Abstract

The methionine–iodine reaction was reinvestigated spectrophotometrically in detail monitoring the absorbance belonging to the isosbestic point of iodine at 468 nm, at T = 25.0 ± 0.1 °C, and at 0.5 M ionic strength in buffered acidic medium. The stoichiometric ratio of the reactants was determined to be 1:1 producing methionine sulfoxide as the lone sulfur-containing product. The direct reaction between methionine and iodine was found to be relatively rapid in the absence of initially added iodide ion, and it can conveniently be followed by the stopped-flow technique. Reduction of iodine eventually leads to the formation of iodide ion that inhibits the reaction making the whole system autoinhibitory with respect to the halide ion. We have also shown that this inhibitory effect appears quite prominently, and addition of iodide ion in the millimole concentration range may result in a rate law where the formal kinetic order of this species becomes −2. In contrast to this, hydrogen ion has just a mildly inhibitory effect giving rise to the fact that iodine is the kinetically active species in the system but not hypoiodous acid. The surprisingly complex kinetics of this simple reaction may readily be interpreted via the initiating rapidly established iodonium-transfer process between the reactants followed by the subsequent hydrolytic decomposition of the short-lived iodinated methionine. A seven-step kinetic model to be able to describe the most important characteristics of the measured kinetic curves is established and discussed in detail.
Introduction
Sulfur-containing amino acids are not only important sources of sulfur nutrients in humans and mammals1 but also play an important role in various biochemical processes such as transformation and synthesis of proteins,2 immunity,3,4 as well as oxidative stress resistance.5−7 It is generally considered that redox reaction balance of many sulfur-containing amino acids is closely associated with cardiovascular disease, neuropsychiatric disorder, neurogenic diseases, renalischemia, liver failure, diabetes, cancer, and aging.1,6,8−12 The sulfur-containing amino acids supplementation may readily scavenge biological reactive oxidants in vivo through their redox reactions to protect the stability and activity of other essential amino acids in proteins reducing the damage to cell membrane and DNA caused by oxidative stress and, in turn, incidence of these diseases.
Methionine (Met), as one of two essential sulfur-containing amino acids, may be obtained only from the human diet. Met is not only a precursor in protein synthesis but also participates in many biochemical processes,3,8,13,14 such as glycogen and d-glucose formation, production of S-adenosylmethionine and Succinyl-CoA, biosynthesis of homocysteine, cysteine, and glutathione, metabolism of phosphatidylcholine and phospholipids, as well as cellular and DNA methylation. In addition, it is found that Met in proteins is highly susceptible to oxidation under oxidative stress.15−19 As an antioxidant defense system, Met oxidation participates in regulation of protein stability20 and cellular viability21 through its own oxidation: Met is oxidized to form methionine sulfoxide(MetSO) by adding oxygen to its sulfur atom in the physiological environment. MetSO produced may easily be reduced back to Met by thioredoxin-dependent enzymes under catalysis of methionine sulfoxide reductase.7,22 The impairment of this regulation is associated with many diseases such as lung disease,23 cancer,24 neurodegeneration (Alzheimer’s disease),25 and cardiovascular and cerebrovascular disease.26,27 However, the regulation functions of methionine as an antioxidant are still not fully explored. In order to understand the relationship between its oxidation process and biological regulation function, it is crucial to perform further investigations on the mechanism of methionine oxidation.
Sulfur-containing amino acids have three possible coordination sites including oxygen, nitrogen, and sulfur parts, and among them, the sulfur site is believed to be the most likely to be attacked by electrophilic agents due to its abundant electron density. Several investigations on the kinetics and mechanism of oxidation of methionine by different biological oxidants have been reported with numerous oxidizing agents like metal ions,28−30 halogen-containing inorganic oxidants,31−33 hydrogen peroxide,34,35 hydroxyl radicals,36 and halogenated organic oxidants.13,37−39 Even though most of these studies showed that the reaction is first order with respect to both methionine and the oxidant and methionine is oxidized to methionine sulfoxide as a final product, transient species during the course of reaction and their pathways are still not completely revealed. Taking the oxidation of methionine with halogen-containing oxidants as examples, the studies31,32,37,39 showed that the methionine was first halogenated to give halosulfonium cation followed by the formation of methionine sulfoxide through the sequence of fast reactions. However, the reaction pathways from halosulfonium cation to methionine sulfoxide are different: Armesto,31 Chikwana,32 and Goyal39 showed methionine sulfoxide is formed by the hydrolysis of halosulfonium cation, while Gangwani37 indicated that the halosulfonium cation is highly solvated to give final product. In addition, the earlier results give evidence for a tetracoordinated sulfurane intermediate and reaction product, cyclic sulfinine dehydromethionine.40 Recently, Diculescu41 pointed out that methionine oxidation leads to methionine sulfoxide by hydrolysis of dehydromethionine intermediate. Instead of product, methionine sulfoxide could be an intermediate to react further with a second oxidant molecule to form a complex yielding the end-product, sulfone, by a series of fast steps.13 Moreover, a theoretical study on the oxidation of methionine by hydroxyl radicals predicted that α-aminoalkyl radical is the intermediate proceeding to the final product, thioether aldehyde.36 The important role of methionine in biochemical processes highlighted above as well as its diverse transformation to various sulfur-containing intermediates and products awaits for comprehensive and detailed kinetic studies to unravel the intimate nature of this essential amino acid to redox processes.
