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Two-photon absorption spectroscopy with a mass-selected beam of CO+2 ions was used to study the predissociative C 2Σ+g state of CO+2. The first photon pumped the A 2Πu←X 2Πg transition and the second photon was used to scan through the C 2Σ+g←A 2Πu transition. A rotational analysis of two bands in this spectrum has been made. The C 2Σ+g state is linear with a C–O bond length of 1.1552(2) Å in the v=0 level. [ABSTRACT FROM AUTHOR]

A technique for the spectroscopic characterization of mass-selected ions in ground and bound excited electronic states involving two-photon absorption and fragment ion detection is demonstrated. A triple quadrupole mass analyzer system is used. Collisionally relaxed ions (M+) from a high pressure source are mass selected, then excited sequentially by two laser colors (λ1,λ2) according to M+→λ1M+*→λ2M+**→F+i and fragment ions (F+i) are detected. Stable ionic states are characterized by scanning λ1 with constant λ2 and this is illustrated on the known transitions of N2O+ (A 2Σ+←X 2Π) and of CS+2 (B 2Σ+u←X 2Πg). New spectroscopic information—vibrational frequencies and rotational constants—and dynamic parameters—lifetimes and fragmentation branching ratios—on N2O+(B 2Σ+) and CS+2 (C 2Σ+g) are obtained by scanning λ2 when λ1 is chosen to populate several or individual rotational levels of the intermediate state. [ABSTRACT FROM AUTHOR]

The objective of this pilot study was to provide data on the oral health status and oral health behaviour of care-dependent elderly people in the canton of Uri. The study aimed at assessing whether age and duration of living in a nursing home is associated with dental attendance, whether there is a relationship between age and the DMF-T index, and how high the risk was for participants to develop oral health problems. The study offered mobile dental services to people residing in nursing homes (NHG) and to community dwellers (CDG). Data was collected on demographics, medical history, presence of pain, ability to eat and oral health behaviour by means of a questionnaire. A clinical examination was performed and data on the oral status was collected. Statistical methods were: median tests, linear regressions and descriptive statistics. Uptake of the programme was low. 56 participants were examined. 47 participants (24 females, 23 males, average age 86.3 ± 7.36 years) resided in nursing home, nine participants (seven females, two males, average age 76 ± 12.8 years) were community dwellers. No significant differences were found between frequency of dental attendance and age (p = 0.35) or duration of stay in a nursing home (p = 0.55). The number of decayed teeth (p=0.005), missing teeth (p=0.01), and the DMF-T index (average in NHG = 26.5, CDG = 20.2, p < 0.001) increased, the number of filled teeth (p=0.02) decreased as age increased. Upon calculation of the 'Teamwerk-index', which takes into account oral health behaviour, dental caries, periodontal status, the majority of participants had a medium risk of developing oral health problems. Our pilot study in rural Switzerland provides first results of the oral health status in dependent elderly people. As people age, oral health deteriorates. More attention should be given in order to achieve better oral hygiene maintenance and more regular dental visits, to ensure a better oral health status in dependent elderly people.

Here we present a guide to ion mobility mass spectrometry experiments, which covers both linear and nonlinear methods: what is measured, how the measurements are done, and how to report the results, including the uncertainties of mobility and collision cross section values. The guide aims to clarify some possibly confusing concepts, and the reporting recommendations should help researchers, authors and reviewers to contribute comprehensive reports, so that the ion mobility data can be reused more confidently. Starting from the concept of the definition of the measurand, we emphasize that (i) mobility values (K 0 ) depend intrinsically on ion structure, the nature of the bath gas, temperature, and E/N; (ii) ion mobility does not measure molecular surfaces directly, but collision cross section (CCS) values are derived from mobility values using a physical model; (iii) methods relying on calibration are empirical (and thus may provide method-dependent results) only if the gas nature, temperature or E/N cannot match those of the primary method. Our analysis highlights the urgency of a community effort toward establishing primary standards and reference materials for ion mobility, and provides recommendations to do so. © 2019 The Authors. Mass Spectrometry Reviews Published by Wiley Periodicals, Inc., (© 2019 The Authors. Mass Spectrometry Reviews Published by Wiley Periodicals, Inc.)

An empirically observed correlation between ion mobility cross sections in helium and nitrogen buffer gases was examined as a function of temperature, molecular size, and shape. Experimental cross sections were determined for tetraglycine, bradykinin, angiotensin 2, melittin, and ubiquitin at 300 K and in the range from 80 to 550 K on home-built instruments and calculated by the projection superposition approximation (PSA) method. The PSA was also used to predict cross sections for larger systems such as human pancreatic alpha-amylase, concanavalin, Pichia pastoris lysyl oxidase, and Klebsiella pneumoniae acetolactate synthase. The data show that the ratio of cross sections in helium and nitrogen depends significantly on the temperature of the buffer gas as well as the size and shape of the analyte ion. Therefore, the analysis of the data indicates that a simple formula that seeks to quantitatively relate the momentum transfer cross sections observed in two distinct buffer gases lacks a sound physical basis.

