The non-covalent interactions between two phase-transfer catalysts allow tuning of reaction kinetics from bimolecular, to pseudo 0th order, to sigmoidal. Kinetic models and DFT calculations are used to obtain detailed insight in the system.
Abstract
The adaptivity of biological reaction networks largely arises through non-covalent regulation of catalysts' activity. Such type of catalyst control is still nascent in synthetic chemical networks and thereby hampers their ability to display life-like behavior. Here, we report a bio-inspired system in which non-covalent interactions between two complementary phase-transfer catalysts are used to regulate reaction kinetics. While one catalyst gives bimolecular kinetics, the second displays autoinductive feedback, resulting in sigmoidal kinetics. When both catalysts are combined, the interactions between them allow rational control over the shape of the kinetic curves. Computational models are used to gain insight into the structure, interplay, and activity of each catalytic species, and the scope of the system is examined by optimizing the linearity of the kinetic curves. Combined, our findings highlight the effectiveness of regulating reaction kinetics using non-covalent catalyst interactions, but also emphasize the risk for unforeseen catalytic contributions in complex systems and the necessity to combine detailed experiments with kinetic modelling.
Introduction
The behavior of living cells is largely regulated through complex networks of biochemical reactions. Without regulatory mechanisms, the kinetics of such reactions would mainly be governed by substrate concentration, leaving cells poorly able to adapt to changes in their environment. By evolving enzymes whose activity can be controlled through the non-covalent binding of cofactors,1,2 Nature has created means to dynamically up or downregulate specific reaction pathways depending on the need for certain products. Such a strategy is especially effective when the enzyme and effector molecule are part of the same metabolic pathway, as the resulting feedback or feedforward loops often give rise to strong and non-linear responses.3 Besides using small molecules to regulate catalysis, Nature also employs interactions between separate catalysts to regulate reaction kinetics. An example is the organization of metabolically linked enzymes into dynamic clusters called metabolons.4 This strategy not only enhances local substrate concentration and helps to segregate metabolic pathways, but also allows for control over entire pathways through disruption of the metabolon,5 or a more nuanced competition between the enzymes therein.6–8 Combined, such dynamic interactions between catalysts and other reaction compounds – including other catalysts – give rise to unique regulatory control that is characteristic of living systems.
Regulatable catalysts have proven to be a useful element in synthetic systems as well. For example, the binding of metals9–12 and other atoms13,14 has been used to create catalysts which can be switched “on” or “off”, or whose enantioselectivity can be altered. However, the catalyst-ligand binding strengths in such systems are usually too large to allow for dynamic competition and the possibility to perturb the system by small changes in concentration, temperature, or solvent composition.15,16 In addition, this type of regulation simply alters the reaction's overall rate or selectivity, and not the shape of its kinetic curves, as is the case in natural systems (e.g., the “sigmoidalness” of certain enzymes' reaction kinetics can be regulated by altering their sensitivity to autocatalytic feedback).17 To enhance synthetic catalysts' adaptability, single catalysts composed of multiple non-covalently bound molecules have been developed.18–22 Because such supramolecular catalysts are typically held together by relatively weak hydrogen bonds, their compositions – and thereby their activities and selectivities – are more open to gradual and dynamic regulation (e.g., by inhibition through the addition of a competing binding motif).23–26 Furthermore, the dynamic nature of supramolecular catalysts enhances their susceptibility to interact with other reaction components, which facilitates feedback mechanisms and communication between otherwise distinct reactions. Overall, the advancement of life-like synthetic systems is expected to benefit from dynamic control over both the overall reaction rate as well as the type of kinetics displayed by a reaction, and this can be achieved by employing multiple catalysts that interact with each other as well as with different reaction components.
