ABSTRACT
ß-casein undergoes a reversible endothermic self-association, forming protein micelles of limited size. In its functional state, a single ß-casein monomer is unfolded, which creates a high structural flexibility, which is supposed to play a major role in preventing the precipitation of calcium phosphate particles. We characterize the structural flexibility in terms of nanosecond molecular motions, depending on the temperature by quasielastic neutron scattering. Our major questions are: Does the self-association reduce the chain flexibility? How does the dynamic spectrum of disordered caseins differ from a compactly globular protein? How does the dynamic spectrum of ß-casein in solution differ from that of a protein in hydrated powder states? We report on two relaxation processes on a nanosecond and a sub-nanosecond timescale for ß-casein in solution. Both processes are analyzed by Brownian oscillator model, by which the spring constant can be defined in the isotropic parabolic potential. The slower process, which is analyzed by neutron spin echo, seems a characteristic feature of the unfolded structure. It requires bulk solvent and is not seen in hydrated protein powders. The faster process, which is analyzed by neutron backscattering, has a smaller amplitude and requires hydration water, which is also observed with folded proteins in the hydrated state. The self-association had no significant influence on internal relaxation, and thus, a ß-casein protein monomer flexibility is preserved in the micelle. We derive spring constants of the faster and slower motions of ß-caseins in solution and compared them with those of some proteins in various states (folded or hydrated powder).
Subject(s)
Caseins , Micelles , Neutrons , Spectrum Analysis , WaterABSTRACT
Pressure is a ubiquitous physical parameter in life and is commonly used in the life sciences to study new protein folding pathways or association-dissociation phenomena. In this paper, an investigation of the influence of pressure on hemoglobin, a multimeric protein, at the picosecond time scale is presented using time-of-flight neutron scattering. The aim is to observe the influence of pressure on the translational diffusion and internal motions of hemoglobin in a concentrated solution and a possible dissociation of the subunits as suggested by Pin et al. (Biochemistry 29:9194, 1990) using fluorescence spectroscopy. A new flat 2 kbar pressure cell made of an aluminum alloy has been used, which allowed the effect of pressure to be studied with minimum background contribution. Within this range of pressure, the effect of this physical parameter on global diffusion can be explained in terms of the change in the water buffer viscosity and an oligomerization of hemoglobin subunits, whereas the internal motions were less affected.
Subject(s)
Hemoglobin Subunits/chemistry , Neutron Diffraction/methods , Pressure , Scattering, Radiation , Diffusion , Humans , Motion , Protein Conformation , ViscosityABSTRACT
Caseins form heterogeneous micelles composed of three types of disordered protein chains (α, ß, κ), which include protein-bound calcium phosphate particles. We probe the stability limits of the micelle by applying hydrostatic pressure. The resulting changes of the size distribution and the average molecular weight are recorded in situ with static and dynamic light scattering. Pressure induces irreversible dissociation of the micelles into monomers above a critical value depending on their size. The critical pressure increases with temperature, pH, and calcium concentration due to the interplay of hydrophobic and electrostatic interactions. The pressure transition curves are biphasic, reflecting the equilibrium of two micelle states with different stability, average size, entropy, and calcium bound. The fast process of pressure dissociation is used to probe the slow equilibrium of the two micelle states under various conditions. Binding and release of ß-casein from the micelle is suggested as the molecular mechanism of stabilization associated with the two states. In situ FTIR spectroscopy covering the P-O stretching region indicates that bound calcium phosphate particles are released from serine phosphate residues at pressures above 100 MPa. The resulting imbalance of charge triggers the complete decomposition of the micelle.
