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Cooperative Formation of Icosahedral Proline Clusters from Dimers

  • Alexander D. Jacobs
  • K. V. Jovan Jose
  • Rachel Horness
  • Krishnan Raghavachari
  • Megan C. Thielges
  • David E. Clemmer
Research Article

Abstract

Ion mobility spectrometry-mass spectrometry and Fourier transform infrared spectroscopy (FTIR) techniques were combined with quantum chemical calculations to examine the origin of icosahedral clusters of the amino acid proline. When enantiopure proline solutions are electrosprayed (using nanospray) from 100 mM ammonium acetate, only three peaks are observed in the mass spectrum across a concentration range of five orders of magnitude: a monomer [Pro+H]+ species, favored from 0.001 to 0.01 mM proline concentrations; a dimer [2Pro+H]+ species, the most abundant species for proline concentrations above 0.01 mM; and, the dimer and dodecamer [12Pro+2H]2+ for 1.0 mM and more concentrated proline solutions. Electrospraying racemic D/L-proline solutions from 100 mM ammonium acetate leads to a monomer at low proline concentrations (0.001 to 0.1 mM), and a dimer at higher concentrations (>0.09 mM), as well as a very small population of 8 to 15 Pro clusters that comprise <0.1% of the total ion signals even at the highest proline concentration. Solution FTIR studies show unique features that increase in intensity in the enantiopure proline solutions, consistent with clustering, presumably from the icosahedral geometry in bulk solution. When normalized for the total proline, these results are indicative of a cooperative formation of the enantiopure 12Pro species from 2Pro.

Graphical Abstract

Keywords

Proline clusters Ion mobility spectrometry Cooperativity 

Introduction

Electrospray ionization (ESI) [1] of aqueous 0.01 M solutions of the amino acid proline leads to the spontaneous resolution of a proline dodecamer [12Pro+H]+ species that favors a hollow structure, where each proline amino acid is positioned at the vertex of an icosahedron and a single proton is trapped in the interior [2]. This cluster size stands out among a broad distribution of other sizes, extending to nanometer scale assemblies [2, 3, 4]. The formation of enantiopure clusters is entropically favored compared with racemic forms [5]. Myung et al. presented an analysis showing that the propensity for 12Pro chiral resolution is even greater than the homochiral preference measured previously for the serine octamer, [8Ser+H]+ [2, 6], a cluster that has captured the imaginations of many because of its potential as a precursor of biological oligomers (having sequences that are dominated by residues of the same chirality) [7, 8].

In the present paper, we present ion mobility spectrometry-mass spectrometry (IMS-MS), Fourier transform infrared spectroscopy (FTIR), and theoretical quantum chemical studies of proline in aqueous solutions containing 100 mM ammonium acetate. Ammonium acetate buffers the solution to a pH of ~6.8, near the proline isoelectric point (pI = 6.3) where proline exists as zwitterion. Remarkably, nano ESI of enantiopure solutions of proline, at concentrations above 1.0 mM, yields only dimers and dodecamers, indicating a cooperative transition between these species. FTIR studies of enantiopure and racemic solutions show differences in vibrational band intensities, and comparisons with theory suggest that these features are consistent with the existence of clusters such as the icosahedral geometry in bulk solution.

The present findings build on a large body of work involving the resolution of specific chiral forms of different amino acids, including: ESI-MS studies of all of the naturally occurring amino acids, a number of unnatural forms [9, 10, 11, 12, 13, 14, 15], as well as some spectroscopic studies of the isolated ions [16, 17, 18, 19]. Analysis of MS data from mixtures of deuterated and non-deuterated enantiomers have provided direct insight into the magnitude of chiral preferences; interestingly some cluster sizes prefer heterochiral compositions [20, 21, 22, 23]. The association of some amino acids is directly relevant to diseases [24]. Others are useful as models for understanding aggregation of larger peptides [25, 26]. Many experiments have focused on issues of chirality that are thought to be possibly associated with the origins of primordial life [27, 28, 29, 30, 31]. To this end, studies of the clustering of amino acids on hot surfaces as well as cluster deposition onto surfaces followed by laser and thermal desorption have been conducted [32, 33]. In some cases, amino acids [34, 35, 36] and small peptides [37, 38, 39, 40] condense to form peptide bonds in unusual environments, leading to oligomers with sequences that incorporate the precursor amino acids [41], as well as unexpected sequences arising from sidechain transformations [42] – providing a fascinating glimpse into the plasticity of amino acid chemistry and the formation of oligomers [8, 14, 41, 42].