Here, we present a combined theoretical and experimental study of a catalytic system in which the interactions between two complementary phase-transfer catalysts allow tuning of reaction kinetics ranging from bimolecular, to pseudo 0th order, to sigmoidal. This system builds upon our earlier findings demonstrating that the supramolecular binding motif 1,8-naphthyridine (NaPy) is able to function as a K2CO3 solubilizing phase-transfer catalyst for the Michael addition, for example in the reaction between maleimide and 2,4-pentanedione in chloroform (Fig. 1a).26 It was shown that this reaction displays bimolecular reaction kinetics and that the overall reaction rate can be regulated by inhibition using the NaPy complementary ureidopyrimidinone (UPy) motif.26 We also showed that a fixed ratio of NaPy and ditopic UPy can be diluted while buffering the concentration of catalytically active free NaPy, thereby desensitizing the Michael additions' rate to dilution.24–27
We now show that UPy motifs functionalized with an ester moiety on their alkylidene position can also function as phase-transfer catalyst and that the interactions between such catalytically active UPys and the NaPy catalyst can be used to regulate the kinetics of the Michael addition (Fig. 1b). Interestingly, sigmoidal kinetics are observed when the Michael addition is catalyzed by ester functionalized UPys which results from the Michael product stabilizing the catalytically active complex between UPy and K2CO3 (diUPy·K2CO3), thereby enhancing the latter's rate of formation (autoinduction). Besides stabilizing the diUPy·K2CO3 catalyst, the Michael product can also act as an individual phase-transfer catalyst by forming a complex with K2CO3 (product·K2CO3), thereby giving rise to autocatalysis. Kinetic models and density functional theory (DFT) calculations are used to obtain insight in the catalytic species' structures and the interplay between them. It is shown that the non-covalent interactions between the UPy and NaPy catalysts can be used to regulate reaction kinetics from bimolecular to strongly sigmoidal (Fig. 1b). In addition, we examine the extent to which the kinetics can be controlled by optimizing the linearity of the kinetic curves, thereby creating pseudo 0th order kinetics. The engineering of such bioinspired reaction networks containing interacting catalysts and multiple feedback loops will aid the development of autonomous chemical systems that sense their environment, processes chemical stimuli, and respond at the molecular level.
Results and discussion
Analyzing the bimolecular kinetics of the Michael addition catalyzed by NaPy and K2CO3
In good agreement with our previous work on a structurally similar NaPy,26 both NaPy 1 and K2CO3 were found to be required for efficient catalysis between Malref3 and Pentref4 (Fig. 2a and b). This NaPy and K2CO3 catalyzed reaction displays bimolecular kinetics and can be described by a mass-action kinetic model based on NaPy catalysis, background reaction catalysis by non-complexed K2CO3, and weak autocatalysis (vide infra). We propose that the observed catalytic activity of NaPy result from NaPy complexing K2CO3 (NaPy·K2CO3), thereby enhancing K2CO3's solubility and catalytic efficiency.26 An optimized DFT structure of the proposed NaPy·K2CO3 complex (see ESI†) shows that the nitrogen lone-pairs of NaPy 1, as well as its phenyl ring and carbonyl oxygen, can coordinate to a K+ ion, closely resembling naphthyridine complexes reported in literature.29–31 Although DFT calculations produced a stable structure assuming a NaPy : K2CO3 ratio of 1 : 1, a much higher stability was obtained for a structure comprising two NaPys per K2CO3 (diNaPy·K2CO3), likely because in that case each K+ ion is stabilized by a separate NaPy (Fig. 2c, see ESI† for the calculated stabilities of mono and diNaPy·K2CO3). Such a diNaPy·K2CO3 complex is also in agreement with our kinetic analysis, which shows that NaPy has a reaction order higher than unity (approximately 1.2, see Fig. S12F†). Combined, these data suggest that a mixture of mono and diNaPy·K2CO3 species is responsible for the catalysis observed, for clarity we will refer to this mixture simply as diNaPy·K2CO3.