The combination of mass spectrometry and ion mobility spectrometry (IMS) employing a temperature-variable drift cell or a drift tube divided into sections to make IMS-IMS experiments possible allows information to be obtained about the molecular dynamics of polyatomic ions in the absence of a solvent. The experiments allow the investigation of structural changes of both activated and native ion populations on a timescale of 1-100 ms. Five different systems representing small and large, polar and nonpolar molecules, as well as noncovalent assemblies, are discussed in detail: a dinucleotide, a sodiated polyethylene glycol chain, the peptide bradykinin, the protein ubiquitin, and two types of peptide oligomers. Barriers to conformational interconversion can be obtained in favorable cases. In other cases, solution-like native structures can be observed, but care must be taken in the experimental protocols. The power of theoretical modeling is demonstrated.

The projected superposition approximation (PSA) method was used to theoretically evaluate the factors contributing to the cross section measured in ion mobility experiments and to study how the significance of these factors varies with ion size from diglycine to a 1 μm oil droplet. Thousands of PSA calculations for ∼400 different molecules in the temperature range from 80 to 700 K revealed that the molecular framework made up of atomic hard spheres is, as expected, a major component of the cross section. However, the ion-buffer gas interaction is almost equally important for very small peptides, and although its significance decreases with increasing ion size, interaction is still a factor for megadalton ions. An additional major factor is the ion shape: Fully convex ions drifting in a buffer gas have a minimal frictional resisting force, whereas the resisting force increases with degree of ion surface concaveness. This added resistance is small for peptides and larger for proteins and increases the ion mobility cross section from 0 to greater than 40%. The proteins with the highest degree of concaveness reach a shape-effected friction similar to, and sometimes larger than that of, macroscopic particles such as oil droplets. In summary, our results suggest that the transition from nanoparticle (with Lennard-Jones-like interaction with the buffer gas) to macroscopic particle (with hard sphere-like interaction) occurs at ∼1 GDa.

The conformations of desolvated ubiquitin ions, lifted into the gas phase by electrospray ionization (ESI), were characterized by ion mobility spectrometry (IMS) and compared to the solution structures they originated from. The IMS instrument combining a two-meter helium drift tube with a quadrupole time-of-flight mass spectrometer was built in-house. Solutions stabilizing the native state of ubiquitin yielded essentially one family of tightly folded desolvated ubiquitin structures with a cross section matching the size of the native state (1000 Å(2)). Solutions favoring the A state yielded several well-defined families of significantly unfolded conformations (1800-2000 Å(2)) matching in size conformations between the A state and a fully unfolded state. On the basis of these results and a wealth of data available in the literature, we conclude that the native state of ubiquitin is preserved in the transition from solution to the desolvated state during the ESI process and survives for >100 ms in a 294 K solvent-free environment. The A state, however, is charged more extensively than the native state during ESI and decays more rapidly following ESI. A state ions unfold on a time scale equal to or shorter than the experiment (≤50 ms) to more extended structures.

Amyloid cascades that lead to peptide β-sheet fibrils and plaques are central to many important diseases. Recently, intermediate assemblies of these cascades were identified as the toxic agents that interact with cellular machinery. The location and cause of the transformation from a natively unstructured assembly to the β-sheet oligomers found in all fibrils is important in understanding disease onset and the development of therapeutic agents. Largely, research on this early oligomeric region was unsuccessful because all the traditional techniques measure only the average oligomer properties of the ensemble. We utilized ion-mobility methods to deduce the peptide self-assembly mechanism and examined a series of amyloid-forming peptides clipped from larger peptides or proteins associated with disease. We provide unambiguous evidence for structural transitions in each of these fibril-forming peptide systems and establish the potential of this method for the development of therapeutic agents and drug evaluation.

Many transmissible spongiform encephalopathies (TSEs) are believed to be caused by a misfolded form of the normal cellular prion protein (PrP(C)) known as PrP(Sc). While PrP(Sc) is known to be exceptionally stable and resistant to protease degradation, PrP(C) has not shown these same unusual characteristics. However, using ion mobility spectrometry mass spectrometry (IMS-MS), we found evidence for at least one very stable conformation of a truncated form of recombinant PrP(C) consisting of residues 90-231, which resists unfolding in the absence of solvent at high injection energies and at temperatures in excess of 600 K. We also report the first absolute collision cross sections measured for recombinant Syrian hamster prion protein PrP(90-231).

