Sergey S.
Zalesskiy
,
Nikita S.
Shlapakov
and
Valentine P.
Ananikov
*
Zelinsky Institute of Organic Chemistry, Russian Academy of Sciences, Leninsky prospekt, 47, Moscow, 119991, Russia. E-mail: val@ioc.ac.ru
First published on 12th July 2016
The carbon–sulfur bond formation reaction is of paramount importance for functionalized materials design, as well as for biochemical applications. The use of expensive metal-based catalysts and the consequent contamination with trace metal impurities are challenging drawbacks of the existing methodologies. Here, we describe the first environmentally friendly metal-free photoredox pathway to the thiol–yne click reaction. Using Eosin Y as a cheap and readily available catalyst, C–S coupling products were obtained in high yields (up to 91%) and excellent selectivity (up to 60:1). A 3D-printed photoreactor was developed to create arrays of parallel reactions with temperature stabilization to improve the performance of the catalytic system.
We propose a practical approach to access valuable S-functionalized products using a cheap and readily available alkyne made by the condensation of acetylene with acetone via the Favorskii reaction (Scheme 1). An atom-economic thiol–yne click reaction yields sulfenylated alkenes, which can be readily converted to dienes by known dehydration protocols in one step (Scheme 1). Sulfenylated dienes are universal building blocks for organic synthesis and polymer science.9 Their high reactivity in Diels–Alder reactions facilitates cycloaddition under mild conditions.10,11 The overall process is totally atom-economic and environmentally benign; the target product is formed from acetylene, acetone and thiol, releasing only one molecule of water. The key step of the overall process is the thiol–yne click reaction, which should be performed with high stereo- and regioselectivity and without a metal catalyst. It is important to exclude transition metal catalysts at this step because their avoidance decreases cost and eliminates the generation of toxic wastes. Thus, carrying out this transformation under metal-free, visible light-mediated conditions would provide an important advance in the synthetic methodology.
Scheme 1 The key light-mediated thiol–yne click reaction for the synthesis of activated dienes from simple precursors. |
Herein, we present the first example of a metal-free photoredox thiol–yne click reaction. We have utilized the outstanding advantages of photocatalytic processes to render transformations of functionalized organic molecules.12 A special emphasis was placed on using organic catalysts13 to avoid metal contamination and to increase cost efficiency. To the best of our knowledge, no examples of metal-free photoredox thiol–yne coupling have been reported to date.14
# | Catalystb | Solvent | LED | 3a, % | E:Z |
---|---|---|---|---|---|
a Conditions: 0.3 mol% catalyst loading, stirring under LED light for 4 h; see ESI for details. b Control experiments in the absence of photocatalyst were also performed; see ESI for details. | |||||
1 | [Ru(bpz)3][PF6]2 | MeCN | 465 nm | 34 | 20:1 |
2 | [Ru(bpy)3][PF6]2 | MeCN | 465 nm | 40 | 30:1 |
3 | Ir(ppy)3 | MeCN | 530 nm | 63 | 40:1 |
4 | Fluorescein | MeOH | 465 nm | 60 | 27:1 |
5 | Bengal rose | DMF | 530 nm | 53 | 25:1 |
6 | Eosin Y | MeOH | 530 nm | 53 | 25:1 |
7 | Eosin Y | DMF | 530 nm | 15 | 14:1 |
8 | Eosin Y | MeCN | 530 nm | 56 | 27:1 |
9 | Eosin Y | Et2O | 530 nm | 20 | 20:1 |
10 | Eosin Y | DMSO | 530 nm | 63 | 30:1 |
Known ruthenium (entries 1 and 2, Table 1) and iridium-based (entry 3) photoredox systems gave good yields and E:Z selectivities of the desired product. Three different organic dyes demonstrated similar yields but afforded lower selectivity (entries 4–6, Table 1) relative to the Ir catalyst (entry 3, Table 1). Varying the solvent (entries 6–10, Table 1) allowed us to achieve 63% yield of 3a and 30:1 selectivity using Eosin Y as a photosensitizer (entry 10, Table 1). Although initial screening did not favor organic dyes as viable catalysts due to lower selectivities (cf. entries 3 and 10, Table 1), we developed this approach further to meet the requirements of cost-efficiency and avoiding metal contamination.
Variation of the amount of photocatalyst revealed a non-uniform trend (Table 2). Decreasing the amount of Eosin Y initially resulted in an increase in both the yield and selectivity (entries 1, 2 and 4, Table 2) but further lowering the amount of the dye led to a decrease in both parameters (entries 4 and 5, Table 2). It is very likely that the combination of two factors, namely excitation of only the surface layer of the solution due to increased optical density (because of the large amount of the dye in solution) and reaction stoppage due to degradation of Eosin Y (especially for very low dye loadings), is responsible for the observed behavior. Indeed, rapid degradation of the photocatalyst was clearly visible at low catalyst loadings, which resulted in discoloration of the solution.