Subject(s)
Caseins/chemistry , Light , Micelles , Pressure , Scattering, Radiation , Animals , Calcium/chemistry , Hydrogen-Ion Concentration , Protein Conformation , Protein Stability , Spectroscopy, Fourier Transform Infrared , TemperatureABSTRACT
Polarization analysis was used to separate experimentally the coherent and spin-incoherent nuclear static scattering functions, from a representative set of samples of interest for protein studies. This method had so far limited application in the study of amorphous materials, despite the relevance of the information that it provides. It allows, for instance, the experimental determination of the structure factor of materials containing a significant amount of hydrogen atoms, avoiding the contamination of measurements by a non-negligible incoherent background. Knowledge of the relative importance of the coherent and incoherent terms at different Q-values is also a pre-requisite for the interpretation of quasielastic neutron scattering experiments, performed at instruments in which the total dynamic scattering function is measured, such as conventional time-of-flight and backscattering spectrometers. Combining data from different instruments, it was possible to cover a wide Q-range, from the small-angle region (0.006
Subject(s)
Hemoglobins/chemistry
, Myoglobin/chemistry
, Water/chemistry
, Deuterium Oxide/chemistry
, Models, Chemical
, Neutron Diffraction/methods
, Phycocyanin/chemistry
, Proteins/chemistry
, Solutions
ABSTRACT
The protein dynamical transition and its connection with the liquid-glass transition (GT) of hydration water and aqueous solvents are reviewed. The protein solvation shell exhibits a regular glass transition, characterized by steps in the specific heat and the thermal expansion coefficient at the calorimetric glass temperature T(G) approximately 170 K. It implies that the time scale of the structural alpha-relaxation has reached the experimental time window of 1-100 s. The protein dynamical transition, identified from elastic neutron scattering experiments by enhanced amplitudes of molecular motions exceeding the vibrational level, probes the alpha-process on a shorter time scale. The corresponding liquid-glass transition occurs at higher temperatures, typically 240 K. The GT is generally associated with diverging viscosities, the freezing of long-range translational diffusion in the supercooled liquid. Due to mutual hydrogen bonding, both, protein- and solvent relaxational degrees of freedom slow down in paralleled near the GT. However, the freezing of protein motions, where surface-coupled rotational and librational degrees of freedom are arrested, is better characterized as a rubber-glass transition. In contrast, internal protein modes such as the rotation of side chains are not affected. Moreover, ligand binding experiments with myoglobin in various glass-forming solvents show, that only ligand entry and exit rates depend on the local viscosity near the protein surface, but protein-internal ligand migration is not coupled to the solvent. The GT leads to structural arrest on a macroscopic scale due to the microscopic cage effect on the scale of the intermolecular distance. Mode coupling theory provides a theoretical framework to understand the microscopic nature of the GT even in complex systems. The role of the alpha- and beta-process in the dynamics of protein hydration water is evaluated. The protein-solvent GT is triggered by hydrogen bond fluctuations, which give rise to fast beta-processes. High-frequency neutron scattering spectra indicate increasing hydrogen bond braking above T(G).
Subject(s)
Proteins/chemistry , Water/chemistry , Carbon Monoxide/chemistry , Models, Chemical , Myoglobin/chemistry , Phase Transition , Solvents/chemistry , Thermodynamics , ViscosityABSTRACT
The article by Lesch et al. "Protein phase diagrams: The physics behind the elliptic shape" [J. Chem. Phys. 121, 12671 (2004)] is criticized since it involves assumptions, which violate a basic statistical theorem: the combined variance of a linear combination of statistically independent variables is always given by the sum of the variances. Thus their main conclusion that correlated fluctuations in the transition volume and enthalpy are the origin of the observed nearly elliptical stability diagrams of proteins should be questioned.