Experimental

Sample Preparation

Aqueous 100 mM ammonium acetate solutions of L-proline and D-proline (Sigma-Aldrich, St. Louis, MO, USA) were prepared such that the proline concentration varied by a factor of ~105. Racemic solutions were prepared from aliquots of standard solutions containing the different enantiomers. For the FTIR studies, samples were dried to remove all H2O and samples were reconstituted in 100 mM ammonium acetate in deuterium oxide (D2O) to the desired proline concentrations.

Ion Mobility Spectrometry-Mass Spectrometry Instrumentation and Measurements

General aspects of IMS theory and instrumentation are described elsewhere [43, 44, 45, 46, 47, 48, 49, 50, 51, 52, 53]. Briefly, the IMS-MS experiments described below were performed on a homebuilt 2m drift tube coupled with a time of flight (TOF) mass spectrometer [49, 54, 55]. A schematic presentation of this instrument is shown in Figure 1. Ions are introduced into the gas phase using a commercial nano electrospray source, a Triversa Nanomate (Advion Bioscience, Inc., Ithaca, NY, USA). Ions are stored in a Smith geometry ion funnel and pulsed periodically (150 μs) into the drift tube [56]. The drift tube is filled with ~3.00 Torr He and is operated under a ~10 V·cm−1 electric field. After mobility separation, ions are transferred into a differentially pumped region and then pulsed into an orthogonal TOF-MS detector. Data are recorded in a nested fashion [46].
Figure 1

Schematic of the homebuilt 2m ion mobility-mass spectrometer

Collision Cross-Section

Drift times (t D ) can be converted to collision cross-sections by using the following equation [53]:
$$ \Omega =\frac{{\left(18\pi \right)}^{1/2}}{16}\frac{ze}{{\left({k}_BT\right)}^{1/2}}{\left[\frac{1}{M_I}+\frac{1}{M_B}\right]}^{1/2}\frac{t_DE}{L}\frac{760}{P}\frac{T}{273.2}\frac{1}{N} $$
(1)
where ze is the charge of the ion, k B is the Boltzmann constant, T is the temperature, E is the electric field, L is the drift tube length, P is the pressure, and N is the neutral number density at STP. M I and M B are the masses of the ion and the buffer gas, in this case helium.

FTIR Measurements

FTIR experiments were carried out on an Agilent Cary 670 FTIR spectrometer with a N2(l)-cooled MCT detector. Spectra were recorded at 2 cm−1 resolution. Aliquots of 10 μL were placed between CaF2 windows with a 25 μm Teflon spacer. The instrument was purged for 30 min with N2 prior to data acquisition. The transmission spectrum from the buffer system was used as a reference and subtracted in order to determine the absorption spectrum of the of amino acid solutions.

Computational Methods and Theory

The location of the electrostatic potential (ESP) minima of the molecule is the likely binding site for an incoming proton. Hence, we have followed a systematic procedure to track the energetically feasible protonated 12Pro clusters. The isomers of [12Pro+H]+ are constructed by placing the proton near the ESP minima of the parent neutral cluster structure and carrying out geometry optimizations using density functional theory (DFT) (vide infra). The feasible [12Pro+2H]2+ isomers are then constructed from the parent [12Pro+H]+ clusters by placing the second proton at the ESP minima in the +1 cluster topography. On energy minimization, the protons in the optimized geometries stay close to the ESP minima (close to the carboxyl oxygen) of the parent cluster. The resulting relative energies of the optimized low-lying cluster isomers included in our analysis fall within an energy window of 0–5 kcal/mol.

