Measurement of electrostatic interactions in protein folding with the use of protein charge ladders

This paper describes a new method for the measurement of the role of interactions between charged groups on the energetics of protein folding. This method uses capillary electrophoresis (CE) and protein charge ladders (mixtures of protein derivatives that differ incrementally in number of charged groups) to measure, in a single set of electrophoresis experiments, the free energy of unfolding (DeltaG(D-N)) of alpha-lactalbumin (alpha-LA) as a function of net charge. These same data also yield the hydrodynamic radius, R(H), and net charge measured by CE, Z(CE), of the folded and denatured proteins. Alpha-LA unfolds to a compact denatured state under mildly alkaline conditions; a small increase in R(H) (11%, 2 A) coincides with a large increase in Z(CE) (71%, -4 charge units), relative to the folded state. The increase in Z(CE), in turn, predicts a large pH dependence of free energy of unfolding (-22 kJ/mol per unit increase in pH), due to differences in proton binding in the folded and denatured states. The free energy of unfolding correlates with the square of net charge of the members of the charge ladder. The differential dependence of DeltaG(D-N) on net charge for holo-alpha-LA, (partial differential) DeltaG(D-N)/(partial differential)Z = -0.14Z kJ/mol per unit of charge. This dependence of DeltaG(D-N) on net charge is a result of a net electrostatic repulsion among charge groups on the protein. These results, together with data from pH titrations, show that both the effects of electrostatic repulsion and differences in proton binding in the folded and denatured states can play an important role in the pH dependence of this protein; the relative magnitude of these effects varies with pH. The combination of charge ladders and CE is a rapid and efficient tool that measures the contributions of electrostatics to the energetics of protein folding, and the size and charge of proteins as they unfold. All this information is obtained from a single set of electrophoresis experiments.     

Zinc-porphyrin Solvation in folded and unfolded states of Zn-cytochrome c

After a brief review of the use of photochemical triggers and heme metal substitution to probe the folding dynamics of cytochrome c, we present new results on the photophysics and photochemistry of folded and unfolded states of the zinc-substituted protein (Zn-cyt c). Our measurements of Zn-cyt c triplet state decay kinetics reveal a systematic isotope effect on lifetimes: the decay in the folded protein (tau(H)2(O) approximately 10 ms) is only modestly affected by isotopically substituted buffers (k(H)2(O)/k(D)2(O) = 1.2), whereas a reduced triplet lifetime (approximately 1.3 ms) and greater isotope effect (1.4) were found for the chemically denatured, fully unfolded protein. The shortest lifetime (0.1-0.4 ms) and greatest isotope effect (1.5) were found for a fully exposed model compound, zinc-substituted N-acetyl-microperoxidase-8 (ZnAcMP8), implying that the unfolded protein provides some protection to the Zn-porphyrin group even under fully denaturing conditions. Further evidence for partial structure in unfolded Zn-cyt c comes from bimolecular quenching experiments using Ru(NH(3))(6)(3+) as an external Zn-porphyrin triplet state quencher. In the presence of quencher, partially unfolded protein at midpoint guanidinium chloride (GdmCl) and urea concentrations exhibits biphasic triplet decay kinetics, a fast component corresponding to an extended, solvent-exposed state (6.6 x 10(8) M(-1) s(-1) in GdmCl, 6.3 x 10(8) M(-1) s(-1) in urea) and a slow component attributable to a compact, relatively solvent-inaccessible, state (5.9 x 10(7) M(-1) s(-1) in GdmCl, 8.6 x 10(6) M(-1) s(-1) in urea). The variation in Zn-porphyrin solvation for the compact states in the two denaturants reveals that the cofactor in the partially unfolded protein is better protected in urea solutions.     