Subject(s)
Phase Transition , Proteins/chemistry , Models, Statistical , Research Design , ThermodynamicsABSTRACT
The dynamics of hydrated proteins and of protein crystals can be studied within a wide temperature range, since the water of hydration does not crystallize at low temperature. Instead it turns into an amorphous glassy state below 200 K. Extending the temperature range facilitates the spectral separation of different molecular processes. The conformational motions of proteins show an abrupt enhancement near 180 K, which has been called a "dynamical transition". In this contribution various aspects of the transition are critically reviewed: the role of the instrumental resolution function in extracting displacements from neutron elastic scattering data and the question of the appropriate dynamic model, discrete transitions between states of different energy versus continuous diffusion inside a harmonic well, are discussed. A decomposition of the transition involving two motional components is performed: rotational transitions of methyl groups and small scale librations of side-chains, induced by water at the protein surface. Both processes create an enhancement of the observed amplitude. The onset occurs, when their time scale becomes compatible with the resolution of the spectrometer. The reorientational rate of hydration water follows a super-Arrhenius temperature dependence, a characteristic feature of a dynamical transition. It occurs only with hydrated proteins, while the torsional motion of methyl groups takes place also in the dehydrated or solvent-vitrified system. Finally, the role of fast hydrogen bond fluctuations contributing to the amplitude enhancement is discussed.
Subject(s)
Proteins/chemistry , Animals , Diffusion , Elasticity , Hydrogen Bonding , Movement , Neutron Diffraction , Spectroscopy, Mossbauer , Temperature , Time Factors , Water/chemistryABSTRACT
The cytoplasm of red blood cells is congested with the oxygen storage protein hemoglobin occupying a quarter of the cell volume. The high protein concentration leads to a reduced mobility; the self-diffusion coefficient of hemoglobin in blood cells is six times lower than in dilute solution. This effect is generally assigned to excluded volume effects in crowded media. However, the collective or gradient diffusion coefficient of hemoglobin is only weakly dependent on concentration, suggesting the compensation of osmotic and friction forces. This would exclude hydrodynamic interactions, which are of dynamic origin and do not contribute to the osmotic pressure. Hydrodynamic coupling between protein molecules is dominant at short time- and length scales before direct interactions are fully established. Employing neutron spin-echo-spectroscopy, we study hemoglobin diffusion on a nanosecond timescale and protein displacements on the scale of a few nanometers. A time- and wave-vector dependent diffusion coefficient is found, suggesting the crossover of self- and collective diffusion. Moreover, a wave-vector dependent friction function is derived, which is a characteristic feature of hydrodynamic interactions. The wave-vector and concentration dependence of the long-time self-diffusion coefficient of hemoglobin agree qualitatively with theoretical results on hydrodynamics in hard spheres suspensions. Quantitative agreement requires us to adjust the volume fraction by including part of the hydration shell: Proteins exhibit a larger surface/volume ratio compared to standard colloids of much larger size. It is concluded that hydrodynamic and not direct interactions dominate long-range molecular transport at high concentration.
Subject(s)
Erythrocytes/chemistry , Hemoglobins/chemistry , Models, Biological , Cell Size , Diffusion , Erythrocytes/metabolism , Hemoglobins/metabolism , Humans , Protein BindingABSTRACT
The heat inactivation of Lactococcus lactis was studied by determination of cell counts, and by FT-IR spectroscopy recording the average structure of cell proteins. Cell counts were measured after incubation milk buffer or milk buffer with 1. 5 M sucrose, and FT-IR spectra were recorded in (2)H(2)O or (2)H(2)O with 1. 5 M sucrose in the range of 6-75 degrees Celsius. Sucrose protected L. lactis against heat inactivation. The cell counts differed by up to 6-log cycles after treatment in milk buffer as compared to milk buffer with sucrose. The (1)H/(2)H exchange in proteins, and secondary structure elements were detected by the analysis of amide I', amide II and amide II' bands. A reduced (1)H/(2)H exchange as well as a lower content of disordered structural elements was observed when sucrose was present. Conformational fluctuations of native proteins as indicated by the (1)H/(2)H exchange were apparent already at sublethal temperatures. The loss of viability of L. lactis occurred in the same temperature range as the loss of the protein secondary structure. These results demonstrate that sucrose protects L. lactis against heat inactivation, and that the increased heat stability of proteins in the presence of sucrose contributed to this enhanced heat resistance.
