The fraction of gauche conformers of N,N-dimethylsuccinamic acid (1) and its Li(+), Na(+), K(+), Mg(2+), Ca(2+), and N(Bu)4(+) salts were estimated in DMSO and D2O solution by comparing the experimental vicinal proton-proton couplings determined by (1)H NMR spectroscopy with those calculated using the Haasnoot, de Leeuw, and Altona (HLA) equation. In DMSO, the gauche preferences were found to increase with decreasing Ahrens ionic radius of the metal counterion. The same trend was not seen in D2O, where the gauche fraction for all of the metallic salts were estimated to be approximately statistical or less. This highlights the importance of metal chelation on the conformation of organic molecules in polar aprotic media, which has implications for protein folding.
The fraction of gauche conformers of N,N-dimethylsuccinamic acid (1) and its Li(+), Na(+), K(+), Mg(2+), Ca(2+), and N(Bu)4(+) salts were estimated in DMSO and D2O solution by comparing the experimental vicinal proton-proton couplings determined by (1)H NMR spectroscopy with those calculated using the Haasnoot, de Leeuw, and Altona (HLA) equation. In DMSO, the gauche preferences were found to increase with decreasing Ahrens ionic radius of the metal counterion. The same trend was not seen in D2O, where the gauche fraction for all of the metallicsalts were estimated to be approximately statistical or less. This highlights the importance of metal chelation on the conformation of organic molecules in polar aprotic media, which has implications for protein folding.
Metal ions interactions
are crucial for many biological processes
including protein folding,[1] enzymatic catalysis,[2] and signal transduction.[3] One of the important roles of metal cations in biological system
is the maintenance of precise electrochemical gradients across cell
membranes. Such electrochemical gradients have been studied extensively
in essential biological mechanisms such as nutrients transport and
the maintenance of resting and action potentials.[4,5] However,
many studies have also demonstrated that conformational changes caused
by metal chelation can alter the biological activities of substances.
For example, Mg2+ and Ca2+ can induce distinct
and separate conformational changes in calcium-binding protein 1,
increasing structural stability of the protein.[6] In addition, the mechanism involved in muscle contraction
is initiated by the complexation of Ca2+ to calmoludin
that is activated by concomitant conformational changes. Also, the
binding of Mg2+ to three aspartic acid residues in CheY,
a signal transduction protein in bacteria, facilitates activation
of the protein.[7]Investigation of
metal-induced conformational changes at the molecular
level within biological systems is often complicated by other competing
forces such as hydrogen bonds. Therefore, it is much more convenient
to study simpler model systems, where a specific interaction of interest
can be isolated. For example, Juaristi et al. used a 5-acetoamido-1,3-dioxane
derivative to show that LiBr is capable of disrupting intramolecular
amidehydrogen bonds through the formation of a six-membered ring
LiBr complex.[8] A subsequent extension of
Juaristi’s study using 5-carboxy-1,3-dioxanes revealed an increase
in the stability of the axial isomer with Ag+ and Li+ salts, while larger metal ions such as Na+ and
K+ had only marginal effects.[9] In a recent paper, Roberts et al. examined the conformational preferences
of ,-dimethylsuccinamic acid (1, DMSA), its tetrabutylammonium
salt (1e), and its lithium salt (1a). Interestingly, 1a resulted in an overwhelming preference for the gauche conformer (Figure 1) in aprotic
solvents, while 1e remained predominantly trans (anti).[10] The un-ionized 1 was determined to have a statistical gauche fraction
of 0.66, indicating no preference for either the gauche or trans conformers. The conformational equilibrium
of 1a were found to be strongly solvent-dependent, such
that the solvents’ hydrogen bonding strength as measured by
Kamlet–Taft’s α scale was a dominant factor.[10]
Figure 1
Conformational equilibria of ,-dimethylsuccinamic
acid (1, top) and its lithium salt (1a,
bottom) in
DMSO.
Conformational equilibria of ,-dimethylsuccinamic
acid (1, top) and its lithium salt (1a,
bottom) in
DMSO.In this paper, the conformational
study of 1 has been
extended by including the Na+, K+, Mg2+, and Ca2+salts. ,-Dimethylsuccinamic acid (1) is particularly suitable for mimicking metal chelation in biological
systems because both the carboxylate and amidemetal complexes are
commonly found in polypeptides.[11] The motivation
behind this work is to draw parallels between the conformational preferences
of 1 as a function of these salts in DMSO and water as
solvents. While water as a solvent imitates the aqueous environments
commonly found in biological systems, DMSO mimics the polar aprotic
media found in the interior of folded polypeptides.
