Jamie S. Fostera and
Gareth O. Lloyd*b
aInstitute of Chemical Sciences, School of Engineering and Physical Sciences, Heriot-Watt University, Edinburgh, Scotland EH14 4AS, UK
bDepartment of Chemistry, School of Natural Sciences, Joseph Banks Laboratories, Lincoln, LN6 7DL, UK. E-mail: glloyd@lincoln.ac.uk
First published on 4th March 2025
Autocatalytic and/or self-replicating systems are important aspects of understanding the link between living systems (origins of life) and chemical networks. As a result, many scientists around the world are attempting to better understand these phenomena by producing chemical networks and linking them to self-assembly and pathway complexity (systems chemistry). We present here a superficially autocatalytic, self-replicating system that utilises dynamic imine chemistry coupled with self-assembling supramolecular hydrogelation kinetics driven by a nucleation autocatalytic cycle (autoinduction). The dynamic nature of the imine bond within water allows “error-checking” correction and driving of the imine equilibrium to the starting materials, but when coupled to the self-assembly process it gives rise to one reaction product from a possible thirteen intermediates and/or products (of a mixed four-step reaction). This product represents a thermodynamic minimum within the system's and reaction network's energy landscape. The self-assembly in solution of the replicator results in the formation of supramolecular polymers, which would normally markedly reduce the catalytic efficiency of the system if a template mechanism of autocatalysis is in play. By overcoming the limiting effects of the self-assembly process, it is possible to demonstrate exponential growth in replicator concentration once nucleation has occurred. It is only once the completed imine can undergo non-reversible tautomerisation that the product is prevented from reacting with water. We thus suggest that this sigmoidal kinetic characterisation is not inherent to autocatalysis kinetics (lowering reaction barriers and/or templating), but rather a result of the nucleation-based assembly allowing for intermediates to be prevented from reacting with water in a water-deficient environment (an autoinduction autocatalytic mechanism). Not only does this study provide a basis with which to explore aspects of self-replication connected with self-assembly, but it also explores how nucleation and self-assembly growth can play a crucial role in self-replication. By controlling the kinetics of the autocatalytic chemical reaction at one end of the hierarchical assembly process, we can influence the physical properties of the supramolecular gel at the other end. This may have wide-ranging applications with in-situ-formed small molecular gelators where specific mechanical properties (rheology) are desired.
The formation of Cn− could be monitored by HPLC and 1H NMR (Sections 9, 14, 15 and 18 of the ESI†). This was done in water with standard experimental conditions of pH 9 at 20 °C. The HPLC analysis measured absorption at 290 nm at retention times corresponding to A and Cn−. 1H NMR analysis focused on the conversion of the aldehyde peak of A at 9.6 ppm to the enamine peak of Cn− at 7.5 ppm.
Two solutions containing A (28 mM) and an excess of B take 72 hours after mixing to completely react to form Cn−. A plot of [Cn−] against time gives rise to a sigmoidal profile that suggests an autocatalytic process (Fig. S13 and S16†). A subsequent plot of the calculated autocatalysis with additional templating (product or seeds) can show the true nature of the kinetics (eqn (1)), either autocatalytic or reduce catalyst efficiency as replicator molecules may form dimers or higher ordered structures. This results in the system showing a non-exponential increase in product concentration, 0.5 ≤ p < 1; such a system's growth is said to be parabolic. To determine the order of the reaction, in terms of product concentration, the reaction was seeded with varying concentrations of previously isolated Cn− and the initial rate of Cn− formation was calculated (Fig. S14, S17 and S20†). von Kiedrowski showed that by plotting logd[Cn−]/dt against log[Cn−], where [Cn−] refers to the concentration of the seed added, p can be determined from the gradient of the line. We therefore determined the relationship, where the reaction rate for Cn− formation (d[C]/dt) against time results in a bell-shaped profile, again indicative of autocatalysis.6,25
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Eqn (1), above, is the general rate equation for an autocatalytic process.25 k[Cn−]p is the autocatalytic term, x is the non-autocatalysed reaction and p is the order of reaction with respect to the product. When p = 1, an autocatalytic system will exhibit an exponential increase in product concentration. The reliance of rate = 2.3[Cn−]1 (Fig. 1). We can see p = 1, thus showing that seeding resulted in an autocatalytic system with an exponential increase in product/replicator occurring.
