Jean-Philippe R.
Chauvin
,
Evan A.
Haidasz
,
Markus
Griesser
and
Derek A.
Pratt
*
Department of Chemistry and Biomolecular Sciences, University of Ottawa, 10 Marie Curie Pvt., Ottawa, Ontario, Canada. E-mail: dpratt@uottawa.ca; Fax: +1-613-562-5170; Tel: +1-613-562-5800 ext. 2119
First published on 23rd June 2016
Polysulfides are important additives to a wide variety of industrial and consumer products and figure prominently in the chemistry and biology of garlic and related medicinal plants. Although their antioxidant activity in biological contexts has received only recent attention, they have long been ascribed ‘secondary antioxidant’ activity in the chemical industry, where they are believed to react with the hydroperoxide products of autoxidation to slow the auto-initiation of new autoxidative chain reactions. Herein we demonstrate that the initial products of trisulfide oxidation, trisulfide-1-oxides, are surprisingly reactive ‘primary antioxidants’, which slow autoxidation by trapping chain-carrying peroxyl radicals. In fact, they do so with rate constants (k = 1–2 × 104 M−1 s−1 at 37 °C) that are indistinguishable from those of the most common primary antioxidants, i.e. hindered phenols, such as BHT. Experimental and computational studies demonstrate that the reaction occurs by a concerted bimolecular homolytic substitution (SH2), liberating a perthiyl radical – which is ca. 16 kcal mol−1 more stable than a peroxyl radical. Interestingly, the (electrophilic) peroxyl radical nominally reacts as a nucleophile – attacking the of the trisulfide-1-oxide – a role hitherto suspected only for its reactions at metal atoms. The analogous reactions of trisulfides are readily reversible and not kinetically competent to inhibit hydrocarbon autoxidation, consistent with the longstanding view that organosulfur compounds must be oxidized to afford significant antioxidant activity. The reactivity of trisulfides and their oxides are contrasted with what is known of their shorter cousins and predictions are made and tested with regards to the reactivity of higher polysulfides and their 1-oxides – the insights from which may be exploited in the design of future antioxidants.
The antioxidant mechanisms of organosulfur compounds are often presented as complex. However, it is generally acknowledged that they must first be oxidized to render them effective.4 Organosulfur compounds are ascribed ‘secondary antioxidant’ activity since it is believed that they slow the rate of initiation (eqn (1)) by decomposing hydroperoxides.5 Two mechanisms are particularly important in this context: the direct reduction of hydroperoxides (eqn (5)) and the production of Brønsted or Lewis acids, which catalytically decompose hydroperoxides (eqn (6)) (Scheme 2).
Secondary antioxidants can be contrasted with ‘primary antioxidants’, which inhibit autoxidation directly via reaction with chain-propagating peroxyl radicals.7,8 The most common examples of primary antioxidants - generally referred to as radical-trapping antioxidants (RTAs) - are phenols and diarylamines.6
Organosulfur compounds may also act as primary antioxidants.7,9 Koelewijn and Berger10 showed that sulfides, upon oxidation to sulfoxides, undergo Cope-type elimination to yield a sulfenic acid (eqn (7)), which they surmised would undergo fast reactions with peroxyl radicals (eqn (8)). Since sulfenic acids are transient species that rapidly undergo self-reaction to yield thiosulfinates, they were unable to directly determine the kinetics of reaction (8), but estimated a rate constant of ca. 107 M−1 s−1 based on inhibited autoxidations of tetralin with in situ formation of t-BuSOH from thermolysis of di-tert-butyl sulfoxide at 60 °C.10
(7) |
(8) |