During our investigation of NaPy's catalytic role, we found that reactions catalyzed by K2CO3 and pre-added product display slightly faster rates than those catalyzed by K2CO3 only (Fig. 2b). We therefore propose that in addition to NaPy, also the product is able to complex and solubilize K2CO3. A plausible structure of such a catalytic complex in which the Michael product binds K2CO3 (product·K2CO3) was provided by DFT calculations, showing coordination of several of the Michael product's carbonyl moieties to K2CO3 (Fig. 2d). Such product-mediated catalyst activation represents an uncommon form of ligand-acceleration,32 which has been classified both as autoinductive33 and autocatalytic.34,35 We chose to use the term autocatalysis to describe product·K2CO3-mediated rate acceleration, as this is in agreement with other systems in which the reaction product promotes its own formation by functioning as phase-transfer catalyst.35–37 Interestingly, no significant increase in reaction rate was observed when the diNaPy·K2CO3 catalyzed reaction was performed in the presence of additional Michael product (Fig. 2b). Subsequent kinetic analysis of these results showed that the high catalytic activity of NaPy 1 reduces the product's contribution to the overall conversion to just a few percent (see Fig. S13C† for computational fits and simulations). Combined, our results show that the kinetics of the NaPy catalyzed Michael addition are composed of diNaPy·K2CO3 catalysis, autocatalysis, and a K2CO3 background reaction, and that the overall kinetics of this reaction can be accurately described using a kinetic model that includes these contributions (Fig. 2e and S12E†).
Analyzing the sigmoidal kinetics of the Michael addition catalyzed by UPy and K2CO3
Having analyzed and modeled the K2CO3 background reaction, autocatalysis, and bimolecular NaPy catalysis, we turned our attention to the sigmoidal kinetics observed for the UPy-catalyzed Michael addition. While UPy homodimers are typically catalytically inactive, we discovered that UPys functionalized with an ester moiety on their alkylidene position (e.g., UPy 2) are able to solubilize K2CO3 and thereby act as phase-transfer catalyst for the Michael addition in CDCl3 (Fig. 3a and c). Surprisingly, the reactions catalyzed by UPy 2 and K2CO3 displayed sigmoidal kinetics, that is, an initial lag-phase followed by a strong increase in reaction rate (Fig. 3b). Interestingly, this lag-phase is only observed when all components are combined simultaneously i.e., when UPy 2 and K2CO3 are combined several days prior to the addition of the Michael substrates the lag-phase is absent (Fig. 3c). This suggests that the lag-phase originates from the time required to form a catalytically active complex between UPy and K2CO3 (diUPy·K2CO3). In good agreement, mixing UPy 2 with K2CO3 generates new signals in the 1H NMR spectrum of UPy 2 which only stabilize after several days (Fig. 3d). When 18-crown-6 is added as a competing K+ complexing agent the typical UPy 1H NMR signals are immediately recovered, proving that the complexation of K2CO3 by UPy 2 is indeed a slow, non-covalent, and reversible interaction. Furthermore, the addition of a separate complexation step between UPy and K2CO3 in our kinetic model results in a similar lag-phase and a better fit of the data (see Fig. S14† for validation). UPys lacking the ester functionality do not show any changes in their 1H NMR spectrum upon mixing with K2CO3, nor any catalytic activity towards the Michael addition. The optimized DFT structure of the diUPy·K2CO3 complex shows a structure in which the esters of the UPys fold back over the plane of the UPy–UPy dimer and thereby coordinate to K2CO3, in good agreement with our experimental observations (Fig. 3e).