The prion protein (PrP) is implicitly involved in the pathogenesis of transmissible spongiform encephalopathies (TSEs). The conversion of normal cellular PrP (PrP(C)), a protein that is predominantly alpha-helical, to a beta-sheet-rich isoform (PrP(Sc)), which has a propensity to aggregate, is the key molecular event in prion diseases. During its short life span, PrP can experience two different pH environments; a mildly acidic environment, whilst cycling within the cell, and a neutral pH when it is glycosyl phosphatidylinositol (GPI)-anchored to the cell membrane. Ion mobility (IM) combined with mass spectrometry has been employed to differentiate between two conformational isoforms of recombinant Syrian hamster prion protein (SHaPrP). The recombinant proteins studied were alpha-helical SHaPrP(90-231) and beta-sheet-rich SHaPrP(90-231) at pH 5.5 and pH 7.0. The recombinant proteins have the same nominal mass-to-charge ratio (m/z) but differ in their secondary and tertiary structures. A comparison of traveling-wave (T-Wave) ion mobility and drift cell ion mobility (DCIM) mass spectrometry estimated and absolute cross-sections showed an excellent agreement between the two techniques. The use of T-Wave ion mobility as a shape-selective separation technique enabled differentiation between the estimated cross-sections and arrival time distributions (ATDs) of alpha-helical SHaPrP(90-231) and beta-sheet-rich SHaPrP(90-231) at pH 5.5. No differences in cross-section or ATD profiles were observed between the protein isoforms at pH 7.0. The findings have potential implications for a new ante-mortem screening assay, in bodily fluids, for prion misfolding diseases such as TSEs., (Copyright 2010 American Society for Mass Spectrometry. Published by Elsevier Inc. All rights reserved.)

A combination of ion mobility and mass spectrometry methods was used to characterize the molecular shape of the protein calmodulin (CaM) and its complexes with calcium and a number of peptide ligands. CaM, a calcium-binding protein composed of 148 amino acid residues, was found by X-ray crystallography to occur both in a globular shape and in the shape of an extended dumbbell. Here, it was found, as solutions of CaM and CaM complexes were sprayed into the solvent-free environment of the mass spectrometer, that major structural features of the molecule and the stoichiometry of the units constituting a complex in solution were preserved in the desolvation process. Two types of CaM structures were observed in our experiments: a compact and an extended form of CaM with measured cross sections in near-perfect agreement with those calculated for the known globular and extended dumbbell X-ray geometries. Calcium-free solutions yielded predominantly an extended CaM conformation. Ca(n)(2+)-CaM complexes were observed in calcium-containing solutions, n = 0-4, with the population of the compact conformation increasing relative to the elongated conformation as n increases. For n = 4, a predominantly compact globular conformation was observed. Solutions containing the peptide CaMKII(290-309), the CaM target domain of the Ca(2+)/calmodulin-dependent protein kinase II (CaMKII) enzyme, yielded predominantly globular Ca(4)(2+)-CaM-CaMKII(290-309) complexes. Similar results were obtained with the 26-residue peptide melittin. For the 14-residue C-terminal melittin fragment, on the other hand, formation of both a 1:1 and a 1:2 CaM-peptide complex was detected. On the basis of the entirety of our results, we conclude that the collapse of extended (dumbbell-like) CaM structures into more compact globular structures occurs upon specific binding of four calcium ions. Furthermore, this calcium-induced structural collapse of CaM appears to be a prerequisite for formation of a particularly stable CaM-peptide complex involving peptides long enough to be engaged in interactions with both lobes of CaM.

The gas-phase structures of a series of potassiated tertiary amino acids have been systematically investigated using infrared multiple photon dissociation (IRMPD) spectroscopy utilizing light generated by a free electron laser, ion mobility spectrometry (IMS), and computational modeling. The examined analytes comprise a set of five linear N,N-dimethyl amino acids derived from N,N-dimethyl glycine and three cyclic N-methyl amino acids including N-methyl proline. The number of methylene groups in either the alkyl chain of the linear members or in the ring of the cyclic members of the series is gradually varied. The spectra of the cyclic potassiated molecular ions are similar and well resolved, whereas the clear signals in the respective spectra of the linear analytes increasingly overlap with longer alkyl chains. Measured IRMPD spectra are compared to spectra calculated at the B3LYP/6-311++G(2d,2p) level of theory to identify the structures present in the experimental studies. On the basis of these experiments and calculations, all potassiated molecular ions of this series adopt salt bridge structures in the gas phase, involving bidentate coordination of the potassium cation to the carboxylate moiety. The assigned salt bridge structures are predicted to be the global minima on the potential energy surfaces. IMS cross-section measurements of the potassiated systems show a monotonic increase with growing system size, suggesting that the precursor ions adopt the same type of structure and comparisons between experimental and theoretical cross sections are consistent with salt bridge structures and the IRMPD results.

Using a mass spectrometer equipped with a drift cell, water binding energies of protonated arginine (ArgH+) and protonated lysine (LysH+) were determined in equilibrium experiments and supplementary calculations at the B3LYP/6-311++G** level of theory. The binding energy of the first water molecule was measured to be 10.3 and 10.9 kcal/mol for ArgH+ and LysH+, respectively. Water binding energies decrease with increasing degree of hydration reaching values of 6-7 kcal/mol for the fourth and fifth water molecule. Theory reproduces this trend of decreasing binding energies correctly and theoretical water binding energies agree with experiment quantitatively within 2 kcal/mol. Lowest-energy theoretical structures of ArgH+ and LysH+ are characterized by protonated side chains and neutral alpha-amino and carboxyl groups which form intramolecular hydrogen bonds to the ionic group (charge solvation or CS structures). The salt bridge (SB) structures with two cationic groups (side chain and alpha-amine) and one anionic group (carboxyl) are 13.1 and 9.3 kcal/mol higher in energy for ArgH+ and LysH+, respectively. Theory indicated that the first water molecule binds to the ionic group of the CS structures of ArgH+ and LysH+. With increasing degree of hydration intramolecular interactions are replaced one by one with water bridges with water inserted into the intramolecular hydrogen bonds. Whereas the global minima of ArgH+.(H2O)n and LysH+.(H2O)n, n<7, were calculated to represent CS structures, 7-fold hydrated CS and SB structures, ArgH+.(H2O)7 and LysH+.(H2O)7, are nearly isoenergetic (within <1 kcal/mol).