Using a persistent sulfenic acid, 9-triptycenesulfenic acid,11 we recently determined the kinetics and thermodynamics of the reaction of a sulfenic acid with peroxyl radicals directly. The weak O–H bond in the sulfenic acid (71.9 kcal mol−1)12 gives way to highly favourable reaction thermodynamics with peroxyl radicals (ca. 14 kcal mol−1), and the presence of the sulfur atom α to the reactive O–H drives a very fast proton-coupled electron transfer reaction with peroxyl radicals (k = 3 × 106 M−1 s−1) – despite the steric demand of the triptycenyl moiety.13,14
Our studies of the radical chemistry of sulfenic acids were motivated by the widely reported antioxidant activity of allicin, the odorous thiosulfinate found in garlic, and petivericin, the analogous thiosulfinate from the medicinal plant Petiveria alliacea. We demonstrated15,16 that the antioxidant activity of both thiosulfinates was dependent on the Cope-type elimination of a sulfenic acid, which proceeds readily for both compounds at ambient temperature owing to the activated β C–H bond.17
(9) |
(10) |
Since trisulfides and their oxides are among the most prevalent organosulfur compounds in Allium species (e.g., diallyltrisulfide and diallyltrisulfide-1-oxide from garlic)18,19 and are predominant among the mixtures of sulfurized materials added to protect petroleum-derived products from autoxidation,4,20 we wondered if they would possess ‘primary antioxidant’ reactivity analogous to that of hindered sulfoxides and activated thiosulfinates. Herein we report an investigation of the RTA activities of some trisulfides and their 1-oxides in an attempt to extend the foregoing knowledge to a more comprehensive view of the primary antioxidant activity of polysulfides and their 1-oxides, in general.21
The data in Fig. 1A and B clearly demonstrate the ability of both trisulfide-1-oxides to retard the oxidation – and to a similar extent. From the rates of the retarded reactions, and assuming a stoichiometric factor of n = 1 (vide infra), the inhibition rate constants for BnS(O)SSBn and t-BuS(O)SSt-Bu were calculated using eqn (11) to be kinh = (1.5 ± 0.4) × 104 M−1 s−1 and (1.1 ± 0.3) × 104 M−1 s−1, respectively. The corresponding disulfides and trisulfides had no effect on the rate of PBD-BODIPY oxidation.
(11) |
The lack of clear inhibited periods for the trisulfide-1-oxides in the foregoing styrene autoxidations precluded a determination of the stoichiometry for their reaction with peroxyl radicals. Therefore, co-autoxidations of cumene and STY-BODIPY were also carried out. These less oxidizable substrates generally provide greater resolution between inhibited and uninhibited phases of the autoxidation.26 The results are shown for t-BuS(O)SSt-Bu and BnS(O)SSBn in Fig. 1C and D, respectively.
The STY-BODIPY/cumene co-autoxidations were less well inhibited by the trisulfide-1-oxides compared to the PBD-BODIPY/styrene co-autoxidations; in fact, t-BuS(O)SSt-Bu was unable to inhibit the autoxidation at all, displaying instead a slight, but reproducible, acceleration of the autoxidation.27 This was particularly surprising given the greater propagation rate constants of PBD-BODIPY (2720 M−1 s−1) and styrene (41 M−1 s−1) compared to STY-BODIPY (141 M−1 s−1) and cumene (0.34 M−1 s−1). Kinetic analysis of the initial rates of the BnS(O)SSBn-inhibited autoxidations (i.e.eqn (11)) afforded kinh = (2.4 ± 0.6) × 103 M−1 s−1; ca. 6-fold smaller than the rate constant derived from the styrene co-autoxidations. Nevertheless, the presence of a distinct inhibited period followed by reaction progress at the same rate as in the uninhibited reaction enabled the determination of the stoichiometry from the length of the inhibited period, τ (as in eqn (12)). The result was n = 0.9 ± 0.2, thereby validating the assumption made in the styrene autoxidations (vide supra).