# | Eosin Y, mol% | Solvent | Yield, % | E:Z |
---|---|---|---|---|
a The reaction conditions were similar to those in Table 1. b The reaction time was 5 h (longer reaction times did not further improve the yield). | ||||
1 | 2 | DMSO | 15 | 30:1 |
2 | 0.3 | DMSO | 38 | 30:1 |
3 | 0.3b | DMSO | 65 | 30:1 |
4 | 0.02 | DMSO | 46 | 45:1 |
5 | 0.001 | DMSO | 33 | 32:1 |
6 | 0.3 | Hexane | 70 | 37:1 |
7 | 0.3b | Hexane | 85 | 50:1 |
8 | 0.02 | Hexane | 11 | 10:1 |
9 | 0.001 | Hexane | 9 | 8:1 |
We found that the dye degradation issues can be overcome by switching the reaction solvent to hexane (Table 2, entries 6 and 7). Eosin Y exhibits very low solubility in hexane, and at the beginning of the reaction, the majority of the Eosin Y remains undissolved. A low concentration of the dissolved catalyst results in a reaction mixture with optimal optical density and ensures uniform excitation of the reaction volume.
The dissolved photocatalyst slowly degrades during the course of the reaction, which makes the solution unsaturated. This naturally leads to the dissolution of subsequent portions of Eosin Y from the solid phase. This “saturation feedback” automatically maintains the concentration of the photocatalyst at the optimal level, thus compensating for the loss of active species. Under such self-regulating conditions, yields and E:Z selectivities as high as 85% and 50:1, respectively, were achieved (entry 7, Table 2).
Thus, a typical photoredox system with Eosin Y suffers from gradual photocatalyst degradation during the course of the reaction when all of the catalyst is dissolved in the reaction mixture (Fig. S1, ESI†). This degradation can halt the progress of the reaction at the middle or even initial stages of the reaction (entries 8 and 9, Table 2). In the developed approach, the low solubility of the photocatalyst increases the efficiency of light utilization by maximizing reactive excitations. The inevitable degradation of the photocatalyst is immediately compensated by the undissolved portion (Fig. S1†). It should be noted that when identical catalyst loadings were used in different solvents, namely DMSO and hexane (i.e., 2.1 mg of Eosin Y for 0.3 mol%), the reaction was governed by the solubility of the photocatalyst. Notably, the reaction in hexane proceeded with higher selectivity and yield than the reaction conducted in DMSO (entries 3 and 7, Table 2).
After establishing the optimal reaction conditions, efforts were focused toward performing thiol–yne click reactions with different substrates. The developed synthetic approach provides excellent opportunities for incorporating various sulfur substituents (R) by using readily available thiols (Scheme 1). However, investigation of the substrate scope has shown that the process suffered from low reproducibility due to poor temperature control and variations in light intensity from one LED set up to another.
A closer examination revealed that experimental conditions (e.g., temperature and light intensity) can significantly vary depending on the particular setup. Commonly used LED strips wrapped around the photocatalytic system substantially heat the reaction vessel. The inner temperature of such an assembly can reach up to 60 °C, with large temperature variations of ±10 °C (Fig. 1A). Another standard setup involves placement of the reaction vessel on top of a single LED or LED matrix (Fig. 1B), which may increase the temperature up to 45 °C with temperature variations of ±5 °C. The optimal solution would provide irradiation of the reaction mixture from top, with the LED source incorporated into the vessel's cap (Fig. 1C). In such a setup, temperature stabilization and stirring can be easily performed using a standard oil or water bath equipped with a magnetic stirrer.
Fig. 1 Comparison of the possible designs of the photoreactor: (A) side irradiation (LED strip); (B) bottom irradiation (LED matrix); (C) developed design with temperature stabilization. |
Because LED sources incorporated into reaction vessel caps are not readily available, we designed a custom cap using 3D computer-aided modeling. The outstanding advantage of computer-aided modeling is the ability to virtually assemble all components of the setup together and to check for possible clearance issues and design pitfalls prior to manufacturing. We have developed a concept optimized for photoredox applications that is designed for compatibility with standard glass reaction vessels (Fig. 2A). The designed photoreactor was fabricated using a commonly available FDM 3D printer (Fig. 2B).
The reactor includes an efficient twist-lock LED mount that allows the LED light source to be changed easily. The bottom part can house a range of common glass vials available in the lab, and the presence of an O-ring ensures a tight fit with the reaction vessel. A detailed description of the reactor and the 3D model are provided in the ESI.† The developed model can be directly printed on a regular 3D printer in approximately 30 minutes and requires only 6 grams of the plastic source material (<$1 cost). The developed photoreactor was totally compatible with common magnetic stirrers and allowed for very good temperature stabilization at 25 ± 0.5 °C (Fig. 1C). The ability to maintain stable experimental conditions (e.g., temperature and light intensity) drastically improves the selectivity and reproducibility of photochemical reactions. An array of the custom-built photoreactors allowed us to execute a study of the substrate scope involving various substituents in a parallel fashion (Scheme 3). Four important advantages deserve particular attention: (i) the catalytic system showed excellent performance for various aryl thiols;9 (ii) excellent stereoselectivity in the range of 60:1–25:1 was achieved; (iii) complete regioselectivity was maintained and the formation of another regioisomer (7a) was not observed; and (iv) the hydroxyl group remained intact during the reaction, which is a necessary prerequisite to access the diene backbone after dehydration (Scheme 1). The developed synthetic approach was tolerant toward electronic and steric effects of the substituents in the thiol moiety (Scheme 3). Even for thiols containing strongly electron-withdrawing substituents, such as CF3 or COOMe, the desired products were formed in very high yield and high selectivity (i.e., 3e, 3g, 3h). We also tested aliphatic thiols in this reaction (R1 = Alk); however, significantly lower selectivity was observed (<10:1). An important factor is the structure of the alkyne, where steric effect played a key role in obtaining high selectivity (see ESI†). Amazingly, high selectivity was observed for the alkynes bearing α-substituted carbon atom, which is required to implement the synthetic methodology proposed in the present study (Scheme 1). For the studied class of alkynes the corresponding products 3a–3m were synthesized in good to high yields and excellent selectivity (Scheme 3) including sterically hindered alkynes, where the products 3n–3p were formed in good yields (89–96%) and high selectivity (35:1–40:1).