To investigate the influence of the Michael product on the UPy 2 catalyzed reaction, the reaction between Malref3 and Pentref4 was performed in the presence of UPy 2, K2CO3, and additional product, added at the start of the reaction (Fig. 3f). Compared to the reactions catalyzed by UPy 2 and K2CO3 only, this led to a much shorter lag-phase and significantly faster reaction rates. Although the Michael product can act as a separate phase-transfer catalyst (vide supra), our model shows that the autocatalysis – determined by analyzing the reaction catalyzed by Michael product and K2CO3 only, Fig. 2b – is not strong enough to explain the observed rate-acceleration. Instead, our kinetic model and DFT calculations suggest that the product stabilizes the diUPy·K2CO3 complex by forming a structure in which K2CO3 is chelated by both the UPy dimer as well as the Michael product (Fig. 3g). Although this diUPy·product·K2CO3 complex catalyzes the Michael addition with a similar rate constant as the diUPy·K2CO3 complex, it is more stable and formed significantly faster, thereby giving rise to rate acceleration. Such product-mediated catalyst activation is termed autoinduction (see Fig. S15† for validation of inclusion of autoinduction in the kinetic model, and Fig. S12E† and DFT results for the determined rate constants and complex stabilities). Combined, our results show that although the product can act as an orthogonal catalyst (autocatalysis), in this reaction it functions mainly as an activator for the diUPy·K2CO3 catalyst (autoinduction, Fig. 3h and i). This autoinductive mechanism is therefore the predominant cause of the sigmoidal kinetic curves observed for the UPy catalyzed Michael addition (see Fig. S14 and S15†).
Tuning the Michael addition's reaction kinetics by combining NaPy 1 and UPy 2
Having analyzed the bimolecular kinetics resulting from NaPy 1 and the sigmoidal kinetics resulting from UPy 2 separately, we set out to examine the effect of combining both motifs (Fig. 4a). Previously, we have shown that binding of NaPy to any type of UPy – with or without ester functionality – inhibits diNaPy·K2CO3 catalysis through to the formation of catalytically inactive UPy–NaPy heterodimers.24,26 This ability of UPy to inhibit NaPy catalysis lead us to hypothesize that the interactions between catalytically active NaPy 1 and UPy 2 might be used to regulate the contribution of each catalytic species to the overall reaction rate, and thereby the kinetic profile of the Michael addition.
To test this hypothesis, the Michael addition between Malref3 and Pentref4 was performed in the presence of NaPy 1, K2CO3, and various amounts of UPy 2 (Fig. 4b). We observed that the addition of small amounts of UPy 2 (0.3 and 0.9 equivalents with respect to NaPy 1), led to a decrease of the overall reaction rate compared to the reaction performed without UPy 2 present. Increasing the UPy 2 concentration to 1.5 equivalents did not lead to a further reduction in the overall reaction rate, but notably altered the shape of the kinetic curve from bimolecular to a more linear character. Interestingly, performing the reaction with even more UPy 2 present (2.5 equivalents) led to an increase in the overall reaction rate and slightly sigmoidal kinetics.
To obtain more insight into this system, a kinetic model was constructed containing background catalysis by non-complexed K2CO3, phase-transfer catalysis by binding of either UPy–NaPy heterodimers, UPy homodimers, or the Michael product to K2CO3, and lastly, autoinduction by the Michael product enhancing the diUPy·K2CO3 catalyst's stability and rate of formation (Fig. 4c). Interestingly, when we used the optimized parameters obtained from modelling the reactions catalyzed by K2CO3 and UPy only, we were unable to model those catalyzed by both K2CO3, UPy and NaPy. Therefore, all parameters used to model the reactions catalyzed by both UPy and NaPy were set free. This discrepancy seems to be caused by an activating role of NaPy on the UPy catalysis vide infra. Gratifying, the computational model revealed that an increase in UPy 2 concentration leads to a rise in the UPy homodimer and UPy–NaPy heterodimer concentrations, as well as a decrease in the free NaPy concentration (Fig. 4b). The effects of the increasing amounts of UPy 2 on the reaction kinetics can thus be qualitatively explained by a decreasing contribution of the bimolecular kinetics resulting from diNaPy·K2CO3 catalysis, and an increasing influence of the sigmoidal kinetics brought about by the diUPy·K2CO3 catalyst. Similarly, the changes in the overall reaction rate arise from the varying amounts of diNaPy·K2CO3 and diUPy·K2CO3 catalyst present.