(12) |
To probe whether the benzylic H-atoms in BnS(O)SSBn play a role in its radical-trapping antioxidant activity, d4-BnS(O)SSBn was synthesized in a manner similar to that used to prepare d4-BnS(O)SBn in our previous work (see Experimental section),13 and its RTA activity was evaluated in styrene/PBD-BODIPY co-autoxidations. Experiments were also carried out wherein a small volume of a protic/deuteric solvent was added to determine if an exchangeable H-atom/D-atom is involved in the radical-trapping reaction. The results are given in Table 1 (see ESI† for the inhibited autoxidation traces). For comparison, kH/kD values of 16 and 18 were determined from d4-BnS(O)SBn-inhibited autoxidations carried out in the presence of D2O.13
Trisulfide-1-oxide/additive | k inh (M−1 s−1) | k H/kD |
---|---|---|
BnS(O)SSBn | (1.5 ± 0.4) × 104 | — |
BnS(O)SSBn/MeOH (1%) | (1.5 ± 0.4) × 104 | — |
BnS(O)SSBn/MeOD (1%) | (1.3 ± 0.4) × 104 | 1.2 |
d 4-BnS(O)SSBn/MeOD (1%) | (1.1 ± 0.2) × 104 | 1.4 |
Analogous co-autoxidations inhibited by t-BuS(O)SSt-Bu in the presence of either 1% MeOH or MeOD yielded indistinguishable results from co-autoxidations carried out in their absence.
CBS-QB3 calculations28 were carried out on model compounds wherein the substituents on the trisulfide-1-oxide and peroxyl radical (R and R′, respectively) were methyl groups. Despite extensive effort, a minimum energy structure for the intermediate in the step-wise reaction (eqn (13)) could not be located. However, transition states for both concerted homolytic substitutions were readily located, and are shown in Fig. 2A. The structures are 15.1 and 18.5 kcal mol−1, respectively, higher in free energy than the separated reactants. Application of transition state theory affords rate constants of 3.8 × 103 and 14 M−1 s−1, respectively – the former in good agreement with the experimental data for BnS(O)SSBn of (1.5 ± 0.4) × 104. Replacement of the methyl substituents on the trisulfide-1-oxide and methylperoxyl radical with t-butyl groups increases the barrier by 3.7 kcal mol−1 – consistent with the fact that t-BuS(O)SSt-Bu does not inhibit cumene autoxidation.29
Both substitutions are predicted to be thermodynamically favourable: ΔG0 = −9.3 kcal mol−1 for reaction at S1 (the sulfinyl sulfur) and ΔG0 = −7.1 kcal mol−1 for reaction at S2. Much of the energetic benefit derives from exchange of the peroxyl radical for either of the more stabilized perthiyl or sulfinyl radicals – which is clear when one considers the X–H BDEs (calculated by CBS-QB3) in MeSS–H (70.8 kcal mol−1) and MeSO–H (68.4 kcal mol−1) compared to MeOO–H (86.2 kcal mol−1) – as well as the stronger S–O bonds in the products (40.1 and 37.2 kcal mol−1 in MeOOS(O)Me and MeOOSSMe compared to 30.6 kcal mol−1 for the S1–S2 bond in MeS(O)SSMe). In the reaction at S1, the sulfinyl S–O bond length (1.480 Å) contracts ever so slightly from the starting material (1.487 Å), whereas in the reaction at S2, the sulfinyl S–O lengthens slightly (1.496 Å) on its way to becoming a free sulfinyl radical (1.511 Å). Consideration of the transition state structure suggests that the lone pair on the S1 sulfur does not participate directly in the reaction. In fact, the electronic structure of the transition state can essentially be viewed as interacting peroxyl, sulfinyl and perthiyl radicals (Fig. 3).
This view is reinforced by the results of natural bond orbital (NBO) analyses30 of the corresponding wavefunction, which is dominated by peroxyl π* (SOMO) → and perthiyl π* (SOMO) → interactions – worth a total of 73.5 kcal mol−1. Interestingly, the NBO analyses also reveal strong interactions between the lone pairs on the sulfinyl oxygen and the and orbitals – worth a total of 60.2 kcal mol−1 – consistent with the fact that the transition state is stabilized by oxidation of S1.