Experimental Section
Materials
All chemicals including iodine, dl-methionine, phosphoric acid, sodium dihydrogen phosphate, potassium iodide, and sodium perchlorate were of the commercially available highest purity and used without further purification. The corresponding stock solutions were prepared from twice ion-exchanged and two times atmospherically distilled water over potassium permanganate to avoid any organic or inorganic impurities originating from the exchange resin. The pH of buffer solutions was adjusted to be in the range of 1.60 and 2.60 by using phosphoric acid and dihydrogen phosphate taking the pKa of phosphoric acid to be 1.8.42 The pKa1 of methionine was also taken into consideration as 2.28.42 The concentration of dihydrogen phosphate was kept constant at 0.3 M, and the ionic strength was kept at 0.5 M in all reactions by adding the necessary amount of sodium perchlorate as the background electrolyte. The methionine and potassium iodide solutions were freshly prepared before each experiment. The concentration of iodine in the stock solution was determined with iodometric method and checked with a UV–vis spectrometer as well before each measurement. The temperature of reaction cell was maintained at 25.0 ± 0.1 °C by thermostatting the cell holder with a water-circulating bath. Some experiments were performed in the absence of initially added iodide ion; however, [I–]0 in the majority of the kinetic measurements was kept constant at 0.003 M, except those ones where the effect of initially added iodide ion was investigated. Initial concentration of iodine and methionine were varied in the range of 0.120–25.01 mM and 0.067–0.872 mM, respectively
Methods and Instrumentation
The kinetic runs in the presence of initially added iodide ion were monitored by an Analytik Jena Specord S600 diode array spectrophotometers in the wavelength range of 400–900 nm. The deuterium lamp of the photometer was switched off during the whole course of experiments to avoid any undesired photochemically induced side effect of the UV radiation. The reaction was carried out in a standard quartz cuvette having a 1 cm optical path and equipped with a magnetic stirrer bar and a closely sealed Teflon cap. The buffer solution followed by the iodide and iodine solutions were delivered into the cuvette from a pipet first, and the spectrum of the solution was always recorded before initiation of the reaction to determine the exact initial iodine concentration. The reaction was then triggered by rapidly adding a necessary amount of methionine stock solution. Several repeated experiments have also been carried out indicating a good reproducibility of the kinetic measurement (see Figure S1 in the Supporting Information).
The reaction without initially added iodide ion at high excess of methionine was found to be too fast to be studied by S600 diode array spectrophotometer. Therefore, at these conditions the reaction was followed at 468 nm wavelength by an Applied Photophysics SX20 stopped-flow instrument equipped with a monochromator. The optical path was set to 1 cm, and the dead-time of the stopped-flow instrument was determined to be 1.3 ms by a standard methodology as described previously.43 Each single kinetic run was repeated five times, and then the average of those runs were used for data evaluation.
The stoichiometric studies of this reaction were carried out in an excess of iodine with and without initially added iodide. The concentration of iodine at the end of reaction was calculated from the absorbance determined by visible spectroscopy when reaction was completely finished. The 1H NMR spectra of end products and dl-methionine were confirmed by a Bruker Avance III 500 spectrometer at 500 MHz. 1H spectra were recorded in D2O, and the chemical shifts are reported in ppm relative to solvent residual peak (4.79 ppm 1H).44
Data Treatment
Because iodine and triiodide ion were found to be the only absorbing species in the visible region, the 468 nm wavelength, which is the isosbestic point of iodine and triiodide ion system, was selected for the data evaluation of the kinetic parameter performed by the comprehensive program package ChemMech/Zita.45 During the whole calculation process pH = −log[H+] is considered and the molar absorbance of iodine and triiodide ion was set to be 750 M–1cm–1.46 Since each experimental kinetic curve originally contained more than 500 absorbance–time data pairs, it was necessary to reduce the number of data points at about 60–80 in each runs to avoid the unnecessarily long and time-consuming evaluation process. A total number of almost 11 500 experimental data obtained from 151 kinetic curves were used for simultaneous data evaluation procedure. A relative fitting method has been chosen to minimize the average deviation between the measured and calculated data. The criterion was that the average deviation approached 1.5%, which is quite close to the experimentally achievable limit of error. The initial conditions can be seen in Table S1 in the Supporting Information.