pH-induced structural transitions of caseins

Caseins are relatively small (molecular mass approximately 20 kDa), unstructured milk proteins of which the main components are referred to as alpha(s)-, beta- and kappa-casein. All three components lack a compact folded conformation, which can be ascribed to a combination of their low overall hydrophobicity and high net charge. Structural transitions of the three caseins in response to variation of pH were investigated using fluorescence and circular dichroism (CD) spectroscopy. Tryptophan emission parameters (intensity and wavelength of emission maximum) and CD spectra showed that at neutral and alkaline pH the caseins exist predominantly in random coil conformation. As the solvent is made acidic the added protons compensate the negative charges on the caseins and reduce the repulsion between like charged residues, allowing the casein chains to fold. At the pI (pH 4-5), the net charge on the protein tends to zero and the protein should approach its maximally structured state. Below pI, the uncompensated charges and their interactions reappear, resulting in slackening of the compact structure and formation of a partially unfolded intermediate. These conclusions were borne out by the biphasic pH-dependence of the fluorescence emission parameters of Trp as well as of ANS incubated with the caseins. Measurement of the efficiency of energy transfer between Trp (donor) and ANS (acceptor) and of the CD spectra of caseins as functions of pH were also consistent with this scenario.     

Evidence for unfolding and refolding of gas-phase cytochrome <Emphasis Type="Italic">c</Emphasis> ions in a Paul trap

The folding pathways of gas-phase cytochrome c ions produced by electrospray ionization have been studied by an ion trapping/ion mobility technique that allows conformations to be examined over extended timescales (10 ms to 10 s). The results show that the +9 charge state emerges from solution as a compact structure and then rapidly unfolds into several substantially more open structures, a transition that requires 30-60 ms; over substantially longer timescales (250 ms to 10 s) elongated states appear to refold into an array of folded structures. The new folded states are less compact than those that are apparent during the initial unfolding. Apparently, unfolding to highly open conformations is a key step that must occur before +9 ions can sample more compact states that are stable at longer times.     

Conformer-dependent proton-transfer reactions of ubiquitin ions

The conformations of ubiquitin ions before and after being exposed to proton transfer reagents have been studied by using ion mobility/mass spectrometry techniques. Ions were produced by electrospray ionization and exposed to acetone, acetophenone, n-butylamine, and 7-methyl-1,5,7-triazabicyclo[4.4.0]dec-5-ene. Under the conditions employed, the +4 to +13 charge states were formed and a variety of conformations, which we have characterized as compact, partially folded, and elongated, have been observed. The low charge state ions have cross sections that are similar to those calculated for the crystal conformation. High charge states favor unfolded conformations. The ion mobility distributions recorded after ions have been exposed to each base show that the lowest charge state that is formed during proton-transfer reactions favors a compact conformation. More open conformations are observed for the higher charge states that remain after reaction. The results show that for a given charge state, the apparent gas-phase acidities of the different conformations are ordered as compact < partially folded < elongated.     

A minimalist model for exploring conformational effects on the electrospray charge state distribution of proteins

The electrospray ionization (ESI) charge state distribution of proteins is highly sensitive to the protein structure in solution. Unfolded conformations generally form higher charge states than tightly folded structures. The current study employs a minimalist molecular dynamics model for simulating the final stages of the ESI process in order to gain insights into the physical reasons underlying this empirical relationship. The protein is described as a string of 27 beads ("residues"), 9 of which are negatively charged and represent possible protonation sites. The unfolded state of this bead string is a random coil, whereas the native conformation adopts a compact fold. The ESI process is simulated by placing the protein inside a solvent droplet with a 2.5 nm radius consisting of 1600 Lennard-Jones particles. In addition, the droplet contains 14 protons which are modeled as highly mobile point charges. Disintegration of the droplet rapidly releases the protein into the gas phase, resulting in average charge states of 4.8+ and 7.4+ for the folded and unfolded conformation, respectively. The protonation probabilities of individual residues in the folded state reveal a characteristic pattern, with values ranging from 0.2 to 0.8. In contrast, the protonation probabilities of the unfolded protein are more uniform and cover the range from 0.8 to 1.0. The origin of these differences can be traced back to a combination of steric and electrostatic effects. Residues exhibiting a small accessible surface area are less likely to capture a proton, an effect that is exacerbated by partial electrostatic shielding from nearby positive residues. Conversely, sites that are sterically exposed are associated with electrostatic funnels that greatly increase the likelihood of protonation. Unfolding enhances the steric and electrostatic exposure of protonation sites, thereby causing the protein to capture a greater number of protons during the droplet disintegration process.     

