Structures of apomyoglobin's various acid-destabilized forms.

The structures and the cold and hot melting thermodynamics of the acid- and salt-destabilized states of horse heart apomyoglobin (apoMb), including the E (extended) and various I forms, are studied using probes of tertiary structure (tryptophan fluorescence and FTIR spectroscopy) and secondary structure (far-UV CD and FTIR spectroscopy). These forms likely resemble early structures in the folding of the largely helical protein. Both the I and E forms retain the AGH core whereby the two ends of the protein are tied together with sufficient numbers of tertiary contacts, involving a number of hydrophobic residues, to show cooperative melting. The melting thermodynamics of E and I are distinctly different. E contains no other tertiary structure and probably little other secondary structure apart from the core. The more destabilized E form appears to contain "random" buried runs of polypeptide backbone which convert to alpha-helix in the I form(s). Most interestingly, E consists not of a single structure but is composed of a heterogeneous mixture of conformations, all showing corelike cooperative melting characteristics, and consisting presumably of varying contacts between the A portion of apomyoglobin and the G-H hairpin. These results bear on the energy landscape and structural features of the early part of apomyoglobin's folding pathway.

Core formation in apomyoglobin: probing the upper reaches of the folding energy landscape.

An acid-destabilized form of apomyoglobin, the so-called E state, consists of a set of heterogeneous structures that are all characterized by a stable hydrophobic core composed of 30-40 residues at the intersection of the A, G, and H helices of the protein, with little other secondary structure and no other tertiary structure. Relaxation kinetics studies were carried out to characterize the dynamics of core melting and formation in this protein. The unfolding and/or refolding response is induced by a laser-induced temperature jump between the folded and unfolded forms of E, and structural changes are monitored using the infrared amide I' absorbance at 1648-1651 cm(-1) that reports on the formation of solvent-protected, native-like helix in the core and by fluorescence emission changes from apomyoglobin's Trp14, a measure of burial of the indole group of this residue. The fluorescence kinetics data are monoexponential with a relaxation time of 14 micros. However, infrared kinetics data are best fit to a biexponential function with relaxation times of 14 and 59 micros. These relaxation times are very fast, close to the limits placed on folding reactions by diffusion. The 14 micros relaxation time is weakly temperature dependent and thus represents a pathway that is energetically downhill. The appearance of this relaxation time in both the fluorescence and infrared measurements indicates that this folding event proceeds by a concomitant formation of compact secondary and tertiary structures. The 59 micros relaxation time is much more strongly temperature dependent and has no fluorescence counterpart, indicating an activated process with a large energy barrier wherein nonspecific hydrophobic interactions between helix A and the G and H helices cause some helix burial but Trp14 remains solvent exposed. These results are best fit by a multiple-pathway kinetic model when U collapses to form the various folded core structures of E. Thus, the results suggest very robust dynamics for core formation involving multiple folding pathways and provide significant insight into the primary processes of protein folding.

The core of apomyoglobin E-form folds at the diffusion limit.

The E-form of apomyoglobin has been characterized using infrared and fluorescence spectroscopies, revealing a compact core with native like contacts, most probably consisting of 15-20 residues of the A, G and H helices of apomyoglobin. Fast temperature-jump, time-resolved infrared measurements reveal that the core is formed within 96 micros at 46 degrees C, close to the diffusion limit for loop formation. Remarkably, the folding pathway of the E-form is such that the formation of a limited number of native-like contacts is not rate limiting, or that the contacts form on the same time scale expected for diffusion controlled loop formation.

Fast events in protein folding: the time evolution of primary processes.

Most experimental studies on the dynamics of protein folding have been confined to timescales of 1 ms and longer. Yet it is obvious that many phenomena that are obligatory elements of the folding process occur on much faster timescales. For example, it is also now clear that the formation of secondary and tertiary structures can occur on nanosecond and microsecond times, respectively. Although fast events are essential to, and sometimes dominate, the overall folding process, with a few exceptions their experimental study has become possible only recently with the development of appropriate techniques. This review discusses new approaches that are capable of initiating and monitoring the fast events in protein folding with temporal resolution down to picoseconds. The first important results from those techniques, which have been obtained for the folding of some globular proteins and polypeptide models, are also discussed.