Results
Stoichiometry
Any reliable kinetic studies should begin with unraveling the stoichiometry of the given process at the experimental condition studied. A suitable and conceivable method seems to be visible-spectroscopy for determination of the consumed iodine/methionine ratio (SR defined as ([I2]0 – [I2]∞)/[Met]0) in excess of iodine. Table 1 displays some examples of the calculated stoichiometric ratio; the rest of them may be found in Table S2 of the Supporting Information. As it can easily be seen, SR values indicate a stoichiometric ratio to be pretty close to 1.0 within the limit of experimental error. It appears to suggest that the following equation describes the stoichiometry of methionine–iodine reaction:
Table 1. Experimental (SR) Defined as ([I2]0 – [I2]∞)/[Met]0 in Excess of Iodine with and without Initially Added Iodide Ion.
| [I2]0/mM | [Met]0/mM | [I–]0/mM | pH | A∞ at 468 nm | SR |
|---|---|---|---|---|---|
| 0.938 | 0.399 | 0.0 | 1.85 | 0.4135 | 0.97 |
| 0.868 | 0.399 | 0.0 | 1.85 | 0.3620 | 0.97 |
| 0.804 | 0.399 | 0.0 | 1.85 | 0.3106 | 0.98 |
| 0.731 | 0.399 | 0.0 | 1.85 | 0.2602 | 0.96 |
| 0.670 | 0.399 | 0.0 | 1.85 | 0.2127 | 0.97 |
| 0.596 | 0.399 | 0.0 | 1.85 | 0.1601 | 0.96 |
| 0.483 | 0.120 | 3.0 | 1.85 | 0.2740 | 0.98 |
| 0.483 | 0.210 | 3.0 | 1.85 | 0.2050 | 1.00 |
| 0.483 | 0.300 | 3.0 | 1.85 | 0.1370 | 1.00 |
| 0.483 | 0.390 | 3.0 | 1.85 | 0.0730 | 0.99 |
| 0.484 | 0.120 | 3.0 | 2.60 | 0.2720 | 1.01 |
| 0.484 | 0.240 | 3.0 | 2.60 | 0.1830 | 1.00 |
| 0.484 | 0.361 | 3.0 | 2.60 | 0.0980 | 0.98 |
| 0.560 | 0.299 | 1.0 | 2.60 | 0.1977 | 0.98 |
| 0.561 | 0.299 | 3.0 | 2.60 | 0.2007 | 0.98 |
| 0.558 | 0.299 | 5.0 | 2.60 | 0.2012 | 0.97 |
| 0.559 | 0.299 | 7.0 | 2.60 | 0.2016 | 0.97 |
| 0.558 | 0.299 | 9.0 | 2.60 | 0.2010 | 0.97 |
| 0.561 | 0.299 | 11.0 | 2.60 | 0.1990 | 0.99 |
| 1 |
Besides methionine sulfoxide,29,35 methionine sulfone13,35 may also be a possible product upon oxidizing the sulfur center in methionine suggesting another possible limiting stoichiometry, but evidently under our experimental condition methionine sulfone cannot be formed in detectable amount.
| 2 |
To support this statement, we have performed 1H NMR studies to analyze the products in slight excess of methionine. Figure 1 shows a strong singlet peak around 2.1 ppm chemical shift belonging to the hydrogens of the S-methyl group of methionine, a triplet at around 2.6 ppm belonging to the methylene group of hydrogens adjacent to the sulfur atom and a triplet at around 3.8 ppm belonging to the hydrogen of the methine group. As it is seen, the most intense peak belongs to the S-methyl group which is suitable to identify the slight excess methionine after the reaction ended. For the sake of completeness, it should be mentioned that the most intense peak of the S-methyl group of methionine sulfoxide and methionine sulfone may be observed at around 2.75 and 3.15 ppm, respectively.32 As it is seen, the NMR-spectrum of the reaction mixture does not contain any observable peak in the 2.8–3.9 ppm region meaning that methionine sulfone cannot be the end-product of the title reaction. At the same time around 2.7 ppm, a singlet peak appears belonging to the methyl group of methionine sulfoxide. This latter peak is very stable for even over a month. Consequently, the stoichiometry of the title reaction can unambiguously be described by eq 1.
Figure 1.

1H NMR spectrum of pure methionine and the product of the reaction at acidic medium. Conditions are as follows: 99.41 mM for pure methionine; 52.94 mM methionine, and 49.97 mM iodine for the reaction.