The direct calculation of the energies and energy derivatives of 12Pro clusters are computationally expensive. Hence, we have employed the molecules-in-molecules (MIM) fragment-based method [57] for evaluating the energies and energy derivatives for performing structural optimizations and IR spectral simulations. In the MIM fragmentation procedure, we have considered each proline molecule as a separate fragment. Hence, the [12Pro+2H]2+ cluster is separated into 12 fragments. Subsequently, each fragment interacts with neighboring fragments based on distance and number-based criteria to construct the primary subsystems. The overcounting due to overlapping primary subsystems is taken into account by the inclusion-exclusion principle to yield derivative subsystems. DFT calculations are then carried out on all the subsystems using the same consistent criteria to perform geometry optimizations and IR spectral evaluations on all the [12Pro+2H]2+ isomers. Further details on the computational procedure and the method involved in the accurate estimation of the electronic energy, molecular geometry, Hessian matrix, and dipole derivatives through MIM method is discussed elsewhere [57, 58]. MIM fragmentation schemes and IR spectral evaluations are implemented through an external Perl script interfacing the Gaussian 09 program suite [59]. All the optimization and IR frequency evaluations have been done using DFT at the MIM2[MPW1PW91/6-311G(d,p):MPW1PW91/6-31G] level of theory using Gaussian 09. All the located structures are confirmed to be minima on the potential energy surface (PES) with no imaginary frequencies. We have also studied the effects of implicit solvation on the IR spectra of these clusters. For comparing the calculated IR spectra with experiment, we have performed a Boltzmann weighted spectral averaging over the local minima.

Results and Discussion

Formation of Proline Monomers, Dimers, and Dodecamers from Ammonium Acetate Solutions

Figure 2 shows representative mass spectra obtained upon electrospraying solutions of ~10.0 mM L-proline and ~10.0 mM D/L-proline in 100 mM ammonium acetate. In both spectra, proline dimer, [2Pro+H]+, is the most abundant species. The only other species detected in the enantiopure solution is the dodecamer, [12Pro+2H]2+. This species is similar to previous work, in which a singly protonated dodecamer was found to be a preferred cluster of proline, favored from enantiopure solutions [2]. The spectrum from the racemic solution shows several low intensity peaks, corresponding to [9Pro+2H]2+ to [15Pro+2H]2+, comprising less than 0.1% of the total ion signal, with no enhancement of the [12Pro+2H]2+ species. This closely resembles results from previous studies, where aggregation of larger oligomeric species was seen for several charge states [3, 5, 22, 23]. We note that the nanoscale droplets used here do not produce the larger clusters observed previously [2, 3]. Apparently in those studies, many clusters arise as proline associates during the drying of the larger droplets. The total ion count between the two solutions is roughly equal (20,000 for enantiopure proline and 22,000 for racemic), when the abundance of enantiopure 12Pro is multiplied by six to account for the number of dimers present in the 12Pro species.
Figure 2

Mass spectra of the raw intensities for ~10 mM L-proline in 100 mM ammonium acetate (a), and ~10 mM D/L-proline in 100 mM ammonium acetate (b). Low abundance species, [9Pro+2H]2+ to [15Pro+2H]2+, from racemic proline are blown up in red. Peaks for [8Pro+2H]2+, [12Pro+2H]2+, and [15Pro+2H]2+ are marked for reference in the racemic solution spectrum, with [8Pro+2H]2+ present at higher concentrations

Cross-section distributions and new simulated proposed structures for [12Pro+2H]2+ are shown in Figure 3 and in Supplementary Figure 1. The measured cross-section for the homochiral [12Pro+2H]2+ species is 286 Å2. When the icosahedron is simulated with two protons instead of one, the calculated cross-section for the new structure shown in Figure 3, Ω = 287 Å2, is in good agreement with the experiment values and is 2% larger than the cross-section, Ω = 281 Å2, reported by Myung et al., for the [12Pro+H]+ species [2]. The larger icosahedron likely arises because Coulombic repulsion from the additional proton causes the hollow structure to expand slightly.
Figure 3

Cross-section distributions of [12Pro+2H]2+ of L-proline (black) and D/L-proline (red), with candidate structures superimposed on the distributions. The major peak in L-proline consists of an icosahedron, whereas racemic proline has two features, an icosahedron and a twisted icosahedron. The inset shows D/L-proline cross-section distribution enlarged to see the two conformations clearly