Although the observed changes in kinetics can be qualitatively explained by the varying concentrations of diNaPy·K2CO3 and diUPy·K2CO3 catalyst, a detailed analysis of our results revealed a complex interplay between these species. First, our DFT calculations revealed that the catalytically inactive UPy–NaPy dimers are able to form a stable complex with K2CO3 (UPy·NaPy·K2CO3), and that this proceeds through a UPy-type mechanism, i.e., the ester moiety on the UPy binds one of the K+ ions, while NaPy does not directly interact with K2CO3 (see ESI† for an optimized DFT structure of UPy·NaPy·K2CO3). This stability of UPy·NaPy·K2CO3 is somewhat surprising, as our kinetic analysis shows that it does not contribute to the overall catalysis (Fig. 4d). While we were not able to isolate UPy·NaPy·K2CO3 for further investigation, its lack of catalytic activity could be explained if multiple UPy–NaPy dimers are required to form an efficient phase-transfer catalyst. Such a structure comprising K2CO3 and several UPy–NaPy dimers might not be formed at concentrations high enough to produce a noticeable effect on the overall reaction rate, which agrees with the high reaction order suggested by our kinetic analysis (Fig. S12F†). Secondly, our kinetic analyses reveal that – although UPy and NaPy partially deactivate each other through the formation of UPy–NaPy dimers – the diUPy·K2CO3 catalyst itself has a higher catalytic activity and rate of formation when in the presence of NaPy 1 (Fig. S12E and F†). This could be explained by K2CO3 exchanging between fast forming diNaPy·K2CO3 and the more stable diUPy·K2CO3 (see ESI† for DFT calculated stabilities of all catalytic species). Lastly, our 1H NMR data suggests that binding of the Michael product to diUPy·K2CO3 (i.e., the autoinduction) shifts the UPy–NaPy equilibria from catalytically inactive UPy–NaPy heterodimers towards catalytically active UPy homodimers and free NaPy (not shown, as quantification of this phenomenon was troubled by gradual deuteration of UPy and NaPy). Such a shift in equilibria would agree with the Michael products' stabilizing influence on the diUPy·K2CO3 catalyst as determined by DFT, and would represent an additional source of rate acceleration by generating additional free NaPy and diUPy phase-transfer catalyst. Combined, these results show that the non-covalent interactions between NaPy 1 and UPy 2 give rise to a complex catalytic system which cannot be fully explained by a simple linear combination of the NaPy and diUPy phase-transfer catalysts.
Our results show that increasing the ratio of UPy 2 to NaPy 1 allows regulation of the Michael addition's kinetics from bimolecular to sigmoidal, with moderately linear kinetics obtained at intermediate UPy 2 concentrations (i.e., 1.5 eq.). However, the rate acceleration induced by UPy catalysis is not sufficient to counteract the influence of the decreasing substrate concentration on the reaction rate, and as a result all curves start to level off above ≈70% conversion (Fig. 4b). To examine the extent to which the kinetics in our system can be regulated – and test our kinetic model – we set out to optimize the linearity of the kinetic profiles. This specific goal was chosen because it requires delicate balancing of the biomolecular and sigmoidal contributions to the overall reaction rate, which will likely provide additional insight in the respective catalysts' properties. To achieve this, two goals need to be met. Firstly, it is essential that the reaction rates at higher conversions are increased, i.e., the rate acceleration resulting from autoinduction needs to be enhanced. Secondly, the optimal amount of NaPy required to linearize the kinetics has to be determined.