Initial Rate Studies
As it was mentioned in the introduction, there is no detailed kinetic study on the title reaction just a single subsection is devoted to unravel some characteristics, even though it is an essential and complex subsystem of the methionine–iodate clock reaction investigated by Chikwana et al.32 It is known from their study that the formal kinetic order of methionine is 1 and that of iodide ion is −1 indicating an autoinhibitory behavior, but no information is available about those of iodine and hydrogen ion. Figure 2 represents the results of our study providing inevitable evidence that the kinetic orders of the reactants (methionine and iodine) are strictly one. Furthermore, displaying the log–log plots of the initial rate versus concentration of iodide and hydrogen ion (shown in Figure 3) reveals a quite complex dynamical feature. As it is seen, both plots indicate nonlinear dependence of the corresponding logarithmic concentration values. In the case of iodide, the result presented here contradicts with the formal kinetic order of iodide reported previously.32 As we shall later show, it is the consequence of the limited concentration range of iodide ion used in Chikwana’s experiments. It also means that the autoinhibitory feature of iodide ion is not as mild as mentioned in Chikwana’s report. Actually, at slightly higher iodide concentrations, a strong second order inhibiting effect may easily be realized as we shall point out later. The sigmoid type of log–log plots shown in Figure 3 confirms that hydrogen ion has a very complex effect, hydrogen ion indeed inhibits the reaction as well, although this inhibition is not so effective. It is interesting to note that such a complex effect of hydrogen ion is not yet recognized previously.32
Figure 2.

Initial rate studies to determine the formal kinetic orders of iodine (filled symbols) and methionine (empty symbols). Experimental conditions are as follows: (black circles) [Met]0 = 0.48 mM, pH = 2.60, [I–]0 = 3.0 mM; (blue squares) [Met]0 = 0.4 mM, pH = 2.10, [I–]0 = 3.0 mM, and c0 values belong to initial total iodine concentrations. (green circles) TI2 = 0.48 mM, pH = 2.35, [I–]0 = 3.0 mM; (red squares) TI2 = 0.48 mM, pH = 1.60, [I–]0 = 3.0 mM.
Figure 3.

Log–log plots of initial rates against iodide and hydrogen ion concentrations. Conditions are as follows: (black circles) [Met]0 = 1.2 mM, TI2 = 0.48 mM, [I–] = 3.0 mM, and c0 corresponds to [H+]; (blue squares) [Met]0 = 0.48, TI2 = 0.48 mM, pH = 2.1, and c0 corresponds to [I–]0.
Individual Evaluation of Kinetic Curves
Our preliminary experiments measured in the absence of initially added iodide ion revealed that the reaction can be monitored by stopped-flow technique. However, even in huge excess of methionine the kinetic traces cannot be described by a single exponential behavior, thus our stopped-flow measurements are fully consistent to those ones reported in Chikwana’s paper.32 Such typical absorbance–time traces are visualized in Figure 4. The reason for this deviation may easily be interpreted in terms of the autoinhibitory effect of iodide ion. It should, however, be emphasized that this autoinhibition has to be strong enough to slow down the rate of conversion at the end of reaction, which means, indeed, more pronounced negative feedback effect of iodide than considered in Chikwana’s paper. Taking into consideration of all these information obtained, we have performed individual evaluation of kinetic curves by considering the stoichiometry as eq 1 with a rate equation of taking into consideration eq 5 as well.
| 3 |
Figure 4.

(A) Measured (filled circles) and calculated (solid lines) absorbance–time profiles with varying the initial concentration of methionine at pH = 1.60 and TI20 = 0.50 mM in the absence of initially added iodide. Other conditions are as follows: [Met]0/mM = 5.0 (black), 10.0 (blue), 15.0 (green), 20.0 (cyan), and 25.0 (red). (B) Measured (empty triangles) and calculated (solid lines) absorbance–time profiles with varying the initial concentration of iodine at pH = 1.60 and [Met]0 = 15.0 mM in the absence of initially added iodide. Other conditions are as follows: TI20/mM = 0.106 (black), 0.193 (blue), 0.285 (green), 0.390 (cyan), 0.500 (red). These curves are obtained by stopped-flow equipment.