For comparison, the analogous transition states for the reaction of a trisulfide with a peroxyl radical were determined and are shown in Fig. 2B. These structures are 18.4 and 25.7 kcal mol−1, respectively, higher in energy than the separated reactants. The corresponding rate constants determined by transition state theory are 17 and 1.2 × 10−4 M−1 s−1, respectively – consistent with the fact that no inhibition of styrene or cumene autoxidation was observed in the presence of the trisulfides. Both of these reactions are endergonic, with reaction at S1 being far less unfavourable (ΔG0 = +1.5 kcal mol−1), than that at S2 (ΔG0 = +14.8 kcal mol−1). This is largely due to the greater stability of the perthiyl radical leaving group in the former reaction relative to the thiyl radical leaving group in the latter reaction (the CBS-QB3-calculated MeS–H and MeSS–H BDEs are 87.1 and 70.8 kcal mol−1, respectively).
Although analogous transition state structures could not be located for the reaction of a disulfide with a peroxyl radical, transition state structures were again readily located for the reaction of a peroxyl radical with a thiosulfinate, and are shown in Fig. 2C. These structures are 13.8 and 17.6 kcal mol−1, respectively, higher in energy than the separated reactants. Interestingly, the barrier for reaction at S1 is even lower than that determined for the reaction of peroxyl radicals with the trisulfide-1-oxide. However, this reaction is endergonic by 3.0 kcal mol−1 – implying that it is readily reversible – while the reaction of the trisulfide-1-oxide is exergonic by 9.3 kcal mol−1. This difference arises largely since the reaction of the thiosulfinate produces a thiyl radical, which is far less stable than the perthiyl radical (by 16.3 kcal mol−1, vide supra). Although the reaction of the thiosulfinate at S2 is significantly exergonic (ΔG0 = −8.1 kcal mol−1), it has a higher barrier. The rate constant calculated for substitution at S2 is 61 M−1 s−1, in reasonable agreement with rate constants determined experimentally for unactivated thiosulfinates (e.g. n-propyl n-propanethiosulfinate, for which kinh = (244 ± 31) M−1 s−1).31
Fig. 4 Thermally-initiated (AIBN, 6 mM) co-autoxidation of cumene (3.6 M) and STY-BODIPY (10 μM) at 37 °C in chlorobenzene in the presence of various concentrations of BnSSH. |
The stoichiometry of the reaction of BnSSH with peroxyl radicals was determined to be n = 1.0 ± 0.2 from this data, consistent with a mechanism involving initial H-atom transfer from the hydropersulfide to a chain-carrying peroxyl radical and then no involvement of the resultant perthiyl radical in the reaction. It should be noted that hydropersulfides are evidently very potent radical-trapping antioxidants – similar in reactivity to α-tocopherol, Nature's premier lipid-soluble radical-trapping antioxidant33,34 – a result we will follow up on in subsequent work.
To provide insight on these possibilities, the reactivity of perthiyl radicals towards oxygen was investigated in chlorobenzene by laser flash photolysis. Di-tert-butyl tetrasulfide was used as a model compound, since it is known to yield a pair of perthiyl radicals upon UV irradiation.36
(16) |
Photolysis of the tetrasulfide at 308 nm yielded a transient species with a pronounced absorption at 375 nm corresponding to the perthiyl radical (Fig. 5A). This transient absorption decayed rapidly (Fig. 5B) with concomitant reformation of the tetrasulfide at 340 nm (Fig. 5A).
The second order rate constant for the recombination of perthiyl radicals to the tetrasulfide was determined to be (6.0 ± 0.5) × 109 M−1 s−1 at 25 °C (assuming ε390 nm = 1600 M−1 cm−1 based on pulse radiolysis studies of similar compounds35,37,38). This is ca. 4-fold larger than the reported values in water (1.5 and 1.9 × 109 M−1 s−1, respectively). Importantly, as is clear in Fig. 5B, no difference in the decay kinetics of the perthiyl radical could be detected in the presence or absence of O2.