Results and Discussions
Model
System
Simple 1,2-disubstituted ethane systems
such as -dimethylsuccinamic acid
(1) are efficient models to study intramolecular interactions
because they adopt well resolved gauche and trans conformers (Figure 2), where intramolecular
noncovalent interactions can stabilize the gauche conformations. Because there are two possible gauche and one trans staggered conformers, the preference
for each conformer can be deduced by measuring the ratios of their
respective populations using proton (1H) NMR spectroscopy.
In the absence of any preferential stabilization, the statistical gauche fraction (F) should
be 0.67. Therefore, an F value greater
than 0.67 indicates stabilization of the gauche conformer,
plausibly by intramolecular interaction. On the other hand, F values less than 0.67 suggest an antagonistic
relationship between the two substituents on the ethane, which may
be due to electrostatic and/or steric repulsions.
Figure 2
Two possible gauche (g+ and g−)
and trans (t) conformers of -dimethylsuccinamate,
where M+ represents the alkali ions (Li+, Na+, and K+) and alkaline earth ions (Mg2+ and Ca2+). The various geometries were deduced from computational
modeling (vide infra) in the gas phase.
Two possible gauche (g+ and g−)
and trans (t) conformers of -dimethylsuccinamate,
where M+ represents the alkali ions (Li+, Na+, and K+) and alkaline earth ions (Mg2+ and Ca2+). The various geometries were deduced from computational
modeling (vide infra) in the gas phase.The gauche fraction of each conformer
was estimated
by comparing the experimental vicinal proton coupling constants (3JHH) measured by 1H
NMR spectroscopy with their semiempirical counterparts calculated
using the Haasnoot, de Leeuw and Altona (HLA) equation (eq 2).[12] Equation 2 is an improved version of the original equation.[13] Because the rotation about the “CH2–CH2” bond is rapid at room temperature,
the experimental vicinal coupling constants (3Jobs) represent weighted averages of the individual couplings
for the gauche and trans conformers,
as described by eq 1. Note here that sum of
the fractions is unity, i.e., F + F = 1. Also note that two experimental 3Jobs values, i.e., 3J13 and 3J14 (where 3J13 = 3J24 and 3J14 = 3J23) can
be used to provide independent values for F and F.The HLA equation gives more accurate
results
than the traditional Karplus equation because it takes into account
the orientation and electronegativity variables (λ) of the substituent
groups attached to the central C–C fragment. The electronegativity
values for CO2–, CO2H, and
CONMe2 have been reported elsewhere.[14] The parameter ζi can take the values +1
or −1 depending on the relative orientation of the substituents.
The essential dihedral angles (φ) were derived from geometries
of the optimized structures from DFT calculations.
Computational
Analysis
Conformational searches for
Na+(1b), K+(1c), Ca2+(1d), and Mg2+(1e) salts
of -dimethylsuccinamic acid were
first performed with SPARTAN at the molecular mechanics level. These
preliminary calculations provided guess-structures for subsequent
DFT calculations. The DFT calculations were carried out at the B3LYP/6-31+G(2d,2p)
level in the gas phase using Gaussian 03 program.[15] Subsequent free energy calculations at the same level as
the optimized structures determined the relative free energies and
revealed that the gas phase optimized structures were of stable forms
and not transition states.[15]The
graphical representations of the DFT gas phase optimized structures
are shown in Figure 3. Distances of carboxylate-metal
ion complex in the respective gauche conformers for 1a–1c were calculated to be greater than
their trans counterparts in each case. For example,
the calculated Li+–O distances for 1a (1.93–1.96 Å) in the gauche conformer
are consistent with the values of 1.90–2.67 Å found in
lithium-carboxylate X-ray crystal structures,[16−18] while the values
of 1.84–1.85 Å observed in the trans conformer
appear to be slightly underestimated. The calculated Na+–O distances (2.26–2.29 Å) in gauche1b and the K+–O distance in gauche1c (2.58–2.70 Å) matched
the values observed in crystal structures (i.e., 2.26–2.67
Å and 2.36–2.73 Å, respectively),[19−22] whereas the values in the trans conformers are slightly lower (i.e., 2.19–2.20
Å for 1b and 2.53–2.54 Å for 1c). As for the divalent metal salts, the calculated Ca2+–O distances (2.41–2.45 Å) in 1d are
within range of values found in crystal structures (2.26–2.59
Å).[23] The calculated Mg2+–O distances (2.10–2.18 Å) however, are slightly
greater than the values found in crystal structures (1.99–2.09
Å),[24,25] which could be a result of differential
packing forces in the solid state.
