a substantial growth advantage to the membrane by creating internal osmotic pressure. The faster replication of a superior replicase would therefore lead to faster vesicle growth, at the expense of cells lacking RNA or containing less efficient replicases. A faster replicase genotype would thus produce the higher-level phenotype of faster cellular growth, a prerequisite of cellular replication (supporting online text). Darwinian evolution at the organismal level might therefore have emerged earlier than previously thought—at the level of a one-gene cell.

    Supporting Online Material

    www.sciencemag.org/cgi/content/full/305/5689/1474/DC1

    Materials and Methods

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