Protein Cold Denaturation as Seen From the Solvent

Spatially resolved protein hydrogen exchange measured by subzero-cooled chip-based nanoelectrospray ionization tandem mass spectrometry

Mass spectrometry has become a valuable method for studying structural dynamics of proteins in solution by measuring their backbone amide hydrogen/deuterium exchange (HDX) kinetics. In a typical exchange experiment one or more proteins are incubated in deuterated buffer at physiological conditions. After a given period of deuteration, the exchange reaction is quenched by acidification (pH 2.5) and cooling (0 °C) and the deuterated protein (or a digest thereof) is analyzed by mass spectrometry. The unavoidable loss of deuterium (back-exchange) that occurs under quench conditions is undesired as it leads to loss of information. Here we describe the successful application of a chip-based nanoelectrospray ionization mass spectrometry top-down fragmentation approach based on cooling to subzero temperature (-15 °C) which reduces the back-exchange at quench conditions to very low levels. For example, only 4% and 6% deuterium loss for fully deuterated ubiquitin and β(2)-microglobulin were observed after 10 min of back-exchange. The practical value of our subzero-cooled setup for top-down fragmentation HDX analyses is demonstrated by electron-transfer dissociation of ubiquitin ions under carefully optimized mass spectrometric conditions where gas-phase hydrogen scrambling is negligible. Our results show that the known dynamic behavior of ubiquitin in solution is accurately reflected in the deuterium contents of the fragment ions.

Mutational analysis of m-values as a strategy to identify cold-resistant substructures of the protein ensemble

Characterizing the native ensemble of protein is an important yet difficult objective of structural biology. The structural dynamics of protein macromolecules play key roles in biological function, but the short lifetimes and low population of near-native states of the protein ensemble limit their ability to be studied directly. In part to address such issues, it was shown recently that the cooperative substructures that populate a protein ensemble could be ascertained by NMR methods performed at very cold temperatures. What is presented here is an argument that these same substructures can also be determined by denaturant-induced unfolding studies performed on protein at room temperature. Data supporting this argument are given for Staphylococcal nuclease, chymotrypsin inhibitor 2, and ubiquitin. The observation of an agreement between the thermodynamics of the protein ensemble simulated under very cold temperatures to the apparent sensitivity of the ensemble to chemical denaturants at room temperature also suggests that the overall structural-thermodynamic character of an ensemble is surprisingly robust and preserved even in the presence of strong denaturing conditions.

Mapping the hydration dynamics of ubiquitin

The nature of water's interaction with biomolecules such as proteins has been difficult to examine in detail at atomic resolution. Solution NMR spectroscopy is potentially a powerful method for characterizing both the structural and temporal aspects of protein hydration but has been plagued by artifacts. Encapsulation of the protein of interest within the aqueous core of a reverse micelle particle results in a general slowing of water dynamics, significant reduction in hydrogen exchange chemistry and elimination of contributions from bulk water thereby enabling the use of nuclear Overhauser effects to quantify interactions between the protein surface and hydration water. Here we extend this approach to allow use of dipolar interactions between hydration water and hydrogens bonded to protein carbon atoms. By manipulating the molecular reorientation time of the reverse micelle particle through use of low viscosity liquid propane, the T(1ρ) relaxation time constants of (1)H bonded to (13)C were sufficiently lengthened to allow high quality rotating frame nuclear Overhauser effects to be obtained. These data supplement previous results obtained from dipolar interactions between the protein and hydrogens bonded to nitrogen and in aggregate cover the majority of the molecular surface of the protein. A wide range of hydration dynamics is observed. Clustering of hydration dynamics on the molecular surface is also seen. Regions of long-lived hydration water correspond with regions of the protein that participate in molecular recognition of binding partners suggesting that the contribution of the solvent entropy to the entropy of binding has been maximized through evolution.

Simulations of the confinement of ubiquitin in self-assembled reverse micelles

We describe the effects of confinement on the structure, hydration, and the internal dynamics of ubiquitin encapsulated in reverse micelles (RM). We performed molecular dynamics simulations of the encapsulation of ubiquitin into self-assembled protein/surfactant reverse micelles to study the positioning and interactions of the protein with the RM and found that ubiquitin binds to the RM interface at low salt concentrations. The same hydrophobic patch that is recognized by ubiquitin binding domains in vivo is found to make direct contact with the surfactant head groups, hydrophobic tails, and the iso-octane solvent. The fast backbone N-H relaxation dynamics show that the fluctuations of the protein encapsulated in the RM are reduced when compared to the protein in bulk. This reduction in fluctuations can be explained by the direct interactions of ubiquitin with the surfactant and by the reduced hydration environment within the RM. At high concentrations of excess salt, the protein does not bind strongly to the RM interface and the fast backbone dynamics are similar to that of the protein in bulk. Our simulations demonstrate that the confinement of protein can result in altered protein dynamics due to the interactions between the protein and the surfactant.