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Fig. 1 Data for the autocatalytic reaction to produce Cn− and the mechanical properties arising from the hydrogel. Graph A shows [Cn−] over time. Standard conditions (○), stirring at 1000 rpm (△), addition of previously isolated C seed at a concentration of 2.5 mM (□). Graph B shows [Cn−] increase over time with increasing [seed]. Graph C shows the rate of formation of Cn− over time with increasing concentration of seeding Cn−. Graph D shows the initial rate of formation of Cn− plotted against concentration of seeding Cn−. Graph E shows the results of frequency-sweep experiments for gels set at different times after the initial mixing of A and B and the subsequent acidification to form C (coloured version, Fig. S12,† with clearer legends available). 0.5 h ○, 1 h ![]() ![]() ![]() ![]() |
The face-to-face, π–π stacking of Cn− molecules, evident in the powder X-ray diffraction patterns of dried samples (Fig. S34 and S35†), is proposed as the supramolecular interaction in the product template-based self-assembly and must be evident during a mechanism for the autocatalytic kinetics.26 The efficiency of the catalytic process relies on the number of accessible faces of Cn− molecules in solution. As the reaction progresses, it is possible to measure an increase in reaction solution viscosity, an indication of the supramolecular polymerisation of Cn−. Utilising isolated C and dissolving it in pH 9 water, an increasing concentration of Cn− in solution also results in an increase in viscosity. The viscosity of the solution shows a dramatic reduction at temperatures >30 °C. This results from dissociation of the π–π stacking interactions between monomers of Cn− that have formed supramolecular polymers.
There are two methods by which propagation of the supramolecular polymers can occur during the reaction: the conglomeration of individual Cn− molecules in solution that form through the non-catalysed process, and/or inclusion of an intermediate of the reaction network into the polymer chains potentially catalysing the formation of Cn−.
The Cn− molecules that form through the reaction process and are part of the supramolecular polymers may fail to dissociate from the polymer, resulting in an increase in polymer length. The presence of supramolecular polymers results in the effectiveness of the autocatalytic process observed experimentally being much lower than the theoretical maximum, as each static linear polymer chain only has two catalytically active end molecules/sites. It is well recognised now that this addition catalytically (similar to the template process of self-replication) would not lead to the kinetics observed. In our reactions, the replicator:product “duplexes” must be dynamic and related to the supramolecular polymerisation, as described by Otto and co-workers in their description of the fibre elongation/breakage mechanism, and many others who have observed autocatalytic kinetics during the self-assembly of supramolecular polymers/fibrils.27 In an attempt to mitigate the effects of the supramolecular polymer formation on the perceived catalytic activity, the solution was subjected to physical agitation (stirring at 1000 rpm with a magnetic stirrer; see ESI Sections 12 and 13† for details).26 Stirring of the solution was started immediately on mixing A and B and continued until the maximum concentration of Cn− was reached. With stirring, the reaction completed within 24 hours, much quicker than the same reaction without stirring. This confirms the autocatalytic kinetics is related to some form of assembly process, as stirring breaks/sheers the polymer chains into smaller units, increasing the number of accessible sites for chemical assembly or reactivity (we cannot determine which). With these observations, data, chemical reactivity, self-assembly, and unknowns in hand, we are naturally led to a discussion (hyperbole) of how do we describe this connectivity between the reaction network and self-assembly arising in an autoinduction observation.1
We can divide this discussion into two parts: (1) are any of the reaction steps (Fig. 2) catalytically enhanced during the process resulting in a self-replication mechanism; (2) is the self-assembly autocatalytic in nature (Fig. 3) and is there a connectivity between the reaction network and this autocatalytic assembly cycle?
