Towards a Light Driven Molecular Assembler

Towards a Light Driven Molecular Assembler

ARTICLE https://doi.org/10.1038/s42004-019-0163-y OPEN Towards a light driven molecular assembler Hanno Sell1, Anika Gehl1, Daniel Plaul1, Frank D. Sönnichsen1, Christian Schütt1, Felix Köhler1, Kim Steinborn1 & Rainer Herges 1 1234567890():,; Chemists usually synthesize molecules using stochastic bond-forming collisions of the reactant molecules in solution. Nature follows a different strategy in biochemical synthesis. The majority of biochemical reactions are driven by machine-type protein complexes that bind and position the reactive molecules for selective transformations. Artificial “molecular assemblers” performing “mechanosynthesis” have been proposed as a new paradigm in chemistry and nanofabrication. Here we present a simple non-proteinogenic machine-type molecule which drives the endergonic condensation of vanadate to cyclic tetravanadate using light as the energy source. The system combines selective binding of the reactants, accurate positioning, and active release of the product. Hydrolysis of the product prevents inhibition of further cycles. Our prototypic system demonstrates the prerequisites that are needed to selectively drive an endergonic reaction using an external energy source. 1 Institute for Organic Chemistry, University Kiel, Otto-Hahn Platz 4, 24098 Kiel, Germany. Correspondence and requests for materials should be addressed to R.H. (email: [email protected]) COMMUNICATIONS CHEMISTRY | (2019) 2:62 | https://doi.org/10.1038/s42004-019-0163-y | www.nature.com/commschem 1 ARTICLE COMMUNICATIONS CHEMISTRY | https://doi.org/10.1038/s42004-019-0163-y ost chemical processes in living organisms, unlike the [V ]total = 1.0 mM, I = 150 mM 100 3– larger part of synthetic chemistry, operate far from VO4 M 1 thermodynamic equilibrium . Major advances in syn- 80 HVO 2– thetic and supramolecular chemistry notwithstanding2–5, the 4 – fi total 60 H VO control of arti cial non-equilibrium systems is still in its infancy, ] 2 4 and has been identified as a major challenge in chemistry6. V 4– 40 V2O7 To achieve control of such systems, a number of prerequisites % [ HV O 3– have to be met that go beyond selective recognition and catalysis. 20 2 7 H V O 2– A crucial point is to couple an exergonic process (driving reac- 0 2 2 7 tion) to an endergonic reaction (driven reaction) in space and 0246810 12 14 V O 6– time to achieve an overall spontaneous process. pH 4 13 5– Here we demonstrate that a strong binding of the product in a HV4O13 [V ]total = 5.0 mM, I = 150 mM ligand can drive an endergonic condensation (Fig. 1). Photo- 4– 100 V4O12 chemical switching of the ligand to a non-binding state triggers V O 5– the release of the product. Subsequent hydrolysis in solution 80 5 15 6– allows for repeated cycles without product inhibition. While the V10O28 total 60 system operates at thermodynamic equilibrium, it may serve as a ] V HV O 5– 40 10 28 prototype for the future development of biomimetic systems. % [ 4– H2V10O28 20 3– H3V10O28 Results 0 + Vanadate condensation equilibria. For the rational design of our 0246810 12 14 VO2 prototype system, the synthesis of ATP from ADP and phosphate pH and the non-ribosomal peptide synthetases served as paragons. Fig. 2 Speciation of oxovanadium species as a function of pH.Percentage We chose the endergonic condensation of monovanadate to of different oxovanadium species in solution (speciation diagram) as a 2−+ + − 4−+ cyclic tetravanadate (4 HVO4 4H >V4O12 4H2O) as function of the pH value at an ionic strength I = 150 mM. For more details the model reaction to be driven. As compared to the phosphate see Supplementary Figs. 3 and 4, Supplementary Tables 2 and 3, 7 condensation, which would be closer to the ATP synthesis , Supplementary Note 1) vanadate aggregation has the advantage of having a lower barrier of activation and therefore is easier to catalyze. Moreover, vana- dium is one of the most NMR-sensitive nuclei in the periodic starting point for the design of a supramolecular system driving table8. Different vanadate aggregates give rise to distinct signals in the endergonic tetravanadate synthesis. We chose light as the the 51V-NMR spectrum, which can be unambiguously assigned, external energy source because it is convenient to apply and no and whose concentrations thus can be easily determined by interfering byproducts are formed in contrast to chemical energy integration9. Their relative concentration depends on con- sources. Moreover, vanadates are completely inert towards light centration, pH, and ionic strength of the solution (Fig. 2, for of wavelengths larger than 300 nm. Therefore, no direct impact details see Supplementary Table 1, Supplementary Note 1, Sup- on the vanadate