R.J. Dougherty et al. / Journal of Molecular Structure 1131 (2017) 196e200
197
nicely with the rate law proposed by Wallace and Mahon and a
detailed derivation of that rate law can be found in their seminal
study [13]. The enthalpic and entropic contributions to the reaction
were then estimated via Erying Plot. Further evidence of an
oxidatively induced change was observed from chemical shift
changes in the 13C NMR data. The observed changes and the derived
thermodynamic parameters are similar between all the three
molecules studied.
The simplified rate equation (Eq. (2)) can be used to describe the
kinetics by virtue of the fact that the total concentration remains
the same, and that are no other any side reactions during the
measurement time of the kinetics.
The concentration of reactant and product were calculated ac-
cording to
½Aꢁ
½Cꢁ ¼ ½Cꢁ0
½Sꢁ
(3)
2. Materials and methods
where [A] is the area of the NMR signal of the reactant, [S] is the
total area of the NMR signals from the product, and [C]0 is the initial
concentration of the reactant at each temperature. Solution to
Equation (3) is given by
2.1. Materials
Commercially, L-Cys and their ester derivatives are readily
ꢀ
ꢁ
available as hydrochloride salts.
L-Cysteine, L-Cysteine methyl ester,
½Cꢁ ¼ ½Cꢁ0eꢃkt or ½Cꢁ ¼ 1 ꢃ ½Cꢁ0eꢃkt
(4)
and -Cysteine ethyl ester hydrochloride were purchased from
L
Sigma-Aldrich (98% purity) and used with no further modification.
Deuterated dimethyl sulfoxide spiked with 0.05% by volume with
tetramethylsilane (TMS) was used as a solvent and internal refer-
ence (Sigma-Aldrich).
With [C] defined in Eq. (3), a linear fit between the estimated
transition rates (natural logarithm scale) vs. inverse of temperature
in K (1000/T) was used to estimate the activation energy of the
Eyring equation given by
2.2. NMR measurements
ꢂ
ꢃ
ꢂ
ꢃꢂ ꢃ
kh
kBT
ꢃ
D
Hz
1
T
D
Sz
ln
¼
þ
R
(5)
All the 1H and 13C NMR experiments were performed in a 400-
MHz (1H resonance frequency) VNMRS spectrometer (Varian-Agi-
lent) and using the one-NMR probe. Measurement of the exact
sample temperatures in the NMR probe was calibrated using the
chemical shift changes in neat methanol standard (CH3OH) [14].
The probe temperature was set between 30 and 55 ꢀC in the
spectrometer, and the calibrated sample temperature was used in
the calculations. Each sample was prepared by freshly dissolving in
DMSO-d6 to a concentration of ~243 mM just before the start of the
NMR experiment. The probe was tuned and the pulse width was
calibrated at each temperature using the experimental sample. The
approximate delay from the time the sample is prepared to start the
collection of the first transient was 10 min. One-dimensional ex-
periments were performed in an arrayed fashion. All the 1D NMR
experiments were performed at a pulse angle that corresponds to
Ernst angle (~70ꢀ) [15]. Each one-dimensional experiment was
collected over 8 transients, with an acquisition time per FID (free
induction decay) of 2.043 s, and a relaxation recycling delay of 4 s.
The total time for each experiment in the array was 48.34 s. The
array continuously collected until the reaction was almost
completed. The reaction completion time ranges from 2 h at high
temperature to >16 h at low temperatures. All the spectra were
processed using Mestrenova (Mestrelab Research, Santiago de
Compostela, Spain).
R
where h is Planks constant (6.62697 ꢂ 10ꢃ34 J$s), kB is Boltzmann
constant (1.3807 ꢂ 10ꢃ23 J/K), R is the gas constant (8.314 J/
(K$mol)), and the T is sample temperature in Kelvins. The enthalpy
D
Hz was calculated by multiplying the negative slope by R and the
entropy
3. Results
The oxidation mediated change ensuring the formation of the
D
Sz was calculated by multiplying the intercept value by R.
disulfide adduct is modeled as a pseudo-first order reaction with
respect to L-Cys. Fig. 1 highlights the effect of the oxidation medi-
ated changes on L-Cys (Fig. 1a), L-CysME (Fig. 1b) and L-CysEE
(Fig. 1c) on the chemical shifts of the 1H
b protons. The spectra
plotted in blue are at the beginning of the experiment while the
ones plotted in red are after the reaction at 30 ꢀC. The chemical
shifts of the 1H and 13C nuclei at t z 0 and at the end of reaction are
listed in Table 1. Supporting information shows a representative 1H
spectrum along with the chemical shift assignments (Fig. S1) and
the observed chemical shift changes in the 13C spectra (Fig. S2) in
the case of L-CysEE. The major chemical shift changes occur at the
b
-position for all the molecules. The 1H
0.3 ppm while the 13C
resonances shift ~13 ppm for all the mol-
ecules (Fig. S2). The oxidation mediated chemical shift changes in
the 13C
are in the range of 2.7e2.9 ppm for all the molecules.
b protons shift downfield by
b
2.3. Reaction kinetics
a
Remaining nuclei show no significant changes in the chemical
shifts, except the N1 protons, become much narrower and slightly
shielded with an integration that yields approximately three pro-
tons (Fig. S1). This trend continues at all the temperatures studied.
The oxidation mediated change is modeled as a pseudo-first
order reaction process. Ignoring the reverse reaction, the differen-
tial rate law can be written as
The
being the
b
-protons show the AB part of the ABX spin system with X
proton. The chemical shifts of the -protons are shiel-
d½Cꢁ
a
b
¼ k0½Cꢁ½DMSOꢁ
(1)
dt
ded (blue to red spectrum in Fig. 1) and the NMR spectra do not
show the thiol protons (Fig. S1).
where [C] is considered representative of either one of the three
molecules studied; -Cysteine. -Cysteine methyl ester (L-CysME)
and
The chemical shifts of the b-protons between the initial and final
L
L
forms of L-CysEE are well resolved and therefore the area under the
curve of each of them is used to quantify the reactants and prod-
ucts. Fig. 2 shows the change in the concentration of the reactants
and products with time for each temperature in the case of L-CysEE.
The corresponding fit to the pseudo-first order process (Eq [4]) is
also shown as continuous curves. The pseudo-first order rate con-
stants, k, estimated from the exponential decay of the reactants
L-Cysteine ethyl ester (L-CysEE). Upon rearranging Eq. (1), and
defining a pseudo first order rate constant k ¼ k0 ꢂ ½DMSOꢁ, giving
rise to the simplified rate equation,
d½Cꢁ
¼ k½Cꢁ
(2)
dt