In recent years, small protein oligomers have been implicated in the aetiology of a number of important amyloid diseases, such as type 2 diabetes, Parkinson's disease and Alzheimer's disease. As a consequence, research efforts are being directed away from traditional targets, such as amyloid plaques, and towards characterization of early oligomer states. Here we present a new analysis method, ion mobility coupled with mass spectrometry, for this challenging problem, which allows determination of in vitro oligomer distributions and the qualitative structure of each of the aggregates. We applied these methods to a number of the amyloid-β protein isoforms of Aβ40 and Aβ42 and showed that their oligomer-size distributions are very different. Our results are consistent with previous observations that Aβ40 and Aβ42 self-assemble via different pathways and provide a candidate in the Aβ42 dodecamer for the primary toxic species in Alzheimer's disease.

The structure of the 21-30 fragment of the amyloid beta-protein (Abeta) was investigated by ion mobility mass spectrometry and replica exchange dynamics simulations. Mutations associated with familial Alzheimer's disease (E22G, E22Q, E22K, and D23N) of Abeta(21-30) were also studied, in order to understand any structural changes that might occur with these substitutions. The structure of the WT peptide shows a bend and a perpendicular turn in the backbone which is maintained by a network of D23 hydrogen bonding. Results for the mutants show that substitutions at E22 do little to alter the overall structure of the fragment. A substitution at D23 resulted in a change of structure for Abeta(21-30). A comparison of these gas-phase studies to previous solution-phase studies reveals that the peptide can fold in the absence of solvent to a structure also seen in solution, highlighting the important role of the D23 hydrogen bonding network in stabilizing the fragment's folded structure.

The first steps of hydration of the protonated aromatic amino acids phenylalanine, tryptophan, and tyrosine were studied experimentally employing a mass spectrometer equipped with a drift cell to examine the sequential addition of individual water molecules in equilibrium experiments and theoretically by a combination of molecular mechanics and electronic structure calculations (B3LYP/6-311++G**) on the three amino acid systems including up to five water molecules. It is found that both the ammonium and carboxyl groups offer good water binding sites with binding energies of the order of 13 kcal/mol for the first water molecule. Subsequent water molecules bind less strongly, in the range of 7-11 kcal/mol for the second through fifth water molecules. The ammonium group is able to host up to three water molecules and the carboxyl group one water molecule before additional water molecules bind either to the amino acid side chain as in tyrosine or to already-bound water in a second solvation shell around the ammonium group. Reasons for the surprisingly high water affinity of the neutral carboxyl group, comparable to that of the charge-carrying ammonium group, are found to be high intrinsic hydrophilicity, favorable charge-dipole alignment, and--for the case of multiply hydrated species--favorable dipole-dipole interaction among water molecules and the lack of alternative fully exposed hydration sites.

Aggregation of alpha-synuclein (alpha-syn), a protein implicated in Parkinson's disease (PD), is believed to progress through formation of a partially folded intermediate. Using nanoelectrospray ionization (nano-ESI) mass spectrometry combined with ion mobility measurements we found evidence for a highly compact partially folded family of structures for alpha-syn and its disease-related A53T mutant with net charges of -6, -7, and -8. For the other early onset PD mutant, A30P, this highly compact population was only evident when the protein had a net charge of -6. When bound to spermine near physiologic pH, all three proteins underwent a charge reduction from the favored solution charge state of -10 to a net charge of -6. This charge reduction is accompanied by a dramatic size reduction of about a factor of 2 (cross section of 2600 A2 (-10 charge state) down to 1430 A2 (-6 charge state)). We conclude that spermine increases the aggregation rate of alpha-syn by inducing a collapsed conformation, which then proceeds to form aggregates.

The effect of single amino acid substitutions associated with the Italian (E22K), Arctic (E22G), Dutch (E22Q) and Iowa (D23N) familial forms of Alzheimer's disease and cerebral amyloid angiopathy on the structure of the 21-30 fragment of the Alzheimer amyloid beta-protein (Abeta) is investigated by replica-exchange molecular dynamics simulations. The 21-30 segment has been shown in our earlier work to adopt a bend structure in solution that may serve as the folding nucleation site for Abeta. Our simulations reveal that the 24-28 bend motif is retained in all E22 mutants, suggesting that mutations involving residue E22 may not affect the structure of the folding nucleation site of Abeta. Enhanced aggregation in Abeta with familial Alzheimer's disease substitutions may result from the depletion of the E22-K28 salt bridge, which destabilizes the bend structure. Alternately, the E22 mutations may affect longer-range interactions outside the 21-30 segment that can impact the aggregation of Abeta. Substituting at residue D23, on the other hand, leads to the formation of a turn rather than a bend motif, implying that in contrast to E22 mutants, the D23N mutant may affect monomer Abeta folding and subsequent aggregation. Our simulations suggest that the mechanisms by which E22 and D23 mutations affect the folding and aggregation of Abeta are fundamentally different.