At each pH, the apparent rate coefficients were averaged and these average values were plotted against the hydrogen ion concentration as seen in Figure 5. We would like to emphasize that all the kinetic traces were analyzed regardless of the initial concentration of iodide ion applied. The average deviation obtained for all the 151 kinetic traces were found to be 0.9% which shows an excellent agreement between the measured and calculated data. A clearly nonlinear hydrogen dependence of kapp is observed, and the average values of kapp can be interpreted by the following empirical formula
| 4 |
where A = 1075.6 ± 89.6 M–2 s–1, B = 149.75 ± 12.35 M–1 s–1, C = 0.32409 ± 0.02657 s–1, D = 696402 ± 6168 M–2, and E = 3845.3 ± 34.1 M–1 were used. This result is completely consistent with the log–log plot of the initial rate against the hydrogen ion concentration (see Figure 3). Later, we shall see how these values may be rationalized in terms of the rate coefficients calculated from simultaneous data evaluation.
Figure 5.
Plot of the averages of kapp apparent rate coefficient values obtained by the individual curve fitting method at different pHs against the hydrogen ion concentration. Error bars indicate the standard deviation of the average of kapp values calculated at each pH.
Proposed Kinetic Model for Simultaneous Evaluation of Kinetic Curves
There are three possible options to explain the autoinhibitory effect of iodide ion in the title reaction. Probably the simplest one is when we consider the following two-step mechanistic possibility
| 5 |
| 6 |
when triiodide is treated as a completely inert species, and the rate of eq 6 is linearly proportional to the concentration of both reactants. Evidently, this model has a serious drawback not to take the pH dependence of the kinetic curves into account, but theoretically the iodide inhibition may be encountered. The average deviation for all the 151 experimental traces was found to be 25% clearly indicating that the model has to be improved. Therefore, in the next trial, we have removed eq 6 and inserted the following steps to eq 5:
| 7 |
| 8 |
As it is seen, hypoiodous acid here is considered to be the lone reactive species. Because eq 7 is established relatively rapidly and follows the law of mass action type kinetics, an increase in iodide and hydrogen ion concentrations would shift this equilibrium to the left; hence, the overall rate of reaction would decrease giving rise to the inhibitory effect of iodide and hydrogen ions found experimentally. The rate coefficients of the forward and reverse reactions are well-established; therefore, they were used as fixed values (presented later in Table 2) during the whole calculation process.47−49 Simultaneous evaluation of all the kinetic traces led to 11% average deviation, but removal of the experimental curves measured in the absence of initially added iodide ion would lead to an 2.5% acceptable average deviation. Even the rate coefficients of eq 8 for the rate equation being established as v = k1HOI[Met][HOI] + k2[Met][HOI][H+] may be calculated (k1HOI = 2.44 × 108 M–1 s–1 and k2 = 8.0 × 109 M–2s–1) within the reasonable diffusion controlled range. Despite these promising results, we concluded that the above-mentioned model still contains systematic errors suggesting further improvements with a special focus on the kinetic curves measured in the absence of initially added iodide ion. As a final step, we, therefore, propose that eqs 5 and 7 have to be augmented with the following steps for adequate description of the kinetic data measured in this system:
| 9 |
| 10 |
| 11 |
| 12 |
| 13 |
where MetH–1 is the deprotonated form of methionine. The proposed kinetic model with the rate coefficients fixed and determined in the simultaneous evaluation procedure along with the proposed rate equations are visualized in Table 2.
Table 2. Rate Equations Fixed and Obtained from Evaluating Simultaneously the Kinetic Data of the Methionine–Iodine Reactiona.
| no. | step | rate equation | rate coefficient |
|---|---|---|---|
| (E1) | H3PO4 ⇌ H+ + H2PO4– | kE1[H3PO4] | 1.585 × 10 s–1 |
| (−E1) | k–E1[H+][H2PO4–] | 107 M–1 s–1 | |
| (E2) | Met ⇌ H+ + MetH–1 | kE2[Met] | 5.248 × 105 s–1 |
| (−E2) | k–E2[H+][MetH–1] | 108 M–1 s–1 | |
| (R1) | I2 + I– ⇌ I3– | kR1[I2][I–] | 5.7 × 109 M–1 s–1 |
| (−R1) | k–R1[I3–] | 8.5 × 106 s–1 | |
| (R2) | I2 + H2O ⇌ H+ + I– + HOI | kR2[I2] | 5.52 × 10–2 s–1 |
| k′R2[I2]/[H+] | 1.98 × 10–3 M s–1 | ||
| (−R2) | k–R2[H+][I–][HOI] | 1.023 × 1011 M–2s–1 | |
| k′–R2[I–][HOI] | 3.67 × 109 M–1 s–1 | ||
| (R3) | Met + I2 ⇌ Met–SI+ + I– | kR3[Met][I2] | 370 M–1 s–1 |
| (−R3) | k–R3[Met–SI+][I–] | 106 M–1 s–1 | |
| (R4) | Met–SI+ + H2O → Met–SO + I– + 2H+ | kR4[Met–SI+] | 4.18 ± 0.07 s–1 |
| k′R4[Met–SI+]/[H+] | 0.582 ± 0.007 M s–1 | ||
| (R5) | MetH–1 + I2 ⇌ MetH–1–SI + I– | kR5[MetH–1][I2] | 370 M–1 s–1 |
| (−R5) | k–R5[MetH–1–SI][I–] | 106 M–1 s–1 | |
| (R6) | MetH–1–SI + H2O → Met–SO + H+ + I– | kR6[MetH–1–SI]/[H+] | 0.240 ± 0.002 M s–1 |
Those rate coefficients where no standard deviation is given are fixed during the whole calculation process.