The new simulation also brings refinement to the previous structure. The addition of a proton reduces the number of proton–proline interactions to stabilize the icosahedron. Previously, the proton was shown to interact with four prolines at any given instant [2]. In the doubly charged 12Pro icosahedron, each proton interacts directly with the carboxylic acid groups from two prolines. Candidate structures for racemic [12Pro+2H]2+ suggest that the far less favorable heterochiral 6D/6L form exists as an icosahedron and a twisted icosahedron. The calculated cross-sections for these two candidate theoretical structures, 287 Å2 and 299 Å2, are in good agreement with the measured cross-sections for racemic 6D/6L [12Pro+2H]2+, 287 Å2 and 297 Å2, respectively. The additional protons associate with the carboxylic acid groups of proline in these structures as well.

Formation of the Enantiopure 12Pro Cluster is Concentration-Dependent

Figure 4 shows the concentration dependence of the ESI-IMS-MS data for both enantiopure and racemic proline solutions. At the lowest concentration, 0.001 mM, of enantiopure proline, only [Pro+H]+ proline is present. As the concentration is increased to 0.03 mM, [2Pro+H]+ appears and becomes the only species present at 0.05 mM. From 1.0 to 100.0 mM, both [2Pro+H]+ and [12Pro+2H]2+ are present in the mass spectra. It is remarkable that even across this wide range of concentrations, nano ESI produces only [2Pro+H]+ and [12Pro+2H]2+. For the racemic proline solution, dimer is formed at higher concentrations than the enantiopure solution, 0.1 mM compared with 0.03 mM, respectively, and the [2Pro+H]+ becomes the most abundant species at all concentrations above 0.1 mM. A small population (<0.1%) of larger clusters, 8–15Pro, are observed from the racemic solution at concentrations above 0.4 mM. Between 3 and 7 mM proline, there is a sharp increase in the total count of clusters for both proline solutions, indicating a possible ESI-based formation of the clusters. In the normalized and mass balanced plots, however, only the enantiopure 12Pro cluster shows an increase in relative abundance whereas the racemic proline clusters do not, suggesting these clusters are emerging from solution. If the increase was related to the ESI process, the change in cluster abundance would appear in the normalized and mass balanced plots for both enantiopure and racemic proline solutions.
Figure 4

Raw ion counts for enantiopure (left) and racemic (right) proline from the ESI-IMS-MS data across a ~105 concentration range (top), normalized intensity at each concentration across the ~105 concentration range (middle), and mass balance concentration, which takes into account the total number of prolines in each species (bottom). Black squares represent Pro, red circles 2Pro, blue triangles 12Pro for enatiopure proline and the summation of 8-15Pro for racemic proline, and dashed lines represent the sum of total proline counts (black), and total proline (red). All data are fit with the best fit line to guide the eye. Representative error bars are shown for 10.0 mM. To obtain the mass balanced concentration values, the abundance of a particular species is multiplied by the number of subunits that form that species. Data are then normalized at each concentration

It is interesting to examine the concentration dependence of cluster formation in more detail. Figure 4 shows that as the proline concentration is increased in the enantiopure solution, the abundances of the 2Pro and 12Pro species also increase. However, above 2 mM the 12Pro abundance increases more rapidly than the 2Pro. This can be observed more clearly in the data that are normalized at each concentration. That is, the relative population of 12Pro increases more rapidly than 2Pro and appears to compete with the 2Pro abundance. At our highest concentration, the 12Pro abundance is ~40% of the total, whereas 2Pro comprises ~60%. An additional normalization that accounts for the total number of prolines in each species is also shown in Figure 4. This shows that 12Pro utilizes the bulk of the available proline in the homochiral solution. This analysis shows that abundance of the enantiopure 12Pro cluster is much greater than clusters formed in the heterochiral solutions. That no intermediates are observed is also remarkable, and is indicative of a cooperative two-state 6(2Pro)⇋12Pro transition in the homochiral system.