Figure 3
DFT-optimized structures for the gauche (top)
and trans (middle) conformers of 1a–1c and gauche (bottom) conformers of 1d–1e at the B3LYP/6-31+G(2d,2p) level
of theory in the gas phase. The calculated metal–oxygen distances
are in Å, and the shown dihedral angles are in deg. Ahrens ionic
radii were used to illustrate the metal ions.
DFT-optimized structures for the gauche (top)
and trans (middle) conformers of 1a–1c and gauche (bottom) conformers of 1d–1e at the B3LYP/6-31+G(2d,2p) level
of theory in the gas phase. The calculated metal–oxygen distances
are in Å, and the shown dihedral angles are in deg. Ahrens ionic
radii were used to illustrate the metal ions.Interestingly, the calculated lowest-energy gauche conformers for 1b and 1c were similar
to that previously calculated for the lithium salt (1a)[10] in the sense that the metal ions preferred
to bridge the carboxylate and amideoxygen atoms (Figure 3). For 1a–1c, DFT
calculations in the gas phase estimated that these gauche conformers are more stable than their trans counterparts
for every case. The calculated free energy of the gauche conformer of 1a is 3.8 kcal/mol more stable than the trans conformer. On the other hand, the gauche conformer of the sodium salt (1b) was calculated to
be only 1.4 kcal/mol more stable than the trans conformer,
while the calculated gauche/trans energy difference is 1.6 kcal/mol for the potassium salt (1b). Free energies of all the DFT gas phase optimized structures
can be found in the Supporting Information.Efforts were also made to investigate the possibility of
an alternative gauche geometry, that is, where only
one of the carboxylateoxygen atoms coordinates to the metal ions. However, the calculations
produced gauche conformers of relatively higher energy
than previously calculated. Other conformational possibilities for 1a–1c may involve aggregation, particularly
for 1a. Lithium salts are known to form dimers, tetramers
and higher-order aggregates.[26] However,
molecular mechanics calculations showed that, even in such aggregates
(dimer and tetramer, for example), both the gauche and trans conformers can still exist. The differences
in the gauche structures calculated for the monovalent
metal salts (1a–1c) were, however,
noticeable in the calculated dihedral angles. For example, of the
three alkali metal salts, 1a had the smallest φ value of 49.4°, and 1c had the largest value of 60.8°. It is reasonable to suggest
that as the Ahrens ionic radius[27,28] of the metal counterion
increases, the dihedral angle widens in order to snugly accommodate
the metal ions. Note that these angles are smaller than the value
of 76.7° calculated for the un-ionized 1, where
“weak” hydrogen bond has been suggested as the only
stabilizing mechanism for the gauche conformer.[10]Unlike 1a–1c, the DFT gas phase
optimized structure of divalent alkaline earth metal salts (1d–1e) share a single metal cation between
two molecules of dimethylsuccinamate.
The divalent metal cation coordinates to six oxygen atoms, forming
a very distorted octahedral geometry, as shown in Figure 3. A randomized conformational search by molecular
mechanics calculations for the divalent metal salts did not find any
conformers in which ,dimethylsuccinamate adopted the trans conformation, which is not surprising considering the higher valency
of Mg2+ and Ca2+ as well as their stronger chelation
to the amide relative to the alkali metals.[29] Synonymous to the trend observed for the alkali metal salts, φ also increases with increasing Ahrens ionic
radii for 1d and 1e, where 1d has a smaller calculated φ of
46.9° and φ 51.3° for 1e.The calculated dihedral angles were used to estimate gauche fractions of 1a–1e in DMSO solution.
In aqueous solvents, however, one would expect that both the carboxylate
and metal cation would be strongly solvated by water molecules, which
should result in the complete dissociation of the ion pairs. Because
hydrated metal ions have larger ionic radii,[30] it is reasonable to assume that the actual φ in aqueous solution should be greater than the calculated
angles for 1a–1e. Furthermore, explicit
solvent–solute hydrogen bond interactions in D2O
are often poorly captured by the current continuum solvation model
(such as the IEFPCM and CPCM) employed by DFT calculations in the
gas phase. For practical purposes, the φ for measurements in aqueous solution was assumed to be 60°
while the trans angle to be 180°.