Fast events in protein folding: relaxation dynamics and structure of the I form of apomyoglobin.

The fast relaxation dynamics of the acid destabilized I form of apomyoglobin (pH* 3, 0.15 M NaCl; apoMb-I) following a laser-induced temperature-jump have been probed using time-resolved infrared spectroscopy. Only a fast, single exponential phase is observed (bleach centered at v = 1633 cm-1 and transient absorbance at 1666 cm-1) with relaxation times of 38 ns at 30 degrees C and 36 ns at 57 degrees C; no additional slow (microsecond) phase is observed as previously found in the native form of apomyoglobin. Folding times of approximately 66 ns are derived from the observed rates based on a simple two-state model. The equilibrium melting of the 1633 cm-1 component shows noncooperative linear behavior over the temperature range studied (10-60 degrees C). The low amide I' frequency, the fast relaxation dynamics, and the noncooperative melting behavior are characteristic of isolated solvated helix. The analysis of the amide-I' band reveals another major component at 1650 cm-1 assigned to native-like structure stabilized by tertiary contacts involving the AGH core, which does not show dynamic or static melting under our conditions. ApoMb-I has generally been taken to be a "molten globule" species. The present results indicate a heterogeneous structure consisting of separate regions of native-like unit(s), solvated helices, and disordered coil, excluding a homogeneous molten globule as a model for apoMb-I. From the current studies and other results, a detailed model of the folding of apomyoglobin is presented.

Structural heterogeneity of the various forms of apomyoglobin: implications for protein folding.

Temperature-induced denaturation transitions of different structural forms of apomyoglobin were studied monitoring intrinsic tryptophan fluorescence. It was found that the tryptophans are effectively screened from solvent both in native and acid forms throughout most of the temperature range tested. Thus, the tryptophans' surrounding do not show a considerable change in structure where major protein conformational transitions have been found in apomyoglobin using other techniques. At high temperatures and under strong destabilizing conditions, the tryptophans' fluorescence parameters show sigmoidal thermal denaturation. These results, combined with previous studies, show that the structure of this protein is heterogeneous, including native-like (tightly packed) and molten globule-like substructures that exhibit conformation (denaturation) transitions under different conditions of pH and temperature (and denaturants). The results suggest that the folding of this protein proceeds via two "nucleation" events whereby native-like contacts are formed. One of these events, which involves AGH "core" formation, appears to occur very early in the folding process, even before significant hydrophobic collapse in the rest of the protein molecule. From the current studies and other results, a rather detailed picture of the folding of myoglobin is presented, on the level of specific structures and their thermodynamical properties as well as formation kinetics.

Fast events in protein folding: relaxation dynamics of secondary and tertiary structure in native apomyoglobin.

We report the fast relaxation dynamics of "native" apomyoglobin (pH 5.3) following a 10-ns, laser-induced temperature jump. The structural dynamics are probed using time-resolved infrared spectroscopy. The infrared kinetics monitored within the amide I absorbance of the polypeptide backbone exhibit two distinct relaxation phases which have different spectral signatures and occur on very different time scales (nu = 1633 cm(-1),tau = 48 ns; nu = 1650 cm(-1),tau = 132 micros). We assign these two spectral components to discrete substructures in the protein: helical structure that is solvated (1633 cm(-1)) and native helix that is protected from solvation by interhelix tertiary interactions (1650 cm(-1)). Folding rate coefficients inferred from the observed relaxations at 60 degrees C are k(f)(solvated) = (7 to 20) x 10(6) s(-1) and k(f)(native) = 3.6 x 10(3) s(-1), respectively. The faster rate is interpreted as the intrinsic rate of solvated helix formation, whereas the slower rate is interpreted as the rate of formation of tertiary contacts that determine a native helix. Thus, at 60 degrees C helix formation precedes the formation of tertiary structure by over three orders of magnitude in this protein. Furthermore, the distinct thermodynamics and kinetics observed for the apomyoglobin substructures suggest that they fold independently, or quasi-independently. The observation of inhomogeneous folding for apomyoglobin is remarkable, given the relatively small size and structural simplicity of this protein.