We also carried out a series of computations to probe the plausibility of the reaction of a perthiyl radical with O2 (eqn (17)). It was not possible to find a bound perthiyl-O2 adduct using the CBS-QB3 approach that we employed above (where geometries are obtained at the B3LYP/CBSB7 level of theory). However, when the calculations were carried out with basis sets that included diffuse functions on the heavy atoms, bound structures were located. The corresponding CBS-QB3(+)39 ΔG0 was 12.9 kcal mol−1 with an associated barrier of ΔG‡ = 14.2 kcal mol−1 – consistent with the lack of reactivity determined experimentally.
(17) |
(18) |
While a transition state for this process was readily located in CBS-QB3 calculations on the corresponding allylic trisulfide-1-oxide (the benzyl groups were exchanged for allyl groups for computational expediency), the structure was a prohibitive 40.9 kcal mol−1 higher in energy than the starting material. For comparison, the transition state structure for Cope-type elimination of 2-propenesulfenic acid from allicin is calculated to have ΔH‡ = 19.5 kcal mol−1 (CBS-QB3), in good agreement with experimental observations.15,16
Of course, the fact that t-BuS(O)SSt-Bu reacts with styrylperoxyl radicals with essentially the same rate constant as BnS(O)SSBn implies that the mechanism involves direct reaction at the trisulfide-1-oxide moiety. We initially surmised that this could take place by an addition/fragmentation mechanism, where the peroxyl radical would add to a lone pair on the sulfur atom to form an intermediate sulfur-centered radical that would be capto-datively stabilized by the sulfur atom on one side and the sulfinyl group on the other (eqn (13)). Subsequent α-cleavage would yield either of two potential pairs of formal substitution products. However, computational efforts to provide evidence for this intermediate were unsuccessful.
Since computations indicated that the S(O)–SS bonds in trisulfide-1-oxides are weak (i.e. 29.8 kcal mol−1 in t-BuS(O)SSt-Bu by CBS-QB3 – see ESI†), a concerted substitution was considered next. This seemed unlikely since it requires that the peroxyl radical serve nominally as the nucleophile. Nevertheless, transition state structures were readily located for substitution at each of the sulfinyl sulfur atom (S1) and S2. Substitution at S1 was predicted to take place with a lower barrier (15.1 kcal mol−1vs. 18.5 kcal mol−1 for substitution at S2) and the corresponding rate constant obtained from application of transition state theory was in good agreement with our experiments. This mechanism is also consistent with the lack of deuterium kinetic isotope effects on peroxyl radical-trapping by either t-BuS(O)SSt-Bu (kH/kD = 1.0) or BnS(O)SSBn (kH/kD = 1.4). This is in sharp contrast with the large KIEs observed for petivericin (kH/kD = 16 or 18.2, depending on experimental approach) – whose mechanism involves two isotope-sensitive steps: C–H bond cleavage in the Cope-type elimination and O–H bond cleavage in the formal H-atom transfer from the sulfenic acid to the peroxyl radical.13
The rates of reactions of peroxyl radicals with RTAs are generally independent of the structure of the peroxyl radical; that is, inhibited autoxidations of styrene or cumene, where the chain reaction is carried by styrylperoxyl or cumylperoxyl radicals, respectively, usually yield the same inhibition rate constant.40 The fact that the trisulfide-1-oxides react at different rates with these peroxyl radicals, and that the steric demand of the substituents on the trisulfide-1-oxide have a greater impact on the rate when the peroxyl radical is also hindered (cumylperoxyl), further support that these reactions take place by a homolytic substitution mechanism at the sulfinyl sulfur atom.