The average deviation for all the 151 kinetic curves was found to be 1.3% indicating a sound agreement between the measured and fitted data. Figures 4 and Figures 6–9 inevitably demonstrate that the model is working correctly in the absence and presence of initially added iodide ion, and it is able to describe the effect of initial methionine, iodine concentration, as well as that of pH on the experimental curves.
Figure 6.

Measured (dots) and calculated (solid lines) absorbance–time profiles with varying the initial concentration of iodine at pH = 1.6 and [Met]0 = 0.48 mM in the presence of initially added iodide ([I–]0 = 3.0 mM). TI20/mM = 0.0877 (black), 0.141 (blue), 0.282 (green), 0.418 (cyan), 0.529 (red), 0.636 (magenta), and 0.810 (yellow).
Figure 9.

Measured (dots) and calculated (solid lines) absorbance–time profiles with varying the pH at [Met]0 = 1.20 mM and TI20 = 0.48 mM in the presence of initially added iodide ion ([I–]0 = 3.0 mM). pH = 2.6 (black), 2.35 (blue), 2.1 (green), 1.85 (cyan), 1.6 (red).
Figure 7.

Measured (dots) and calculated (solid lines) absorbance–time profiles with varying the initial concentration of methionine at pH = 2.1 and TI20 = 0.485 mM in the presence of initially added iodide ([I–]0 = 3.0 mM). [Met]0/mM = 0.120 (black), 0.210 (blue), 0.300 (green), 0.390 (cyan), 0.480 (red), 0.720 (magenta), and 1.20 (yellow).
Figure 8.

Measured (dots) and calculated (solid lines) absorbance–time profiles with varying the initial iodide concentrations at pH = 2.60 and at [Met]0 = 0.72 mM and TI20 = 0.410 mM. [I–]0/mM = 1.0 (black), 3.0 (blue), 5.0 (green), 7.0 (cyan), 9.0 (red), 11.0 (magenta).
Discussion
Validation of the Kinetic Parameters
Step E1 is only an auxiliary process that takes the slight pH change into consideration during the whole calculation procedure. Because this equilibrium is established instantaneously, the rate coefficients of both the forward and reverse reactions are fixed to relatively large values, kE1 = 1.585 × 105 s–1 and k–E1 = 107 M–1 s–1, respectively. The ratio of these rate coefficients provides the pKa1 of phosphoric acid to be 1.8.42 This value worked consistently well in a number of previous systems investigated.50−54
Step E2 is the acid dissociation constant of methionine, which is a rapidly established equilibrium. The rate coefficients of the forward and reverse processes are fixed to be kE2 = 5.248 × 105 s–1 and k–E2 = 108 M–1 s–1, respectively. The ratio of these rate coefficients gives the pKa1 of methionine to be 2.28.42 This value along with the pH range studied suggests that Step E2 would indeed be an inevitable process to be considered to describe the measured absorbance–time series.
Step
R1 is the well-known rapidly established equilibrium between
iodine and triiodide ion studied comprehensively by independent research
groups.55,56 The individual rate coefficients of the
forward and backward processes were fixed during the whole calculation
procedure as kR1 = 5.7 × 109 M–1 s–1 and k–R1 = 8.5 × 106 s–1, respectively, to provide log
= 2.83,
where
is the formation
constant of triiodide
ion.
Step R2 is the well-established hydrolytic equilibrium of iodine studied thoroughly decades ago. The rate coefficients of the forward and backward processes including the H+-inhibited pathway were determined previously,47−49 and these rate coefficients were directly adopted here. Because this equilibrium is established relatively rapidly under our experimental circumstances, it enables us to eliminate H2OI+ species from the model. Consequently, the rate coefficient of k–R2 was recalculated from the values reported by Lengyel et al.49 The fixed rate coefficients used throughout the whole calculation process are indicated in Table 2.