Experimental 3JHH Coupling
Constants
With the calculated dihedral angles in hand, the
next task is to determine the Jij experimental 3JHH coupling constants. NMR simulation
software (gNMR 5.0)[31] was used to iteratively
reproduce the experimental 1H NMR spectra of the methylene
protons region. Such simulations are essential because they provide
an accurate depiction of the “real” coupling constants
using 4-spin, AA′XX′ systems. The chemical shifts for
the methylene protons are different for all the salts prepared, however,
their spin–spin splitting appeared as doublet of triplets (Figure 4).
Figure 4
Stacked spectra of DMSA (1, top), its tetrabutylammonium
salt (1f, middle), and its lithium salt (1a, bottom) in D2O, spectral unit recorded in ppm.
Stacked spectra of DMSA (1, top), its tetrabutylammonium
salt (1f, middle), and its lithium salt (1a, bottom) in D2O, spectral unit recorded in ppm.
Conformational Analysis
Using the vicinal proton–proton
coupling constants obtained from simulation of the experimental 1H NMR spectra and the dihedral angles from DFT gas phase calculations,
the respective Fg values for 1a-e were estimated as discussed earlier (Table 1 and 2). Compared to the un-ionized 1, which has a small gauche fraction of 0.66
± 0.01,[10] the metal salts generally
showed higher gauche fraction in DMSO. The relatively
small gauche fraction estimated for 1 in DMSO is likely the result of the carboxylic acid’s unfavorable E configuration (Figure 5) that must
be adopted in order to form an intramolecular hydrogen bond.[32]
Table 1
Experimental Vicinal
H–H Couplings
for the N,N-Dimethylsuccinamic Acid
Salts (1a–1e) in DMSO and D2O, Measured in Units of Hz
Li+ salt 1aa
Na+ salt 1b
K+ salt 1c
Mg2+ salt 1d
Ca+ salt 1e
solvents
J13
J14
J13
J14
J13
J14
J13
J14
J13
J14
DMSO
6.02
8.13
6.64
7.75
6.64
8.36
6.08
8.18
7.29
7.31
D2O
6.59
8.33
7.08
7.35
7.04
7.94
7.28
7.31
6.36
8.37
Data obtained from ref (10).
Table 2
Estimated Fraction Gauche (F) for the N,N-Dimethylsuccinamic
Acid Salts (1a–1e) and the Ahrens
Ionic Radiic (in Å) of the Metal Counter
Ionsa
gauche
fractions (Fg)
solvent
Li+ salt 1ab
Na+ salt 1b
K+ salt 1c
Mg2+ salt 1dd
Ca+ salt 1e
DMSO
1.00 ± 0.03
0.78 ± 0.02
0.55 ± 0.01
0.99 ± 0.04
0.79 ± 0.01
D2O
0.55 ± 0.02
0.68 ± 0.01
0.61 ± 0.01
0.67 ± 0.01
0.53 ± 0.05
radii (Å)c
0.68
0.97
1.33
0.66
0.99
The error in F is the deviation of using
the J13 and J14 coupling constants for calculations.
Data obtained from ref (10).
Ahrens
ionic radii were obtained
from ref (28).
F in
DMSO was obtained assuming the dihedral angle to be 50°.