Evidence from cross section data indicates that ubiquitin +13 ions lose their secondary and tertiary structure in mass spectrometric experiments. These transitions from the folded state into the near linear final structure occur at the experimental temperatures on time scales that are far too long for conventional molecular dynamics simulations. In this study, an approach to mass spectrometric unfolding processes is developed and a detailed application to an ubiquitin +13 ion system is presented. The approach involves a sequence of molecular dynamics simulations at gradually increasing temperatures leading to identification of major intermediate states, and the unfolding pathway. The unfolding rate at any temperature can then be calculated by a Rice-Ramsperger-Kassel (RRK) approach. For ubiquitin +13, three interesting intermediate states were found and the final near linear geometry was computed. The several relevant energy barriers calculated for the process are in the range of 7 to 15 kcal mol(-1). The unfolding time scale at 300 K was computed to be 2 ms. Cross section calculations using a hard sphere scattering model were carried out for the final structure and found to be in good accord with the results of electrospray experiments supporting the theoretical model used. The approach employed here should be applicable to any other solvent-free protein system.

The interaction of the cyclic nonapeptide oxytocin (OT) with a number of alkaline earth and divalent transition metal ions (X(2+)) was examined employing mass spectrometry (MS) and ion mobility spectrometry (IMS) techniques in combination with molecular dynamics (MD) and density functional theory (DFT) calculations. Under acidic conditions it was found that OT exhibits an exceptionally strong affinity for all divalent metal ions resulting in strong [OT + X](2+) peaks in the mass spectrum. Under basic conditions only Cu(2+) and Ni(2+)-OT complexes were detected and these were singly, doubly, triply, or quadruply deprotonated. Collision-induced dissociation of the [OT - 3H + Cu](-) complex yielded exclusively C-terminal Cu(2+)-containing fragments (Cu(2+)fragment(3-)), suggesting that the Cu(2+) ligation site includes deprotonated C-terminal backbone amide nitrogen atoms and the N-terminal amino nitrogen atom in [OT - 3H + Cu](-). MD and DFT calculations indicate a square-planar complex is consistent with these observations and with experimental collision cross sections. MD and DFT calculations also indicate either an octahedral or trigonal-bipyramidal complex between Zn(2+) and OT is lowest in energy with carbonyl oxygens being the primary ligation sites. Both complexes yield cross sections in agreement with experiment. The biological impact of the structural changes induced in OT by divalent metal ion coodination is discussed.

With the development of electrospray and matrix-assisted laser desorption ionization, mass spectrometry (MS) evolved into a powerful tool in the field of biochemistry. Whereas MS is primarily analytical in nature, an increasing number of MS research groups employ the method to address fundamental biochemical questions. Probing the interaction of noncovalently bound molecules in the mass spectrometer is one of the most interesting MS-based experiments possible today, with the potential of making a significant contribution to the basic understanding of the structure and function of biochemical complexes. Here we review a number of current research efforts employing primarily MS techniques to investigate intermolecular interactions in biochemical systems. Examples chosen include the interaction of biomolecules with solvent molecules; interactions between nucleic-acid molecules, in particular, interactions in duplex and quadruplex structures; and interactions between proteins involved in neurodegenerative diseases. Finally we conclude by presenting a few examples of very large biomolecular assemblies in the mega-Dalton range analyzed by MS.

The sequential addition of water molecules to protonated and deprotonated forms of the four mononucleotides dAMP, dCMP, dGMP, and dTMP was studied experimentally by equilibrium measurements using an electrospray mass spectrometer equipped with a drift cell and theoretically by computational methods including molecular modeling and density functional theory calculations. Experiments were carried out in positive and negative ion mode, and calculations included the protonated and deprotonated forms of the four nucleotides. For deprotonated anionic nucleotides the experimental enthalpies of hydration (DeltaH degrees n) were found to be similar for all four systems and varied between -10.1 and -11.5 kcal mol-1 for the first water molecule (n = 1) and -8.3 and -9.6 kcal mol-1 for additional water molecules (n = 2-4). Theory indicated that the first water molecule binds to the charge-carrying phosphate group. Simulations of deprotonated mononucleotides with four water molecules yielded a large number of structures with similar energies. In some of the structures all four water molecules cluster around the phosphate group, and in other structures the four water molecules each hydrate a different functional group of the nucleotide. These include the phosphate group, the deoxyribose hydroxyl group, and various functional groups on the nucleobases. Experimental DeltaH degrees 1 values for the protonated cationic mononucleotides ranged from -10.5 to -13.5 kcal mol-1 with more negative values (< or =-12 kcal mol-1) for dCMP, dGMP, and dTMP and the least negative value for dAMP. For n = 2-4 DeltaH degrees n values varied from -6.9 to -9.7 kcal/mol and were similar in value to the deprotonated nucleotides except for dAMP. Theory on the protonated nucleotides indicated that the first water molecule binds to the charge-carrying group for dCMP, dGMP, and dTMP. For protonated dAMP, on the other hand, the charge-carrying N3 group is well self-solvated by the phosphate group and not readily available for a hydrogen bond with the water molecule. The insight gained on nucleotide stabilization by individual water molecules is used to discuss the competition between hydration of individual nucleotides and Watson-Crick base pairing.