Scheme 3 The scope of the developed photocatalytic thiol–yne click reactiona. (a Isolated yields are given in parentheses, reaction time – 5 h. b Reaction time – 10 h. c Reaction time – 20 h). |
A plausible mechanism for the photoredox thiol–yne click reaction is presented in Scheme 4A.13,15 A photoexcited molecule of Eosin Y (E*) undergoes oxidative quenching, furnishing a radical cation of arylthiol. Pyridine abstracts a proton from this species, yielding thiyl radicals and preventing side reactions of ArSH˙+. In the next step, ArS˙ is involved in the radical addition to the alkyne, giving the desired product 3 and regenerating ArS˙ radicals. Within the mechanism the E-species of Eosin Y are regenerated upon interaction with molecular oxygen from ambient air. According to thermodynamic properties single electron oxidation of benzenethiol by excited state of Eosin Y is a feasible process: the potential EE*/E− = 1.18 V vs. SCE is much higher as compared to EPhSH/PhSH+ ≈ 0.95 V vs. SCE.16
Scheme 4 The proposed mechanism (A) for the Eosin Y mediated thiol–yne photoredox coupling (Eosin Y is denoted with E), plausible origins of reaction regioselectivity (B) and stereoselectivity (C). |
Rather different stability of the primary and secondary intermediate radical species governs high regioselectivity in the studied reaction (Scheme 4B). According to DFT calculations secondary radical is more stable by >8 kcal mol−1 compared to primary radical (see ESI†). In total agreement with relative stability of the radical species linear (anti-Markovnikov type) products 3 were formed in the reactions, whereas formation of branched (Markovnikov type) products was not observed.
Steric effect of the substituent R provides the necessary control for stereoselectivity in the studied transformation (Scheme 4C). Decreasing steric bulk resulted in lower reaction selectivity or non-selective transformation (see ESI†). The presence of OH group and two other substituents at the α-carbon atom in the developed concept (Scheme 1) perfectly matches the structure of the alkyne towards getting a high stereoselectivity.
Radical nature of the studied process was confirmed by performing a control experiment using a radical trap. Indeed, addition of γ-terpinene suppressed the reaction between the thiol and alkyne. Several other control experiments were also carried out to confirm the proposed mechanism and to demonstrate regeneration of the dye in the presence of oxygen (see ESI†).
Finally, as a proof of concept, we have prepared the target diene 8a using the industrially available starting materials acetylene, acetone and benzenethiol (Scheme 5). In the first step, alkyne 1a was prepared according to the published procedure.17 Alkyne 1a was converted to vinyl sulfide 3a using the developed photochemical protocol. Dehydration of 3a under mild conditions furnished diene 8a in 94% isolated yield. Thus, a demanding S-functionalized 1,3-diene was prepared starting from simple precursors through a sequence of atom-economic addition reactions with the only release of water (Scheme 5).
An efficient photocatalytic system was created using a combination of Eosin Y and hexane as solvent. Utilization of the “saturation feedback” approach described here to maintain the optimal concentration of the catalyst may substantially facilitate development of a variety of other photocatalytic transformations.
Formation of double addition products was observed in a few studied cases at a trace level. Purification was easily performed using a regular flash chromatography as described below.
High-resolution mass spectra were recorded on a Bruker maXis Q-TOF instrument (Bruker Daltonik GmbH, Bremen, Germany) equipped with electrospray ionization (ESI) ion source. The measurements were performed in a positive (+MS; +MS/MS) ion mode (HV capillary: 4500 V; HV end plate offset: −500 V) with a scan range m/z: 50–3000. External calibration of the mass spectrometer was performed using an electrospray calibrant solution (Fluka). A direct syringe injection was used for all of the analyzed solutions in MeCN or DCM (flow rate: 3 μL min−1). Nitrogen was used as the nebulizer gas (0.4 bar), dry gas (4.0 L min−1) and collision gas for all of the MS/MS analyses and experiments; the dry temperature was set at 180 °C. All of the recorded spectra were processed using the Bruker DataAnalysis 4.0 software package.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c6sc02132h |
This journal is © The Royal Society of Chemistry 2016 |