Role of opposite charges in protein electrospray ionization mass spectrometry

The conformation dependence of protein spectra recorded by electrospray ionization mass spectrometry (ESI-MS) is an interesting and useful phenomenon, whose origin is still the object of debate. Different mechanisms have been invoked in the attempt to explain the lower charge state of folded versus unfolded protein ions in ESI-MS, such as electrostatic repulsions, solvent accessibility, charge availability, and native-like interactions. In this work we try to subject to direct experimental test the hypothesis that conformation-dependent neutralization of charges with polarity opposite to the net charge of the protein ion could play a critical role in such an effect. We present results of time-of-flight nano-ESI-MS on the peptide angiotensin II, indicating that negative charges of carboxylate groups can contribute to spectra recorded in positive-ion mode when stabilized by favorable electrostatic interactions, which is the central assumption of our hypothesis. Comparison of horse and spermwhale myoglobin (Mb) shows that changing the total number of basic residues within a given three-dimensional structure shifts the charge-state distribution (CSD) of the folded protein in positive-ion mode. This result appears to be in contrast to models in which electrostatic repulsions or availability of charges in the ESI droplets represent the limiting factor for the ionization of folded protein ions in ESI-MS. At the same time, it suggests a role of acidic residues in conformational effects in positive-ion mode. Furthermore, an attempt is made to rationalize those cases in which, in contrast, the main charge state observed in ESI-MS under non-denaturing conditions deviates considerably from the net charge expected on the basis of the amino-acid composition. These cases usually correspond to proteins with quite balanced content in basic and acidic residues, suggesting that this might be a factor influencing their charging behavior in ESI-MS. Experiments on mutants of ribonuclease Sa (RNase Sa) reveal that progressively reducing the excess of acidic residues, replacing them by lysine, causes almost no shift in the spectrum of the folded protein in negative-ion mode. Analogously, variants with an excess of three or five basic residues give similar spectra in positive-ion mode. These results indicate a lower limit to the extent of ionization observable by ESI-MS (6- or 8+ in the case of RNase Sa in water). Below such limit of net charge, changes in the relative amount of ionizable side chains do not affect the qualitative features of the observed CSDs. A progressive loss of signal intensity caused by the mutations in negative-ion mode suggests that low charge states might also be counterselected, even within the m/z range theoretically accessible to the instrument.     

Fast folding of a four-helical bundle protein

The FK506-FKBP12 binding-domain of the kinase FRAP (FRB) forms a classic up-down four-helical bundle. The folding pathway of this protein has been investigated using a combination of equilibrium and kinetic studies. The native state of the protein is stable with respect to the unfolded state by some 7 kcal mol(-1) at pH 6.0, 10 degrees C. A kinetic analysis of unfolding and refolding rate constants as a function of chemical denaturant concentration suggests that an intermediate state may be populated during folding at low concentrations of denaturant. The presence of this intermediate state is confirmed by refolding experiments performed in the presence of the hydrophobic dye 8-anilinonaphthalene-1 sulfonate (ANS). ANS binds to the partially folded intermediate state populated during the folding of FRB and undergoes a large change in fluorescence that can be detected using stopped-flow techniques. Analysis of the kinetic data suggests that the intermediate state is compact and it may even be a misfolded species that has to partially unfold before it can reach the transition state. Folding and unfolding rate constants in water are approximately 150-200 s(-1) and 0.005-0.06 s(-1), respectively, at neutral pH and 10 degrees C. The folding of FRB is somewhat slower than for other all-helical proteins, probably as a consequence of the formation of a metastable intermediate state. The folding rate constant in the absence of any populated intermediate can be estimated to be 8800 s(-1). Despite the presence of an intermediate state, which effectively slows folding, the protein still folds rapidly with a half-life of 5 ms at 10 degrees C. The dependence of the rate constants on denaturant concentration indicates that the transition state for folding is compact with some 80% of the surface area exposed in the unfolded state buried in the transition state. Data presented for FRB is compared with kinetic data obtained for other all-helical proteins.     