Subject(s)
Hot Temperature , Lactococcus lactis/drug effects , Microbial Viability/drug effects , Sucrose/pharmacology , Amides/chemistry , Bacterial Proteins/chemistry , Cell Membrane/chemistry , Cell Membrane/drug effects , Colony Count, Microbial , Fatty Acids/chemistry , Lactococcus lactis/growth & development , Lipids/chemistry , Phase Transition/drug effects , Protein Conformation , Protein Denaturation/drug effects , Protein Structure, Secondary , Spectroscopy, Fourier Transform Infrared , TemperatureABSTRACT
Reversible and irreversible states of pressure-dissociated casein micelles were studied by in situ light scattering techniques and ex situ atomic force microscopy. AFM experiments performed at ambient pressure reveal heterogeneities across the micelle, suggesting a sub-structure on a 20 nm scale. At pressures between 50 and 250 MPa, the native micelles disintegrate into small fragments on the scale of the observed sub-structure. At pressures above 300 MPa the micelles fully decompose into their monomeric constituents. After pressure release two discrete populations of casein aggregates are observed, depending on the applied initial pressure: Between 160 and 240 MPa stable micelles with diameters near 100 nm without detectable sub-structures are formed. Casein micelles exposed to pressures above 280 MPa re-associate at ambient pressure yielding mini-micelles with diameters near 25 nm. The implications concerning structural models are discussed.
Subject(s)
Caseins/chemistry , Micelles , Models, Molecular , Biophysical Phenomena , Biophysics , Light , Microscopy, Atomic Force , Pressure , Scattering, RadiationABSTRACT
The statistical properties of fast protein-water motions are analyzed by dynamic neutron scattering experiments. Using isotopic exchange, one probes either protein or water hydrogen displacements. A moment analysis of the scattering function in the time domain yields model-independent information such as time-resolved mean square displacements and the Gauss-deviation. From the moments, one can reconstruct the displacement distribution. Hydration water displays two dynamical components, related to librational motions and anomalous diffusion along the protein surface. Rotational transitions of side chains, in particular of methyl groups, persist in the dehydrated and in the solvent-vitrified protein structure. The interaction with water induces further continuous protein motions on a small scale. Water acts as a plasticizer of displacements, which couple to functional processes such as open-closed transitions and ligand exchange.
Subject(s)
Biophysics , Models, Chemical , Protein Conformation , Proteins/chemistry , Solvents/chemistry , Water/chemistry , Biophysical Phenomena , Neutron DiffractionABSTRACT
The bactericidal effect of hydrostatic pressure is reduced when bacteria are suspended in media with high osmolarity. To elucidate mechanisms responsible for the baroprotective effect of ionic and nonionic solutes, Lactococcus lactis was treated with pressures ranging from 200 to 600 MPa in a low-osmolarity buffer or with buffer containing 0.5 M sucrose or 4 M NaCl. Pressure-treated cells were characterized in order to determine viability, the transmembrane difference in pH (DeltapH), and multiple-drug-resistance (MDR) transport activity. Furthermore, pressure effects on the intracellular pH and the fluidity of the membrane were determined during pressure treatment. In the presence of external sucrose and NaCl, high intracellular levels of sucrose and lactose, respectively, were accumulated by L. lactis; 4 M NaCl and, to a lesser extent, 0.5 M sucrose provided protection against pressure-induced cell death. The transmembrane DeltapH was reversibly dissipated during pressure treatment in any buffer system. Sucrose but not NaCl prevented the irreversible inactivation of enzymes involved in pH homeostasis and MDR transport activity. In the presence 0.5 M sucrose or 4 M NaCl, the fluidity of the cytoplasmic membrane was maintained even at low temperatures and high pressure. These results indicate that disaccharides protect microorganisms against pressure-induced inactivation of vital cellular components. The protective effect of ionic solutes relies on the intracellular accumulation of compatible solutes as a response to the osmotic stress. Thus, ionic solutes provide only asymmetric protection, and baroprotection with ionic solutes requires higher concentrations of the osmolytes than of disaccharides.