The first reflexion of the reaction to take note of is that there is no analytical observation of any of the intermediates of the reaction network. This is a classic analytical limitation of many chemical reactions (most reactions have timescales/kinetics far quicker than most analytical tools) but is unusual given the network possibilities (13 intermediates and/or products, plus an additional five unlikely products associated with the tautomerisation of the five intermediates with free aldehyde groups). An additional fact is the reaction takes three days to complete. We and many others often observe intermediates of complex networks, so why do we not with this one?21 We postulate that the majority of the intermediates are unstable and transient within the water environment of the reaction, water (which is at its maximum chemical activity as both the solvent and reactant) driving the breaking of any imine formation back to starting materials (in terms of equilibrium chemistry, the water concentration (activity) is unbalancing the equilibrium away from product formation). If there was a template/autocatalytic process occurring with an intermediate and the final product (which clearly has the capacity to cause autoinduction by observation of the seeding process), then we can argue that something observable would be analytically determined so there is a high likelihood of there being no need or possibility for a templated autocatalytic chemical process as part of the imine equilibrium chemistry, except for the potential of the enol–keto tautomerisation. The chemistry presented in this discussion is well recognised as a non-reversible (normally thermally induced)21a,28 reaction that is not the reaction between two or more reactants but simply a conversion between two compounds that normally has a significant kinetic barrier. Enol–keto tautomerisations are normally in equilibrium and for the chemistry presented it has been observed to be different in water than in other chemical environments (not thermally induced and can be made reversible through an acid:base switch in certain circumstances).21a,28,29 Indeed, the chemistry has been used to make materials that are chemically inert to water. For the aniline derivatives we have worked with and published, we do not observe the enol form. Therefore the presence of water and salts (H+, OH− and Na+) are likely enhancing (catalysing) the enol–keto tautomerisation, as has been seen in many sugar chemistries (probably the most important autocatalytic process in regard to origin of life chemistries).
In most sugar chemistries that show autocatalytic behaviour (like the Breslow cycle), the products can be reincorporated into the reaction cycle/network. This is not possible for this chemistry and a template mechanism is the only option for generating an autocatalytic cycle. This reaction may be catalysed by the intermediate imine interacting with its product (the enol–keto process), and with water and the other constituents of the solution resulting in enhanced enol–keto tautomerisation. If we take our linear reaction steps from A and B to the two intermediates then to the thrice-reacted enol, we could potentially observe the simplest template-led autocatalytic chemistry for the tautomerisation. However, the product forms supramolecular polymers, and polymerisation is a known mechanism for poisoning a template autocatalysis reaction. Therefore, we think that we can preclude an in-solution template autocatalytic process. And therefore our focus should be put onto how the self-assembly may induce autocatalysis and the observed autoinduction (discussion point (2)) (Fig. 3).