Oligomeric, neurotoxic amyloid protein assemblies are thought to be causative agents in Alzheimer's and other neurodegenerative diseases. Development of oligomer-specific therapeutic agents requires a mechanistic understanding of the oligomerization process. This is a daunting task because amyloidogenic protein oligomers often are metastable and comprise structurally heterogeneous populations in equilibrium with monomers and fibrils. A single methodological approach cannot elucidate the entire protein assembly process. An integrated multidisciplinary program is required. We discuss here the synergistic application of in hydro, in vacuo, and in silico methods to the study of the amyloid beta-protein, the key pathogenetic agent in Alzheimer's disease.

Folding and self-assembly of the 42-residue amyloid beta-protein (Abeta) are linked to Alzheimer's disease (AD). The 21-30 region of Abeta, Abeta(21-30), is resistant to proteolysis and is believed to nucleate the folding of full-length Abeta. The conformational space accessible to the Abeta(21-30) peptide is investigated by using replica exchange molecular dynamics simulations in explicit solvent. Conformations belonging to the global free energy minimum (the "native" state) from simulation are in good agreement with reported NMR structures. These conformations possess a bend motif spanning the central residues V24-K28. This bend is stabilized by a network of hydrogen bonds involving the side chain of residue D23 and the amide hydrogens of adjacent residues G25, S26, N27, and K28, as well as by a salt bridge formed between side chains of K28 and E22. The non-native states of this peptide are compact and retain a native-like bend topology. The persistence of structure in the denatured state may account for the resistance of this peptide to protease degradation and aggregation, even at elevated temperatures.

The structural properties of the Abeta42 peptide, a main constituent of the amyloid plaques formed in Alzheimer's disease, were investigated through a combination of ion-mobility mass spectrometry and theoretical modeling. Replica exchange molecular dynamics simulations using a fully atomic description of the peptide and implicit water solvent were performed on the -3 charge state of the peptide, its preferred state under experimental conditions. Equilibrated structures at 300 K were clustered into three distinct families with similar structural features within a family and with significant root mean square deviations between families. An analysis of secondary structure indicates the Abeta42 peptide conformations are dominated by loops and turns but show some helical structure in the C-terminal hydrophobic tail. A second calculation on Abeta42 in a solvent-free environment yields compact structures turned "inside out" from the solution structures (hydrophobic parts on the outside, polar parts on the inside). Ion mobility experiments on the Abeta42 -3 charge state electrosprayed from solution yield a bimodal arrival time distribution. This distribution can be quantitatively fit using cross-sections from dehydrated forms of the three families of calculated solution structures and the calculated solvent-free family of structures. Implications of the calculations on the early stages of aggregation of Abeta42 are discussed.

Biologists have observed that the presence of divalent metal is essential for the binding of the hormone oxytocin (OT) to its cellular receptor. However, this interaction is not understood on the molecular level. Because conformation is a key factor controlling ligand binding in biomolecule systems, we have used ion mobility experiments and molecular modeling to probe the conformation of the oxytocin-zinc complex. Results show that Zn2+ occupies an octahedral site in the interior of the OT peptide that frees the N-terminus and creates a structured hydrophobic binding site on the peptide exterior; both factors are conducive to binding oxytocin to its receptor.

The amyloid beta-protein (Abeta) is a seminal neuropathic agent in Alzheimer's disease (AD). Recent evidence points to soluble Abeta oligomers as the probable neurotoxic species. Among the naturally occurring Abeta peptides, the 42-residue form Abeta42 is linked particularly strongly with AD, even though it is produced at approximately 10% of the levels of the more abundant 40-residue form Abeta40. Here, we apply mass spectrometry and ion mobility to the study of Abeta42 and its Pro19 alloform. The Phe19 --> Pro19 substitution blocks fibril formation by [Pro19]Abeta42. Evidence indicates that solution-like structures of Abeta monomers are electrosprayed and characterized. Unfiltered solutions of Abeta42 produce only monomers and large oligomers, whereas [Pro19]Abeta42 solutions produce abundant monomers, dimers, trimers, and tetramers but no large oligomers. When passed through a 10,000 amu filter and immediately sampled, Abeta42 solutions produce monomers, dimers, tetramers, hexamers, and an aggregate of two hexamers that may be the first step in protofibril formation. These results are consistent with recently published photochemical cross-linking data and lend support to recent aggregation mechanisms proposed by Bitan, Teplow, and co-workers [J. Biol. Chem. 2003, 278, 34882-34889].