Thus, the RTA activity of the trisulfide-1-oxides in organic solution can be ascribed to the reactions in Scheme 5. The substitution products are a perthiyl radical and a peroxysulfinate ester (eqn (19)). Interestingly, in contrast with the literature precedent (in aqueous solution), our flash photolysis experiments indicate that the perthiyl radical rapidly combines with another of itself to form a tetrasulfide (eqn (20)) even in the presence of O2. The peroxysulfinate ester is the same product that is formed upon reaction of a sulfinyl radical with a peroxyl radical, and is believed to rapidly rearrange to a sulfonate ester (eqn (21)) – possibly by O–O cleavage and in-cage recombination.13,16 This reaction mechanism is consistent with all of the foregoing data, including the fact that a trisulfide-1-oxide traps a single peroxyl radical under ambient conditions, unlike activated thiosulfinates and sulfoxides, which trap 2.
The reactions of peroxyl radicals at metal centers (e.g. magnesium, zinc, aluminum and tin) have been proposed to occur via an SH2 mechanism,42 but to the best of our knowledge, this mechanism does not seem to be operative on non-metal centers. Substitution of an alkyl substituent for a peroxyl substituent is commonly invoked in the autoxidation of trialkylboranes (e.g. in the common Et3B/O2 radical initiator system),43 but this is likely to be mechanistically distinct owing to the initial formation of a Lewis acid–base complex between a lone-pair on the peroxyl radical and the vacant boron 2p orbital that precedes homolytic boron–carbon bond cleavage.44 The substitutions of peroxyl radicals at centres that have non-bonded electron pairs, such as in phosphines and sulfides, are believed to proceed via addition–fragmentation sequences in non-polar solvents45 and by electron transfer in polar solvents when the peroxyl is highly electrophilic (i.e. halogenated methylperoxyls),46,47 respectively.
In light of the mechanism in Scheme 5, the foregoing investigations were extended to include the next polysulfide-1-oxide. Initial CBS-QB3 calculations predicted ΔG0 = −8.2 kcal mol−1 for MeOO˙ + MeS(O)SSSMe – little different from the −9.3 kcal mol−1 calculated for MeOO˙ + MeS(O)SSMe. This is explained simply on the basis that the leaving groups (MeSSS˙ and MeSS˙) are similarly stabilized (CBS-QB3 BDEs in MeSS–H and MeSSS–H are 70.8 and 72.7 kcal mol−1, respectively). Moreover, the transition state for the SH2 reaction of the tetrasulfide-1-oxide was readily located (cf.Fig. 6), and its associated ΔG‡ = 14.7 kcal mol−1 was essentially the same as that which was calculated for the corresponding trisulfide-1-oxide (15.1 kcal mol−1).
This reactivity was subsequently confirmed in styrene autoxidations inhibited by t-BuS(O)SSSt-Bu, which yielded data that were indistinguishable from those wherein t-BuS(O)SSt-Bu was used as the inhibitor of (cf.Fig. 7), and characterized by a kinh = (1.0 ± 0.3) × 104 M−1 s−1. Although no stoichiometric information could be gleaned from the styrene autoxidations inhibited by t-BuS(O)SSSt-Bu (as was the case with t-BuS(O)SSt-Bu, vide supra), it is highly likely based on the foregoing that it also traps a single peroxyl radical by a mechanism analogous to that shown in Scheme 5. Similarly to the trisulfide, the tetrasulfide displayed no such RTA activity.
Fig. 7 Thermally-initiated (AIBN, 6 mM) co-autoxidation of styrene (4.4 M) and PBD-BODIPY (10 μM) at 37 °C in chlorobenzene in the presence of various concentrations of t-BuS(O)SSSt-Bu. |
It seems reasonable to suggest that the reactivity of trisulfide-1-oxides and tetrasulfide-1-oxides extends to higher polysulfide-1-oxides, since the S–S bond strength in higher polysulfides is essentially independent of the number of sulfur atoms.48 The generality of this reactivity is in sharp contrast to that of the lower thiosulfinates and sulfoxides, whose activities require appropriate substitution to promote Cope-type elimination of a sulfenic acid.
Footnote |
† Electronic supplementary information (ESI) available: NMR spectra of new compounds, KIE experiments, details of LFP experiments and optimized geometries and energies for computational results. See DOI: 10.1039/c6sc01434h |
This journal is © The Royal Society of Chemistry 2016 |