Can the self-assembly of supramolecular polymers be autocatalytic in nature? Yes, this is evidenced by over a century of investigations into the nucleation phenomena of crystals, and the more recent work on supramolecular polymers, like amyloid fibrils.1,13 There are two published mechanisms in which the supramolecular polymers in this system could generate autocatalytic kinetics/cycles as part of their self-assembly process. These are: (i) fragmentation, which is the shearing of individual polymers into one or two “daughters” resulting in an averaged polymer length that is continuously sheared into growing smaller polymers; and (ii) detachment, where secondary nucleation on the surfaces of the polymers results in new polymers that are sheared off once a new polymer is of an appropriate size. With these facts in hand, we need now only couple the self-assembly of the supramolecular polymer to the reaction sequence, thus defining our system as autoinduction autocatalysis (Fig. 3).1 We hypothesise that the simplest way to do this is to couple the irreversible enol–keto tautomerisation to the autocatalytic cycle (conversion of the unstable enol intermediate AB3 to C). The alternative/related mechanism would be the surface functionality of the supramolecular polymer catalysing the formation of C via one of the four steps (causing an enhancement of secondary nucleation). This is a possibility but is rather complex in nature. A simpler mechanism can be suggested by taking into account that AB3 and C can coassemble into supramolecular polymers as their chemical structures are significantly similar. Once formed, this new chemical environment for AB3 (out of water) would enhance the probability of it converting to C permanently. If we then apply Le Chatelier's principle for the equilibria forming AB3, we can ascertain that the autocatalytic cycle coupled to the coassembly would dominate the kinetics resulting in our observations, i.e., the rates of inclusion and tautomerisation are greater than the rate of disassembly of the AB3Cp polymer.30 Our final remark is about why B is so important to these observations and the reaction network (as similar chemistries we have reported have not been observed to show these autoinduction kinetics). The other similar aniline chemistries we have performed have not had the competitive alternative reaction pathways that we see with the alkyl amine and aniline functional groups available in B. The other aniline kinetics are far too fast to analytically determine accurately, typically taking minutes, but with the reaction competition from the alkyl amine, the reaction with B is substantially slowed to days and also provides a “convenient” set of products that do not self-assemble, thus slowing nucleation (the induction point). Future work therefore aims to take this competitive chemistry and couple it to other aniline derivatives to determine if this autoinduction can be universally applied to our reactivity of A.
Once the reaction had reached completion, the solution was acidified to induce gelation. This resulted in an increase in the concentration of the charge-neutral form of Cn− (C), which is likely to be part of a more complex supramolecular polymer assembly. This alters the Cn−:
C dynamic ratio with the hydrophobic, zwitterionic species C proving to be an effective low molecular weight gelator (LMWG).31,32 C has a critical gel concentration (CGC) of 7.2 mM (0.5 wt%). Acidification of the solution was performed utilising glucono-delta-lactone (GdL) to ensure a homogenous pH change throughout the solution.33–35 With the isoelectric point (pI) of phenylalanine (5.91) being comparable to the apparent pI of C, it is possible to understand how the addition of GdL induces gelation. At the initial pH of 9, a point which lies above the pI, Cn− is the dominant compound (equilibrium) and is the more soluble form. Upon addition of GdL, the pH is slowly lowered below the pI of C, changing the dynamic ratio towards the more insoluble zwitterion. This insolubility gives rise to the formation of the fibrous network. The discotic nature of C lends itself to the one-dimensional assembly of fibres. It is a fibrous morphology that is observed by scanning electron microscopy (SEM) (Fig. S8†). It also means there is a reasonable agreement with the cellular solid model for describing the structure of supramolecular gels.36–38 The cellular solid model predicts that G′ ∝ [gelator]n, where G′ is the elastic modulus of the gel and n can lie between 1 and 2. By performing a concentration study and examining the gels’ responses to an applied oscillatory stress across a range of frequencies, the relationship G′ = 866[C]1.9 was obtained (see the ESI, Section 5†). This is in good agreement with the cellular solid model. This relationship allows kinetic data on the chemical reaction that produces Cn− to be extracted from the mechanical properties of the produced gels. Because the reaction is performed in situ, a gel can be set before the final maximum concentration of C (or Cn−) is reached, provided that [C] ≥ CGC. This will result in a gel with a G′ value that corresponds to the specific concentration of C achieved at the time of setting. This trapping out of C by a mass transfer limitation mechanism allows the mechanical strength of the gel in terms of G′ to be predictably controlled. By changing the time at which the gel is set, under specific conditions of the reaction, we have produced gels from a single stock solution with G′ values ranging from 730–2400 Pa. This results in a temporal dependence of the gels’ mechanical strength with respect to the reaction rate (the rate being autocatalytic in mathematical terms). The rheological measurements can also be utilised to calculate the concentration of C using the cellular solid model. Doing so results in a close match in the kinetics determined through rheology to that determined by NMR and HPLC (Fig. 1).
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5fd00016e |
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