The protein alpha-synuclein, implicated in Parkinson's disease, was studied by combining nano-electrospray ionization (N-ESI) mass spectrometry and ion mobility. It was found that both the charge-state distribution in the mass spectra and the average protein shape deduced from ion mobility data, depend on the pH of the spray solution. Negative-ion N-ESI of pH 7 solutions yielded a broad charge-state distribution from -6 to -16, centered at -11, and ion mobility data consistent with extended protein structures. Data obtained for pH 2.5 solutions, on the other hand, showed a narrow charge-state distribution from -6 to -11, centered at -8, and ion mobilities in agreement with compact alpha-synuclein structures. The data indicated that there are two distinct families of structures: one consisting of relatively compact proteins with eight or less negative charges and one consisting of relatively extended structures with nine or more charges. The average cross section of a-synuclein at pH 2.5 is 33% smaller than for the extended protein sprayed from pH 7 solution. Significant dimer formation was observed when sprayed from pH 7 solution but no dimers were observed from the low pH solution. A plausible mechanism for aggregate formation in solution is proposed.

Noncovalent peptide-peptide and peptide-water interactions in small model systems were examined using an electrospray mass spectrometer equipped with a high-pressure drift cell. The results of these aggregation and hydration experiments were interpreted with the aid of molecular mechanics (MM) and density functional theory (DFT) calculations. The systems investigated include bare deprotonated monomers and dimers [P(1,2)-H](-) and hydrated deprotonated monomers and dimers [P(1,2)-H](-).(H(2)O)(n)() for the peptides dialanine (P = AA) and diglycine (P = GG). Mass spectra indicated that both peptides AA and GG form exclusively dimer ions in the electrospray process. Monomeric ions were generated by high-energy injection of the dimers into the drift cell. Temperature-dependent hydration equilibrium experiments carried out in the drift cell yielded water binding energies ranging from 11.7 (first water molecule) to 7.1 kcal/mol (fourth water) for [AA-H](-) and 11.0 to 7.4 kcal/mol for [GG-H](-). The first water molecule adding to the dimer ions [AA-H](-).(AA) and [GG-H](-).(GG) is bound by 8.4 and 7.5 kcal/mol, respectively. The hydration mass spectra for the monomers and dimers provide a means to compare the ability of water and a neutral peptide to solvate a deprotonated peptide [P-H](-). The data indicate that a similar degree of solvation is achieved by four water molecules, [P-H](-).(H(2)O)(4), or one neutral peptide, [P-H](-).(P). Temperature-dependent kinetics experiments yielded activation energies for dissociation of the dimers [AA-H](-).(AA) and [GG-H](-).(GG) of 34.9 and 32.2 kcal/mol, respectively. MM and DFT calculations carried out for the dialanine system indicated that the dimer binding energy is 24.3 kcal/mol, when the [AA-H](-) and AA products are relaxed to their global minimum structures. However, a value of 38.9 kcal/mol is obtained if [AA-H](-) and AA dissociate but retain the structures of the moieties in the dimer, suggesting the transition state occurs early in the dissociation process. Similar results were found for the diglycine dimer.

A series of gas-phase experiments and extensive theoretical modeling was done on the family of singly protonated peptides AARAA, Ac-AARAA, and AARAA-OMe. (AARAA)H(+) underwent extensive H/D exchange with D(2)O, whereas the other two peptides with blocked termini did not, implying that a salt bridge was involved in the H/D exchange process. Ion mobility measurements and complementary molecular modeling unambiguously identified the 300 K structures of all three protonated peptides as charge solvation structures, not salt bridges. High-level density functional theory calculations indicated the global minimum of (AARAA)H(+) was a charge solvation structure with the lowest-energy salt bridge structure 4.8 kcal/mol higher in energy. Uptake of the first five water molecules of hydration at 260 K showed near identical propensities for all three peptides consistent with a common structural motif. Quantitative measurements of Delta H degrees and Delta S degrees for the first two waters of hydration were very similar for all three peptides, again suggestive of a common structure. A detailed search of the potential energy surface for the singly hydrated (AARAA)H(+) using molecular mechanics and density functional theory approaches indicated a charge solvation structure was the global minimum, but now the lowest-energy salt bridge structure was only 1.8 kcal/mol higher in energy. Importantly, a low-energy transition state connecting the charge solvation and the salt bridge structures was found where the D(2)O molecule facilitated H/D exchange via the relay mechanism. This "relay" transition state was 7 kcal/mol below the (AARAA)H(+) + D(2)O asymptotic energy, suggesting that facile H/D exchange could occur in this system. There was no equivalent low-lying relay mechanism transition state for the (Ac-AARAA)H(+) and (AARAA-OMe)H(+) peptides, consistent with the fact that H/D exchange was not observed. Hence, the combined experimental and theoretical methods confirmed that a salt bridge was involved in the H/D exchange by D(2)O of (AARAA)H(+), but it existed only as a kinetic intermediate, not as a global minimum structure. These findings suggest that caution must be observed in drawing structural conclusions from H/D exchange only. A prescription is given here for understanding both the structural and H/D exchange mechanistic aspects of bare and singly hydrated peptides.