2,2,2-trifluoroethanol-induced molten globule state of concanavalin a and energetics of 8-anilinonaphthalene sulfonate binding: calorimetric and spectroscopic investigation

The interaction of 2,2,2-trifluoroethanol (TFE) with concanavalin A has been investigated by using a combination of differential scanning calorimetry, isothermal titration calorimetry (ITC), circular dichroism (CD), and fluorescence spectroscopy at pH 2.5 and 5.2. All of the calorimetric transitions at both the pH values were found to be irreversible. In the presence of 4 mol kg(-1) TFE at pH 2.5, concanavalin A is observed to be in a partially folded state with significant loss of native tertiary structure. The loss of specific side chain interactions in the transition from native to the TFE-induced partially folded state is demonstrated by the loss of cooperative thermal transition and reduction of the CD bands in the aromatic region. Acrylamide quenching, 8-anilinonaphthalene sulfonate (ANS) binding, and energy transfer also suggest that in the presence of 4 mol kg(-1) TFE at pH 2.5 concanavalin A is in a molten globule state. ITC has been used for the first time to characterize the energetics of ANS binding to the molten globule state. ITC results indicate that the binding of ANS to the molten globule state and acid-induced state at pH 2.5 displays heterogeneity with two classes of non-interacting binding sites. The results provide insights into the role of hydrophobic and electrostatic interactions in the binding of ANS to concanavalin A. The results also demonstrate that ITC can be used to characterize the partially folded states of the protein both qualitatively and quantitatively.     

Electrospray ionization mass spectra of acyl carrier protein are insensitive to its solution phase conformation

Electrospray ionization mass spectrometry (ESI-MS) can be used to monitor conformational changes of proteins in solution based on the charge state distribution (CSD) of the corresponding gas-phase ions, although relatively few studies of acidic proteins have been reported. Here, we have compared the CSD and solution structure of recombinant Vibrio harveyi acyl carrier protein (rACP), a small acidic protein whose secondary and tertiary structure can be manipulated by pH, fatty acylation, and site-directed mutagenesis. Circular dichroism and intrinsic fluorescence demonstrated that apo-rACP adopts a folded helical conformation in aqueous solution below pH 6 or in 50% acetonitrile/0.1% formic acid, but is unfolded at neutral and basic pH values. A rACP mutant, in which seven conserved acidic residues were replaced with their corresponding neutral amides, was folded over the entire pH range of 5 to 9. However, under the same solvent conditions, both wild type and mutant ACPs exhibited similar CSDs (6(+)-9(+) species) at all pH values. Covalent attachment of myristic acid to the phosphopantetheine prosthetic group of rACP, which is known to stabilize a folded conformation in solution, also had little influence on its CSD in either positive or negative ion modes. Overall, our results are consistent with ACP as a "natively unfolded" protein in a dynamic conformational equilibrium, which allows access to (de)protonation events during the electrospray process.     