Step R3 was already suggested by Chikwana et al.,32 where iodonium ion transfer is considered to take place on the nonbonding electron pair of the inner sulfur atom in a rapid preequilibrium. This kind of heterolytic transfer process seems to be a general phenomenon of iodine oxidation reactions when I2 attacks an inner sulfur atom of a substrate molecule.57−59 Our calculation confirmed that the title reaction is initiated by this equilibrium. We have systematically checked as well whether either of these individual rate coefficients may be obtained from our experiments or not. Our preliminary calculation showed that set of kR3, k–R3, kR4 and that of kR3, k–R3, kR4′ are in total correlation, therefore these individual rate coefficients cannot be determined independently. As a first step we have fixed k–R3 and performed a series of calculations with varying kR3, kR4, and kR4′. These calculations showed that any value higher than k–R3 = 106 M–1 s–1 would lead to the same average deviation; therefore, we have fixed k–R3 to this lower limit value and tried to determine kR3. Unfortunately, kR3 was also found to be strongly correlated with kR4 and kR4′. Systematic analysis of calculation series has revealed that when kR3 is between 300 and 500 M–1 s–1, then the average deviation in the case of all the 151 kinetic traces would lead to 1.3–1.4% average deviation, but outside this region, it increases significantly indicating systematic deviations between the measured and calculated data. Therefore, we have fixed kR3 = 370 M–1 s–1 and determined kR4 and kR4′. It means that a low value of KR3 = kR3/k–R3 = 3.7 × 10–4 may be calculated for the equilibrium constant of Step R3. Later, we shall see that it provides such parametric conditions that Met–SI+ can be treated as short-lived intermediate with having a small steady-state concentration value for this species. For the sake of completeness, it should also be mentioned that Young and Hsieh40 came to a conclusion that the methionine–iodine reaction is subject to general base catalysis because at low buffer concentration the reaction rate is inversely dependent on the iodide concentration but at high buffer concentrations it shows nonlinear dependence. This observation is explained by the formation of a tetracoordinated sulfurane species. We have therefore performed series of experiments with varying the buffer components concentration but found no observable effect as seen in Figure S3 of the Supporting Information. From these experiments we have concluded that buffer component concentration change, keeping the rest of the conditions constant, does not affect the kinetic traces, thus at least under our experimental conditions the general base catalysis seems to be dubious. It is interesting to note, however, that changing kinetic order of iodide ion is confirmed in our present experiments as well, but this phenomenon is rather related to the varying iodide concentration but not to the alteration of buffer concentration. It appears to suggest that iodide impurities might have played a notable role in Young and Hsieh experiments.
Step R4 is the hydrolysis of Met–SI+ formed in the preequilibrium. We have also found that the rate of this process must contain two terms, the first one has to be independent of pH and the second one is inversely proportional to [H+]. The inclusion of the latter pathway is experimentally verified by the pH dependence of the kinetic curves seen in Figure 9. After fixing kR3 = 370 M–1 s–1 and k–R3 = 106 M–1 s–1, we could calculate kR4 = 10.9 ± 0.2 s–1 and kR4′ = 0.350 ± 0.005 M s–1, which means that only kR3kR4/k–R3 = 4.033 × 10–3 s–1 and kR3kR4′/k–R3 = 1.295 × 10–4 M s–1 can be determined unambiguously from our experiments, with some restrictions that k–R3 ≥ 106 M–1 s–1 and 300 ≤ kR3 ≤ 500 M–1 s–1 inequalities have to be fulfilled.
Step R5 is also an iodonium ion transfer process that occurs between the deprotonated form of methionine and iodine. Neither the individual rate coefficient of the forward process nor that of the reverse reaction can unambiguously be determined from our experiments. Therefore, we fixed kR5 = 370 M–1 s–1 and k–R5 = 106 M–1 s–1 throughout the calculation process.
Step R6 is the rapid hydrolysis of MetH–1–SI, and its rate coefficient may be calculated if kR5 and k–R5 are fixed. Our calculation has revealed that kR6 = 0.240 ± 0.002 M s–1, but actually KR5kR6 = 8.88 × 10–5 M s–1 can be determined unambiguously from our experiments.
Interpretation of the Results
As it was already mentioned Met–SI+ and MetH–1–SI are a short-lived intermediates; therefore, their steady state concentrations may be obtained from the following equations
| 14 |
| 15 |
leading to the following steady-state concentrations
| 16 |
| 17 |
Because the consumption of total amount of iodine (and methionine) can be described by the following differential equation
| 18 |
substitution of eqs 16 and 17 into eq 18 followed by some algebraic rearrangements and simplifications leads to
| 19 |
where
![]() |
20 |
From this equation, it is easy to realize that A, B, C, D, and E in eq 4 may easily be expressed in terms of the rate coefficients obtained and that of initial iodide concentration used in the majority of experiments. Using the above-mentioned rate coefficients presented in Table 2 and [I–]0 = 3.0 mM, one can easily calculate A = 1072.95 M–2 s–1, B = 149.65 M–1 s–1, C = 0.32465 s–1, D = 694712 M–2, and E = 3836.4 M–1 to describe averages of kapp against the [H+] obtained from individual evaluation. Another important experimental result regarding the log–log plot of initial rate versus hydrogen ion concentration may also be confirmed by eq 20. To highlight it, the limits of kapp at high and low values of [H+] may be obtained as follows, when [I–]0 = 3.0 mM is used:
| 21 |
and
| 22 |
meaning that under these conditions, the initial rate becomes independent of pH as it is manifested in Figure 3.