Protein dynamics and pressure: what can high pressure tell us about protein structural flexibility?

After a brief overview of NMR and X-ray crystallography studies on protein flexibility under pressure, we summarize the effects of hydrostatic pressure on the native fold of azurin from Pseudomonas aeruginosa as inferred from the variation of the intrinsic phosphorescence lifetime and the acrylamide bimolecular quenching rate constants of the buried Trp residue. The pressure/temperature response of the globular fold and modulation of its dynamical structure is analyzed both in terms of a reduction of internal cavities and of the hydration of the polypeptide. The study of the effect of two single point cavity forming mutations, F110S and I7S, on the unfolding volume change (ΔV(0)) of azurin and on the internal dynamics of the protein fold under pressure demonstrate that the creation of an internal cavity will enhance the plasticity and lower the stability of the globular structure. This article is part of a Special Issue entitled: Protein Dynamics: Experimental and Computational Approaches.

The cold denatured state of the C-terminal domain of protein L9 is compact and contains both native and non-native structure

Cold denaturation is a general property of globular proteins, and the process provides insight into the origins of the cooperativity of protein folding and the nature of partially folded states. Unfortunately, studies of protein cold denaturation have been hindered by the fact that the cold denatured state is normally difficult to access experimentally. Special conditions such as addition of high concentrations of denaturant, encapsulation into reverse micelles, the formation of emulsified solutions, high pressure, or extremes of pH have been applied, but these can perturb the unfolded state of proteins. The cold denatured state of the C-terminal domain of the ribosomal protein L9 can be populated under native-like conditions by taking advantage of a destabilizing point mutation which leads to cold denaturation at temperatures above 0 degrees C. This state is in slow exchange with the native state on the NMR time scale. Virtually complete backbone (15)N, (13)C, and (1)H as well as side-chain (13)C(beta) and (1)H(beta) chemical shift assignments were obtained for the cold denatured state at pH 5.7, 12 degrees C. Chemical shift analysis, backbone N-H residual dipolar couplings, amide proton NOEs, and R(2) relaxation rates all indicate that the cold denatured state of CTL9 (the C-terminal domain of the ribosomal protein L9) not only contains significant native-like secondary structure but also non-native structure. The regions corresponding to the two native alpha-helices show a strong tendency to populate helical Phi and Psi angles. The segment which connects alpha-helix 2 and beta-strand 2 (residues 107-124) in the native state exhibits a significant preference to form non-native helical structure in the cold denatured state. The structure observed in the cold denatured state of the I98A mutant is similar to that observed in the pH 3.8 unfolded state of wild type CTL9 at 25 degrees C, suggesting that it is a robust feature of the denatured state ensemble of this protein. The implications for protein folding and for studies of cold denatured states are discussed.

Cold denaturation of monoclonal antibodies

The susceptibility of monoclonal antibodies (mAbs) to undergo cold denaturation remains unexplored. In this study, the phenomenon of cold denaturation was investigated for a mAb, mAb1, through thermodynamic and spectroscopic analyses. Tryptophan fluorescence and circular dichroism (CD) spectra were recorded for the guanidine hydrochloride (GuHCl)-induced unfolding of mAb1 at pH 6.3 at temperatures ranging from -5 to 50 degrees C. A three-state unfolding model incorporating the linear extrapolation method was fit to the fluorescence data to obtain an apparent free energy of unfolding, DeltaG(u), at each temperature. CD studies revealed that mAb1 exhibited polyproline II helical structure at low temperatures and at high GuHCl concentrations. The Gibbs-Helmholtz expression fit to the DeltaG(u) versus temperature data from fluorescence gave a DeltaC(p) of 8.0 kcal mol(-1) K(-1), a maximum apparent stability of 23.7 kcal mol(-1) at 18 degrees C, and an apparent cold denaturation temperature (T(CD)) of -23 degrees C. DeltaG(u) values for another mAb (mAb2) with a similar framework exhibited less stability at low temperatures, suggesting a depressed protein stability curve and a higher relative T(CD). Direct experimental evidence of the susceptibility of mAb1 and mAb2 to undergo cold denaturation in the absence of denaturant was confirmed at pH 2.5. Thus, mAbs have a potential to undergo cold denaturation at storage temperatures near -20 degrees C (pH 6.3), and this potential needs to be evaluated independently for individual mAbs.