Enhancing the rate acceleration resulting from autoinduction
In our search for ways to enhance the rate-acceleration induced by the autoinductive binding of the Michael product to diUPy·K2CO3 – and thereby the linearity of the kinetic curves – we noticed that reaction rates have been shown to increase when a catalyst is covalently linked to one of its substrates.38,39 We hypothesized that in our system this approach might not only increase the overall reaction rate, but also enhance the degree of rate-acceleration by bringing the Michael product in close proximity of the diUPy·K2CO3 catalyst. To test our hypothesis, we synthesized UPypent5 in which pentanedione is covalently attached to the UPy motif (Fig. 5a). Functionalizing UPy in this manner is expected to have several effects: (1) the linker increases the local concentration of substrate (pentanedione) around the diUPy·K2CO3 catalyst, which is expected to increase the overall reaction rate; (2) after the pentanedione has reacted, the local concentration of Michael product around the diUPy·K2CO3 is increased in a similar manner. Since binding of the product to the diUPy·K2CO3 catalyst is the driving force for the rate-acceleration in the UPy catalysis (vide supra), this is expected to lead to stronger rate-acceleration; and (3) during the reaction, UPypent5 gets converted to UPyproduct6, as a result, the UPy catalyst gradually changes from diUPypent·K2CO3 to UPypent·UPyproduct·K2CO3 to diUPyproduct·K2CO3 (Fig. 5a). Given their different structures, it is proposed that these catalysts have different activities as well.
To test the influence of covalently linking UPy to pentanedione on the reaction kinetics, UPypent5 was reacted with Malref3. Interestingly, the reaction between 5 and 3 is much faster compared to reactions between Michael substrates 3 and 4 catalyzed by similar amounts of UPy 2 (Fig. 3b and 5b). As the high activity of UPypent5 is proposed to result from intramolecular interactions, and the equilibrium between intra- and intermolecular contacts depends strongly on concentration,39,40 we investigated the influence of concentration on the Michael addition catalyzed by UPypent5 and K2CO3. Surprisingly, reducing the concentration of UPypent5 and Malref3 by a factor eight resulted in only a slight decrease in reaction rate (Fig. 5b). This insensitivity could be described by a kinetic mass action model that includes the effects described (Fig. 5c), and revealed that the catalysts' efficiency increases from diUPypent (UD2) to UPypent·UPyproduct (UDUP) to diUPyproduct (see Fig. S16† for calculated reaction constants).
Optimizing the kinetic curves' linearity by tuning the NaPy concentration
Having successfully increased the rate-acceleration by linking pentanedione to the UPy motif, we investigated the influence of NaPy 1 on this system (Fig. 6a). The NaPy parameters obtained from the experiments using Malref3 and Pentref4 were used to predict the kinetics of mixtures containing K2CO3, NaPy 1, Malref3, and UPypent5. These simulations indicate that changing the concentration of NaPy is an excellent way to alter the linearity of the kinetic curves (Fig. 6b). According to our predictions, the most linear kinetic curve can be obtained using a mixture of 4 mM UPypent5 and ≈5 mM NaPy 1. Using these model results as a guide, we set out to experimentally determine the optimal ratio of NaPy 1 and UPypent5 for obtaining linear kinetics. While measurements performed using 4 mM UPypent5 and 4 mM NaPy 1 still displayed a lag-phase, increasing the NaPy 1 concentration to 6.5 mM resulted in near linear kinetics up to approximately 80% conversion (Fig. 6c). Further increasing the concentration of NaPy 1 to 8 mM lead to a decrease in the linearity of the kinetic curve and more bimolecular-like kinetics. These results show that, although absolute reaction rates cannot be predicted reliably, our model was successful in predicting the optimal conditions required to obtain pseudo 0th order kinetics. Furthermore, the linearity of the kinetic curves was increased in comparison to the curves obtained using UPy 2 and NaPy 1 (Fig. 6c).
In our current study we have mainly altered the UPy–NaPy equilibria by changing the ratio of these motifs. However, it has been shown that many stimuli, such as light,41 pH,42 temperature,28 redox chemistry,43,44 and disulfide exchange45 can also be used to influence UPy–NaPy dimerization. In addition, changing the molecular structure of UPy or NaPy,15,27,46 or the addition of complementary binding motifs,47,48 have also proven excellent means of controlling these equilibria. Incorporating such mechanisms in our system will likely generate alternative means to enhance its applicability.