Finally, we shall also point out, how the formal kinetic order of iodide ion increases up to even −2 as suggested in Figure 3. It is well-known that the [I2] may easily be expressed by the help total iodine concentration (TI2) as follows:
| 23 |
where KR1 is the formation constant of triiodide ion. Substituting this equation into eq 19 combined with eq 20 followed by some algebraic manipulations leads to the following expression:
| 24 |
It is easy to see if [I–]0 ≫ 1.5 × 10–3 M condition is fulfilled, then the first term in the denominator is negligible; thus, the formal kinetic order of iodide becomes −2 indicating a very efficient autoinhibitory feature.
Last but not least, some words are also in an order here to put a clear emphasis why this detailed investigation was necessary even if the kinetics of this system was already reported in seemingly sufficient details in a recent report by Chikwana et al.32 in 2009. First, the abstract of the cited paper explicitly says that the direct reaction between iodine and methionine is slow and mildly autoinhibitory. Our results presented here, however, just partially agrees with this statement. The reaction in the absence of initially added iodide ion is fairly rapid (stopped-flow technique is required to follow conveniently the reaction) but indeed autoinhibitory with respect to iodide ion. This autoinhibitory effect is, however, not as mild as stated, at pH = 2 and above, [I–]0 > 3.0 mM condition, it is so effective that an order of magnitude increase in the iodide concentration decreases the initial rate by 2 orders of magnitude! This hidden characteristic is indeed the consequence of limited range of initially added iodide ion concentration used in the previous study.32 Second, it was recently shown by Stanbury60 that the model, intended to describe the methionine–iodate and methionine–iodine combined system, proposed by these authors extremely violates the principle of detailed balancing by 11(!) orders of magnitude making their mechanism completely unreliable. Third, no pH dependence of the methionine–iodine reaction was suggested by Chikwana et al. at the same pH range where slight pH-dependence should have been observed. For the sake of completeness, we have to admit that it is a bit difficult to realize this effect without systematically focusing the pH region where it appears the most prominently. Fourth, the iodide inhibitory effect of the title system in Chikwana’s paper was explained by the concurrent but more sluggish reaction between methionine and triiodide ion compared to the one between methionine and iodine. This model, however, fails to properly describe the measured curves in excess of methionine reported in Chikwana’s article (see Figure 8a of ref (32) compared to Figure S2 of the Supporting Information).
Conclusion
Significant improvement of the kinetic model of the methionine–iodine reaction, which was designated to be the key process of the methionine–iodate system, is presented here to provide a meaningful assistance for adequately describing the clock characteristics of the parent reaction. It was clearly shown that the strong autoinhibitory feature of iodide ion may be observed even at its relatively low concentration. At the same time, mild hydrogen ion dependence of its rate reveals that among the I-containing species, iodine is the kinetically active form. A simple seven-step kinetic model is proposed to describe all of the most important characteristics of the kinetic curves measured from which a rate equation may as well be derived. Last but not least, this work provides a strong warning flag in a sense that even a seemingly simple reaction has to be studied with special circumspection to establish a reliable model to avoid misinterpretation of the dynamics of a more complex system where the given mechanism is believed to play a crucial role.
Acknowledgments
This work was as well supported by the GINOP-2.3.2-15-2016-00049 grant. The study was also financed by the Higher Education Institutional Excellence Programme of the Ministry of Innovation and Technology in Hungary, within the framework of the innovation for sustainable and healthy living and environment thematic programme of the University of Pécs. The project has been supported by the European Union, cofinanced by the European Social Fund Grant No. EFOP-3.6.1.-16-2016-00004 entitled by Comprehensive Development for Implementing Smart Specialization Strategies at the University of Pécs. Financial support of the Hungarian Research Fund NKFIH-OTKA Grant No. K116591 is also acknowledged. This work was also supported by the Start-up Funding (Grant No. DHBK2017163) from East China University of Technology. The authors are grateful to Dr. Attila Takács for his helpful assistance in the 1H NMR measurements.
Supporting Information Available
The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.jpca.0c04271.
The authors declare no competing financial interest.
Supplementary Material
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Data Citations
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