condensation during irradiation was expected. plementary Figs. 3 and 4)10,11. At pH 9.5, and a total vanadate concentration of 1.5 mM, 2− monovanadate HVO4 is the predominant species in solution Design and synthesis of the photoswitchable ligand. To couple (>95%) (Fig. 2). This monovanadate solution served as the light energy to our photochemically inert reaction, we designed a ditopic, photoswitchable receptor12,13. The receptor consists Δ G1 > 0 of a photochromic azobenzene unit, and two Zn-cyclene moieties attached to both ends via methylene groups. Azobenzenes are very reliable, efficient, and frequently used photoswitches14, and Endergonic Zn-cyclene is known to bind phosphates15 and vanadates9 even in water with high affinity. Upon irradiation with 365 nm light, the azobenzene isomerizes from its trans to the cis form, and light + Δ Δ G3 ~ 0 + G4 << 0 of 430 nm induces the isomerization back to the trans config- uration. Thereby, the receptor performs a pincer-like motion (cis 1 ⇄ trans 1, Fig. 3). The two binding sites (Zn-cyclene units) approach each other Δ from a distance of about 11 Å (Zn–Zn distance, open form) to less G2 < 0 than 4 Å (closed form). Density functional theory calculations (B3LYP/6-31 G*) predict that the cyclic tetravanadate fits exactly Exergonic between the two Zn-cyclen units if the ditopic receptor is in Δ Δ Δ fi G2 = G1 + G4 < 0 the open trans con guration (monovanadate and divanadate are too small and the linear trivanadate is too large, Supplementary Fig. 1 Thermodynamic cycle of a dimerization model reaction, driven by Figs. 12 and 13 and Supplementary Note 3). A second ligand can strong binding of the product in a host ligand.The overall reaction is interact with the remaining four terminal oxygen atoms, thus spontaneous, if the sum of the (positive) free energy of dimerization ΔG1 is wrapping the tetravanadate in a tennis ball-like fashion and more than outmatched by the (negative) free energy of binding ΔG4. The preventing hydrolysis. The ditopic receptor in its closed cis dimerization reaction may either take place inside the ligand or the ligand configuration does not bind any vanadate species because the two traps small amounts of the product formed in equilibrium outside the binding sites are too close to each other. Thus, upon alternating ligand. The free energy change from the initial to the final stage is irradiation with 365 and 430 nm the ditopic receptor switches independent of the mechanism (Hess Law) between a non-binding mode and a configuration that is strongly 2 COMMUNICATIONS CHEMISTRY | (2019) 2:62 | https://doi.org/10.1038/s42004-019-0163-y | www.nature.com/commschem COMMUNICATIONS CHEMISTRY | https://doi.org/10.1038/s42004-019-0163-y ARTICLE hν 430 nm N N 3+ 2 4+ N N N 2 H N N N N N Zn O N N Zn Zn N Zn N trans 1 N N N N N N O 4– 2– cis 1 O O O V O OO 4 V OH O O V O V O V O O 4– O O or V412 O + hν + 4 H 365 nm + 4 H2 O – 4 H2 O 25 ms + – 4 H 4+ N N N NH 2– O O Zn N O N N O N V N V N O Zn O OH O O 4 Zn O H V V N O N O V N H N O N N H O O ZnZ N N N N Fig. 3 Cyclic process of photoswitchable ligand 1 driving the condensation of monovanadate to cyclic tetravanadate.To enhance comprehensibility the cyclene units are shown in red, the tetravanadate ring in blue and the phenyl rings in grey shade and selectively binding cyclic tetravanadate. The ditopic receptor conditions is −68.3 kcal mol−1. Proton NMR spectra are also in was prepared in a three-step synthesis (for details see Supple- agreement with the theoretically predicted binding mode. mentary Fig. 1)16. Whereas the 1H NMR spectrum of the closed form of the receptor does not change upon addition of vanadate, the phenyl proton signals of the open form broaden, and shift upfield by 0.3 Thermodynamic measurements. The monotopic ligand Zn- ppm by anion–aromatic interactions22. The experimental value benzylcyclene12 served as a reference compound. NMR titrations is in very good agreement with the calculated (GIAO B3LYP/ following the 1H as well as the 51V NMR signals reveal that there 6-31 G*) upfield shift of 0.4 ppm in the tennis ball-type complex is no measurable interaction between the closed cis-receptor compared to the free receptor (Supplementary Fig. 11). The signal and the vanadate in solution (Supplementary Fig. 7), whereas broadening is due to the restriction of the conformational flex- the monotopic receptor binds vanadate with a formation constant ibility of the phenyl groups in the rigid complex. of log K = 3.812. We attribute the non-coordinating property The product is now stuck in the receptor and the situation of the ditopic cis-receptor to the fact that the two Zn2+ ions are corresponds to what Smalley coined the sticky finger problem23.

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