The sequential addition of water molecules to a series of small protonated peptides was studied by equilibrium experiments using electrospray ionization combined with drift cell techniques. The experimental data were compared to theoretical structures of selected hydrated species obtained by molecular mechanics simulations. The sequential water binding energies were measured to be of the order of 7-15 kcal/mol, with the largest values for the first water molecule adding to either a small nonarginine containing peptide (e.g., protonated dialanine) or to a larger peptide in a high charge state (e.g., triply protonated neurotensin). General trends are (a) that the first water molecules are more strongly bound than the following water molecules, (b) that very small peptides (2-3 residues) bind the first few water molecules more strongly than larger peptides, (c) that the first few water molecules bind more strongly to higher charge states than to lower charge states, and (d) that water binds less strongly to a protonated guanidino group (arginine containing peptides) than to a protonated amino group. Experimental differential entropies of hydration were found to be of the order of -20 cal/mol/K although values vary from system to system. At constant experimental conditions the number of water molecules adding to any peptide ion is strongly dependent on the peptide charge state (with higher charge states adding proportionally more water molecules) and only weakly dependent on the choice of peptide. For small peptides molecular mechanics calculations indicate that the first few water molecules add preferentially to the site of protonation until a complete solvation shell is formed around the charge. Subsequent water molecules add either to water molecules of the first solvation shell or add to charge remote functional groups of the peptide. In larger peptides, charge remote sites generally compete more effectively with charge proximate sites even for the first few water molecules.

Conformational data for macromolecules in the gas phase have been obtained by the coupling of a matrix-assisted laser desorption ion source to an ion chromatograph. A series of polyethylene glycol (PEG) polymers "cationized" (converted to a cation) by sodium ions (Na(+)PEG9 to Na(+)PEG19) and a protonated neurotransmitter protein, bradykinin, were studied. Mobilities of Na(+)PEG9 to Na(+)PEG19 are reported. Detailed modeling of Na(+)PEG9 with molecular mechanics methods indicates that the lowest energy structure has the Na(+) ion "solvated" by the polymer chain with seven oxygen atoms as nearest neighbors. The agreement between the model and experiment is within 1 percent for Na(+)PEG9, Na(+)PEG13, and Na(+)PEG17, giving strong support to both the method and the deduced structures. Similar agreement was obtained in initial studies that modeled experimental data for arginine-protonated bradykinin.

The present study assessed the progression rate of periodontal disease over 8 years in a group of 52 adult patients with various forms of cleft lip, alveolus, and palate considered at risk for progression of periodontal disease. Of special interest was the evaluation of periodontal disease progression at sites adjacent to cleft regions compared to changes found at control sites not directly affected by such defects. High incidences of generalized plaque accumulation and bleeding on probing were noted at both examinations in 1979 and 1987. A mean apical shift of the clinical attachment level amounting to 0.2 mm had occurred over the 8-year observation period. A slight apical displacement of the mesial and distal mean crestal alveolar bone was also noted. The rate of progression of periodontal disease over the 8 years was not found to be different at statistically significant levels at cleft sites compared to control sites. However, the results of this study documented that the cumulative periodontal destruction at 26 to 28 years of age was statistically significant and more pronounced at cleft sites as revealed by greater probing pocket depth and loss of clinical attachment. The differences between test and control sites amounted to 0.3 and 0.4 mm respectively for probing depth and 0.6 mm for loss of clinical attachment. In addition, the discrepancy between alveolar bone height and the levels of the clinical attachment at cleft sites demonstrated the presence of a long supracrestal connective tissue attachment adjacent to cleft defects. Therefore, the alveolar bone height as visualized in radiographs at such sites was considered an unreliable diagnostic tool for the assessment of the degree of periodontal destruction.

The periodontal conditions in 19 patients with unilateral cleft lip, alveolus and palate (CLAP) and in 6 patients with bilateral CLAP, were evaluated in 1979 and re-examined in 1987. During these 8 years, these patients were not subjected to any professionally supervised maintenance care program. Pronounced plaque accumulation and high frequency of gingival units exhibiting bleeding on probing were noted in the majority of the patients both in 1979 and 1987, documenting inadequate oral hygiene standards with resulting inflammatory reactions of the periodontal tissues. Progression of periodontal disease over time was assessed as loss of clinical attachment and loss of alveolar bone height. The periodontal destruction was not found to be more severe at cleft sites with a long connective tissue attachment than at control sites not affected by cleft defects. It was concluded that sites with a long supracrestal connective tissue attachment do not seem to be more prone to periodontal destruction, induced by bacterial infection, than sites with a normal length of the supraalveolar fibrous attachment. The results also show that the alveolar bone height, as visualized in radiographs at sites with alveolar defects, is of limited value for the diagnosis of the degree of periodontal destruction at such sites.