Transfer of structural elements from compact to extended states in unsolvated ubiquitin

Multidimensional ion mobility spectrometry techniques (IMS-IMS and IMS-IMS-IMS) combined with mass spectrometry are used to study structural transitions of ubiquitin ions in the gas phase. It is possible to select and activate narrow distributions of compact and partially folded conformation types and examine new distributions of structures that are formed. Different compact conformations unfold, producing a range of new partially folded states and three resolvable peaks associated with elongated conformers. Under gentle activation conditions, the final populations of the three elongated forms depend on the initial structures of the selected ions. This requires that some memory of the compact state (most likely secondary structure) is preserved along the unfolding pathway. Activation of selected, partially folded intermediates (formed from specific compact states) leads to elongated state populations that are consistent with the initial selected compact form-evidence that intermediates not only retain elements of initial structure but also are capable of transmitting structure to final states.     

Do Charge State Signatures Guarantee Protein Conformations?

The extent to which proteins in the gas phase retain their condensed-phase structure is a hotly debated issue. Closely related to this is the degree to which the observed charge state reflects protein conformation. Evidence from electron capture dissociation, hydrogen/deuterium exchange, ion mobility, and molecular dynamics shows clearly that there is often a strong correlation between the degree of folding and charge state, with the most compact conformations observed for the lowest charge states. In this article, we address recent controversies surrounding the relationship between charge states and folding, focussing also on the manipulation of charge in solution and its effect on conformation. 'Supercharging' reagents that have been used to effect change in charge state can promote unfolding in the electrospray droplet. However for several protein complexes, supercharging does not appear to perturb the structure in that unfolding is not detected. Consequently, a higher charge state does not necessarily imply unfolding. Whilst the effect of charge manipulation on conformation remains controversial, there is strong evidence that a folded, compact state of a protein can survive in the gas phase, at least on a millisecond timescale. The exact nature of the side-chain packing and secondary structural elements in these compact states, however, remains elusive and prompts further research.     

Folding transition of a single semiflexible polyelectrolyte chain through toroidal bundling of loop structures

We consider how the DNA coil-globule transition progresses via the formation of a toroidal ring structure. We formulate a theoretical model of this transition as a phenomenon in which an unstable single loop generated as a result of thermal fluctuation is stabilized through association with other loops along a polyelectrolyte chain. An essential property of the chain under consideration is that it follows a wormlike chain model. A toroidal bundle of loop structures is characterized by a radius and a winding number. The statistical properties of such a chain are discussed in terms of the free energy as a function of the fraction of unfolded segments. We also present an actual experimental observation of the coil-globule transition of single giant DNA molecules, T4 DNA (165.5 kbp), with spermidine (3+), where intrachain phase segregation appears at a NaCl concentration of more than 10 mM. Both the theory and experiments lead to two important points. First, the transition from a partially folded state to a completely folded state has the characteristics of a continuous transition, while the transition from an unfolded state to a folded state has the characteristics of a first-order phase transition. Second, the appearance of a partially folded structure requires a folded structure to be less densely packed than in the fully folded compact state.     

Measuring pK(a) values in protein folding transition state ensembles by NMR spectroscopy

Protein folding kinetic data have been obtained for the marginally stable N-terminal SH3 domain of the Drosophila protein drk as a function of pH in order to investigate the electrostatic properties of Asp8 in the folding transition state ensemble. The slow exchange between folded and unfolded forms of the protein gives rise to separate NMR resonances for both folded and unfolded states at equilibrium. As a result, kinetic data can be derived from magnetization transfer between these two states without the need for denaturants. Using the fact that ionization of Asp8 dominates the electrostatic behavior of the protein between pH 2 and 3, along with pKa values for titrating groups in both folded and unfolded states that have been determined in a previous study, values of 2.9 +/- 0.1 and 3.3 +/- 0.2 are obtained for the pKa of Asp8 in the transition state for the wild-type protein and for a His7Ala mutant, respectively. The data are consistent with the partial formation in the transition state ensemble of an Asp8 side chain carboxylate-a Lys21 backbone amide interaction that represents a highly conserved contact in folded SH3 domains.     