Total ion count and total monomeric proline are also shown in Figure 4 in the black dashed and red dotted lines, respectively. The total ion count was calculated by adding the ion counts of each species at each concentration. Total monomeric proline was calculated by multiplying the proline species by the number of prolines that form that species. These values were then added together. Results from these calculations show that for the enantiopure proline solution, while the dimer constitutes most of the ion count, most of the available proline is actually incorporated into the dodecamer, shown in the total monomeric proline. This is reflected in the mass balance normalized plot, also in Figure 4.

FTIR Measurements of L-Proline and D/L-Proline Solutions

Figure 5 shows FTIR spectra for solutions of enantiopure and racemic proline, at concentrations of 0.01, 0.5, 10, and 100 mM in 100 mM ammonium acetate in D2O. These concentrations correspond to regions of the MS data where the monomer, dimer, and mixtures of dimer and clusters are observed (see Figure 4). We focus on the IR region between 1000 and 2000 cm−1 because this region leads to the largest differences for the range of solution concentrations. At the lowest concentration of 0.01 mM, at which ESI-IMS-MS predicts the presence of only monomer, there is a broad distribution around 1460 cm−1 that is likely associated with the HOD stretching mode from residual water [60]. As the concentration is increased to 0.5 mM, a sharper feature at ~1420 cm–1 that is assigned to the COO symmetric stretch appears for both solutions [61]. At 10.0 mM, the spectra of both enantiopure and racemic proline solutions show additional sharp peaks at ~1620 cm−1 and 1560 cm−1 that are ascribed to the COO asymmetric stretching and the NH2 + scissoring vibration, respectively (Figure 5) [61]. At 100.0 mM, the absorbance of the COO asymmetric stretch for the enantiopure solution proline shows a dramatic increase. There is more 12Pro present in the ESI-IMS-MS data at this concentration, suggesting that the additional absorbance is related to the presence of larger clusters. We note that the lack of a linear response in absorbance at the highest concentrations is likely an outcome of the high concentration used in these studies [62].
Figure 5

FTIR spectra of L-proline (left) and D/L-proline (right) at concentrations of 0.01, 0.5, 10, and 100 mM. Experimental data is in black solid lines, simulated 12Pro icosahedron is in red dotted lines, shifted down by 5% to account for anharmonicity. Dashed lines and associated labels indicate the vibrations with the greatest changes between the concentrations

Figure 5 also shows a calculated IR spectrum of the theoretical 12Pro structure in solution (scaled down uniformly by 5% to take the anharmonicity into account). Several of the carboxylate stretches are found in the region near the peaks observed for the enantiopure solution, consistent with the presence of clusters. There is far less agreement between the experimental spectrum measured for the racemic proline solution and the calculated 12Pro spectrum. Overall these results require that different species must be present in the racemic and enantiopure bulk solutions. While the results do not unambiguously show that the 12Pro icosahedron is present in the enantiopure solution, these findings are not inconsistent with this conclusion.

Conclusions

Nano-ESI-IMS-MS experiments have been combined with FTIR measurements and theory to study enantiopure and racemic solutions of proline over a range of concentrations, from 0.001 to 100 mM. The ESI-IMS-MS results show only peaks corresponding to 2Pro and 12Pro for the enantiopure solution at proline concentrations above 1.0 mM. This requires that the 12Pro icosahedron is formed through a cooperative two-state 6(2Pro)⇋12Pro transition. That no intermediates are observed is remarkable. Theoretical calculations are consistent with the formation of such a structure and when combined with FTIR studies suggest that 12Pro may exist in bulk solution.

Notes

Acknowledgments

K.R. is supported by National Science Foundation [grant number CHE-1665427] at Indiana University. A.D.J. is supported by Robert and Marjorie Mann Fellowship from Indiana University.

Supplementary material

13361_2017_1833_MOESM1_ESM.docx (573 kb)
Supplementary Figure 1 (DOCX 572 kb)

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Copyright information

© American Society for Mass Spectrometry 2017

Authors and Affiliations

  • Alexander D. Jacobs
    • 1
  • K. V. Jovan Jose
    • 1
  • Rachel Horness
    • 1
  • Krishnan Raghavachari
    • 1
  • Megan C. Thielges
    • 1
  • David E. Clemmer
    • 1
  1. 1.Department of ChemistryIndiana UniversityBloomingtonUSA

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