Figure 5
E and Z configurations
of a carboxylic
acid. Also see Figure 1
Data obtained from ref (10).The error in F is the deviation of using
the J13 and J14 coupling constants for calculations.Data obtained from ref (10).Ahrens
ionic radii were obtained
from ref (28).F in
DMSO was obtained assuming the dihedral angle to be 50°.E and Z configurations
of a carboxylic
acid. Also see Figure 1In DMSO, the changing influence of the metal cation on the
conformational
preferences of -dimethylsuccinamate
is evident from the experimentally estimated gauche fractions of 1a–1e. Of the alkali
metal salts, both the lithium and sodium salts (1a and 1b, respectively) showed preferences for the gauche conformer. 1a has the higher gauche fraction of 1.00, followed by 0.78 for 1b. These estimated gauche preferences are in agreement with DFT gas phase calculations,
which predicted the gauche conformer to be more stable
in both cases. DFT gas phase calculations also estimated the energy
difference between the gauche and trans conformer of the lithium salt to be the highest among all the alkali
metal salts, hence 1a’s relatively high gauche
preference. The potassium salt (1c) on the other hand,
has a much lower gauche faction of 0.55 in DMSO,
which suggests that 1c prefers the trans conformer. As for the alkaline earth metal ions, both the magnesium
and calciumsalts (1d and 1e, respectively)
have relatively high preferences for the gauche conformer
in DMSO. For 1d, when the DFT calculated φ of 46.9° was used for the estimation
of the gauche fraction, a value of 1.07 ± 0.05
was obtained. This is likely due to the underestimation of φ by DFT gas phase calculations, as adjusting
the φ to 50° yielded a gauche fraction of 0.99 ± 0.04.The calculated gauche fractions for the metalsalts (1a–1e) are shown schematically
in Figure 6 as a function of the Ahrens ionic
radius of the metal counterion. For the metal salts in DMSO, it is
apparent that gauche fractions of the salts decrease
with increasing Ahrens ionic radii of the metal counterion. Metal
cations with smaller Ahrens ionic radii are likely able to better
fit between the amideoxygen atom and carboxylate to bridge the two
functional groups and induce gauche preference in ,-dimethylsuccinamate.
This assertion is supported by the DFT calculation results shown in
Figure 3, where metal counterions with smaller
Ahrens ionic radii resulted in shorter metal–oxygen distances
and smaller dihedral angles. In the case of 1c, K+ is likely too large to allow a proper fit between the amide
and carboxylate.
Figure 6
Trend in conformational equilibria of the metallic salts
of ,-dimethylsuccinamic
acid as a function of its cationic counterion, arranged from left
to right in decreasing Ahrens ionic radius of the metal counterion.
Trend in conformational equilibria of the metallicsalts
of ,-dimethylsuccinamic
acid as a function of its cationic counterion, arranged from left
to right in decreasing Ahrens ionic radius of the metal counterion.In D2O however, the
interaction between ,-dimethylsuccinamate
and metal cations appears significantly different. No noticeable correlation
between the Ahrens ionic radius of the metal counterion and gauche fraction of the ,-dimethylsuccinamate could be
established. For the metallicsalts in D2O, there is generally
a lower gauche preference than in DMSO. In fact,
none of the N,N-dimethylsuccinamatesalts investigated have gauche fractions significantly
higher than the statistical value of 0.67. The lack of gauche preferences in aqueous solution can be explained by the solvation
efficiency of water. Water molecules can isolate and solvate cations
(metal cation) and anions (carboxylates) appreciably well. Such isolated
solvation would greatly diminish interactions between metal ions and ,dimethylsuccinamate.
Previous study also found that 1a has a lower gauche fraction in solvents with better hydrogendonor propensities,
which are also solvents likely to solvate anions efficiently.[10]
Conclusions
Using 1H
NMR spectroscopy, we have demonstrated that
the conformational equilibria of DMSA and its metal salts are strongly
solvent dependent. In DMSO solution, as the Ahrens ionic radius of
the metal counterion increases, the gauche fraction
of N,N-dimethylsuccinamate decreases.
Interestingly, DFT calculations strongly suggest that the gauche preferences of the metallicsalts are caused by cationic
bridging of the amide and carboxylateoxygen atoms. The same interaction
is much weaker in D2O, where the estimated gauche fractions were significantly below the statistical 0.67 value. These
results seem to suggest that metal chelation has an especially powerful
influence on the conformation of organic molecules in polar aprotic
media.
Experimental Section
Commercial N,N-dimethylsuccinamic
acid (1) of ∼98% purity was used without further
purification. The Na+(1b) salt was prepared
by treating 1 with an equivalent mole of NaH in THF.
The K+(1c) salt was prepared by treating 1 with an equivalent mole of KCN. The Mg2+ (1d) and Ca2+(1e) salts were prepared
by treating 1 with 0.5 equiv of Mg(OH)2 and
Ca(OH)2 respectively in water. Solvent was then evaporated
and samples were dried in vacuo. Commercial DMSO-d6 and D2O were used without further
purifications.The 1H NMR spectra were taken with
Varian 300, 400,
and 600 MHz spectrometers at 25 °C. See Supporting
Information for specific acquisition parameters of each sample.