Study of metal ion labeling of the conformational and charge states of lysozyme by ion mobility mass spectrometry

The efficiency of Zn(2+), Cu(2+), Ni(2+), Co(2+), Fe(2+) or Mn(2+) labeling of the conformational and charge states of lysozyme was studied in H(2)O solvent at pH 2.5-6.8. Labeling of lysozyme was conducted with 50 M, 100 M and 500 M excess of the metal ion, resulting in the number of metal ions attached to lysozyme increasing two-fold over this range. At pH 6.2-6.8, Zn(2+), Cu(2+), Ni(2+), Co(2+) and Mn(2+) labeled the highly folded 7+ conformer and the 8+ and 9+ partially unfolded conformers of lysozyme with the same number of metal ion tags, with only Fe(2+) exhibiting no labeling. Lysozyme conserved its charge after metal ion labeling which shows at each charge state the divalent metal ion is replacing two protons. As the pH is lowered to 4.7-5.0 and 2.5-2.9, the labeling of lysozyme by Zn(2+), Cu(2+), Ni(2+), Co(2+) or Mn(2+) decreased in efficiency due to increased competition from protons for the aspartate and glutamate binding sites. The metal ions preferentially labeled the highly folded 7+ and partially unfolded 8+ conformers, but labeling decreased as the charge of lysozyme increased. In contrast to the other metal ions, Fe(2+) exhibited labeling of lysozyme only at the lowest pH of 2.8. At higher pH, the oxidation of Fe(2+) and formation of hydroxy-bridged complexes probably make the Fe(2+) unreactive towards lysozyme.     

Probing electrostatic interactions and structural changes in highly charged protein polyanions by conformer-selective photoelectron spectroscopy

We have recorded the first conformer-selective photoelectron spectra of a protein polyanion in the gas-phase. Bovine cytochrome c protein was studied in 8 different negative charge states ranging from 5- to 12-. Electron binding energies were extracted for all charge states and used as a direct probe of intramolecular Coulomb repulsion. Comparison of experimental results with simulations shows that the experimental outcome can be reproduced with a simple electrostatic model. Energetics are consistent with a structural transition from a folded to an unfolded conformational state of the protein as the number of charges increases. Furthermore, the additional ion-mobility data show that the onset of unfolding can be assigned to charge state 6- where three conformers can be distinguished.     

Surface Induced Dissociation Yields Quaternary Substructure of Refractory Noncovalent Phosphorylase B and Glutamate Dehydrogenase Complexes

Ion mobility (IM) and tandem mass spectrometry (MS/MS) coupled with native MS are useful for studying noncovalent protein complexes. Collision induced dissociation (CID) is the most common MS/MS dissociation method. However, some protein complexes, including glycogen phosphorylase B kinase (PHB) and L-glutamate dehydrogenase (GDH) examined in this study, are resistant to dissociation by CID at the maximum collision energy available in the instrument. Surface induced dissociation (SID) was applied to dissociate the two refractory protein complexes. Different charge state precursor ions of the two complexes were examined by CID and SID. The PHB dimer was successfully dissociated to monomers and the GDH hexamer formed trimeric subcomplexes that are informative of its quaternary structure. The unfolding of the precursor and the percentages of the distinct products suggest that the dissociation pathways vary for different charge states. The precursors at lower charge states (+21 for PHB dimer and +27 for GDH hexamer) produce a higher percentage of folded fragments and dissociate more symmetrically than the precusors at higher charge states (+29 for PHB dimer and +39 for GDH hexamer). The precursors at lower charge state may be more native-like than the higher charge state because a higher percentage of folded fragments and a lower percentage of highly charged unfolded fragments are detected. The combination of SID and charge reduction is shown to be a powerful tool for quaternary structure analysis of refractory noncovalent protein complexes, as illustrated by the data for PHB dimer and GDH hexamer.