Nevertheless, our study also highlights the challenges associated with further increasing the system's complexity. It underscores the high likelihood of (unexpected) interactions arising in complex catalytic systems and the difficulties associated with fully comprehending and modeling these. For example, while our kinetic models could accurately describe the reaction progress curves, we were not able to precisely determine the value of all reaction rate constants. Furthermore, certain rate constants seem to vary with the complexity of the system (e.g., the rate constants obtained from experiments with UPy only could not be used to satisfyingly predict the kinetics of reactions catalyzed by both UPy and NaPy). As explained, these limitations result from the exclusion of certain processes in our model, including transfer of K2CO3 between both catalysts and gradual shifts in the UPy–NaPy equilibria. Therefore, we believe that the further advancement of complex catalytic systems will increasingly rely on extensive kinetic modeling and the meticulous analysis of all interactions.
Conclusions and perspectives
Non-covalently interacting catalysts are excellent tools to regulate reaction kinetics. It was revealed that the commonly used ureidopyrimidinone (UPy) binding motif is able to function as a phase-transfer catalyst in the K2CO3 catalyzed Michael addition and that such UPy catalyzed reactions display sigmoidal kinetics as a result of autoinductive feedback. The kinetics of this Michael addition can be regulated from bimolecular to strongly sigmoidal using the non-covalent interactions between UPy and the complementary NaPy motif, which was previously shown to also function as a phase-transfer catalyst. The duration of the lag-phase and strength of the rate acceleration can be controlled using a variety of parameters, such as the premixing time of UPy and K2CO3, the ratio between UPy and NaPy, and by covalently attaching UPy to one of the substrates. The results obtained were far from easy to predict nor explained without using theoretical models. Using these detailed kinetic models, as well as DFT calculations, it was possible to propose molecular structures for the catalysts while insight into their contribution to the overall reaction rate were obtained. These insights were subsequently used to examine the systems' scope – and kinetic model's accuracy – by optimizing the linearity of the kinetic curves, thereby mimicking the kinetics of a 0th order reaction. Our findings suggest that catalytic supramolecular motifs are quite common and demonstrate how these can provide a direct link between covalent and non-covalent chemistry, a strategy that will benefit the advancement of life-like chemical systems. However, our results also emphasize the high likelihood of complex and hard to predict interactions arising in such catalytic systems and the accompanied necessity to computational model them.
Experimental
Detailed descriptions about the synthesis and characterization of the new molecules are given in the ESI.† Also, the theoretical models are presented as well as the way the kinetics were measured. In short, the kinetic measurements on the Michael additions were performed on 5 mL CDCl3 scale in Wilmad screw-cap NMR tubes, diameter 10 mm, length 7 inch. Solutions were made by mixing premade 20 mM stock solutions of all organic compounds. The NMR tubes were shaken and rotated on a Hecht Assistant rotating mixer and removed for ≈20 minutes to measure their conversion by 1H NMR. Conversions were determined by measuring the decrease in signals associated with the maleimide and 2,4-pentanedione moieties. K2CO3 (99.995% purity) was ground and filtered (<0.125 mm) before use.
Conflicts of interest
The authors declare no competing financial interest.
Supplementary Material
Acknowledgments
We would like to thank Dr Anja Palmans for useful discussions about synthesis and Roy van der Haas for synthesizing some of the organic compounds. This work is financed by the Dutch Organization for Scientific Research (NWOTOP and ECHO-STIP grant: No. 10007851 and No. 717.013.001), the Dutch Ministry of Education, Culture and Science (Gravity program 024.001.035), and the European Research Council (FP7/2007-2013 and H2020/2014-2020, ERC Advanced Grant No. 246829 and ERC Starting Grant No. 677313). Supercomputing facilities were funded by The Netherlands Organization for Scientific Research.
Footnotes
†Electronic supplementary information (ESI) available. See DOI: 10.1039/c9sc02357g
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