A fast flow tube study of gas phase H/D exchange of multiply protonated ubiquitin

An electrospray ionization (ESI)/fast-flow technique has been applied to the study of gas phase hydrogen/deuterium (H/D) exchange kinetics. Multiply charged ubiquitin ions [ubiquitin + nH](n)(+), in charge states n = 7-13, were reacted with ND(3). The behavior of ND(3) as exchange reagent is different from that of the previously studied reagents, D(2)O and CH(3)OD. Contrary to those, the maximum number of exchanged hydrogen atoms and the overall exchange rate were observed to increase with increasing charge state of the ubiquitin ions. The results are reagent-dependent because the exchange mechanisms are different for the different reagents. This observation is in agreement with a recent conclusion by Beauchamp and co-workers that contrary to the assumption often expressed in earlier studies, H/D exchange kinetics may not directly reflect ion structures. The results for all three reagents are, however, consistent with observations of previous ion mobility experiments that with increasing charge state the conformers change from more compact, partially folded structures to elongated nearly linear ones. H/D exchange of (ubiquitin + 13H)(13+) with ND(3) leads to two separated ion populations reflecting the possible existence of two conformers with different exchange rates. The ions (ubiquitin + 8H)(8+) and (ubiquitin + 11H)(11+) represent a partially folded structure and an unfolded structure, respectively, and were studied in greater detail. The relative abundances of ions were measured in steps of 0.5 m/z (mass-to-charge ratio), as a function of the ND(3) flow rate. The experimental results were simulated by computer fitted curves based on a recently developed algorithm. The algorithm allows the extraction of sets of grouped rate constants. Eight rate constant groups were deduced for each of the two ions. These rate constants correspond to 32 and 44 H/D exchanges for the 8+ and 11+ charged ions, respectively. The results indicate higher individual rates for most of the exchanged atoms in the 11+ ion compared to the 8+ ion.     

Large anhydrous polyalanine ions: evidence for extended helices and onset of a more compact state.

Ion mobility measurements and molecular modeling calculations have been used to examine the conformations of large multiply charged polyalanine peptides. Two series of [Ala(n)+3H](3+) conformations which do not interconvert during the 10 to 30 ms experimental timescales are observed: a family of elongated structures for n = 18 to 39 and a series of more compact conformations for n = 24 to 41. The more compact state becomes the dominant conformer type for n > 32. Molecular modeling studies and comparisons of calculated collision cross sections with experiment indicate that the elongated ions have extended helical conformations. We suggest that the more compact state corresponds to a new conformer type: a folded hinged helix-coil state in which helical and coil regions have similar physical dimensions. The competition between extended and compact states is rationalized by considering differences in charge stabilization and entropy.     

The effects of cation adduction upon the conformation of three-helix bundle protein domains

The ubiquitin-binding, three-helix bundle domains of the proteins ubiquilin 1 (UQ1) and hHR23A both exhibited remarkably high, but discrete, ammonium ion adduction when electrosprayed from aqueous ammonium acetate. The degree of adduction was highly charge state dependent with, unusually, the lowest charge states (+3 for UQ1 and +4 for hHR23A) showing almost no adducts and the highest charge states (+5 for UQ1 and +6 for hHR23A) exhibiting adduction with two ammonium cations as the most abundant form. As the charge state of protein ions produced by electrospray ionisation (ESI) is related to solvent-accessible surface area we inferred that the ammonium-carrying ions were of a more open conformation than their protonated counterparts. This was confirmed by ESI-travelling wave ion mobility spectrometry-mass spectrometry (TWIMS-MS), which showed that, although the purely protonated ions were compact, their equivalents bearing one or two ammonium adducts exhibited populations of significantly larger collisional cross section (CCS). We postulate that complexation with the ammonium cation may disrupt a key salt bridge(s) in the compact structure. A similar effect is observed with mono-sodium ion adduction, but this is diminished with each additional sodium ion in the complex to produce more compact structures.