Fast events in protein folding: helix melting and formation in a small peptide.

The helix is a common secondary structural motif found in proteins, and the mechanism of helix-coil interconversion is key to understanding the protein-folding problem. We report the observation of the fast kinetics (nanosecond to millisecond) of helix melting in a small 21-residue alanine-based peptide. The unfolding reaction is initiated using a laser-induced temperature jump and probed using time-resolved infrared spectroscopy. The model peptide exhibits fast unfolding kinetics with a time constant of 160 +/- 60 ns at 28 degrees C in response to a laser-induced temperature jump of 18 degrees C which is completed within 20 ns. Using the unfolding time and the measured helix-coil equilibrium constant of the model peptide, a folding rate constant of approximately 6 x 10(7) s-1 (t1/2 = 16 ns) can be inferred for the helix formation reaction at 28 degrees C. These results demonstrate that secondary structure formation is fast enough to be a key event at early times in the protein-folding process and that helices are capable of forming before long range tertiary contacts are made.

Annexin IV reduces the rate of lateral lipid diffusion and changes the fluid phase structure of the lipid bilayer when it binds to negatively charged membranes in the presence of calcium.

Bovine annexin IV (endonexin) was bound to supported planar bilayers composed of 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) in the first monolayer facing the substrate, and varying mole fractions of POPC, 1-palmitoyl-2-oleoylphosphatidylglycerol (POPG) and small amounts of the fluorescent lipid analogs NBD-PC or NBD-PG in the second monolayer facing the large aqueous compartment. Lateral diffusion coefficients and mobile fractions of these phospholipids were measured by fluorescence recovery after photobleaching (FRAP) as a function of protein concentration and lipid composition in the presence of 2 mM CaCl2 or 1 mM EDTA. In the absence of annexin IV, the lateral diffusion coefficients depended only little on the POPC:POPG ratios and were approximately 3.0 microns2/s for NBD-PG (no Ca2+), 2.5 microns2/s for NBD-PG (2 mM Ca2+), and 1.6 microns2/s for NBD-PC (with or without 2 mM Ca2+). In the presence of 2 mM Ca2+ these diffusion coefficients decreased as a function of the added annexin concentration. A transition from a state with "rapid" lipid diffusion to a state with "slow" lipid diffusion occurred at about 80 nM annexin IV and was independent of the POPC:POPG ratio. In addition to reducing the lipid lateral diffusion coefficients, annexin IV also gave rise to two-component lateral diffusion of the lipids in these mixed bilayers. The split of the single diffusion coefficient of NBD-PG into two components occurred at most POPC:POPG ratios upon binding of annexin IV, but required higher annexin concentrations at mole fractions of POPC between 66 and 82 mol % than at high mole fractions of POPG or 90 mol % POPC.(ABSTRACT TRUNCATED AT 250 WORDS)

Study of the "molten globule" intermediate state in protein folding by a hydrophobic fluorescent probe.

Binding of the hydrophobic fluorescent probe, 1-anilino-naphthalene-8-sulfonate (ANS), to synthetic polypeptides and proteins with a different structural organization has been studied. It has been shown that ANS has a much stronger affinity to the protein "molten globule" state, with a pronounced secondary structure and compactness, but without a tightly packed tertiary structure as compared with its affinity to the native and coil-like proteins, or to coil-like, alpha-helical, or beta-structural hydrophilic homopolypeptides. The possibility of using ANS for the study of equilibrium and kinetic molten globule intermediates is demonstrated, with carbonic anhydrase, beta-lactamase, and alpha-lactalbumin as examples.

An early intermediate of refolding alpha-lactalbumin forms within 20 ms.

The kinetics of alpha-lactalbumin refolding were studied by the stopped-flow method with the registration of CD and intrinsic fluorescence at several wavelengths. It was shown that the early kinetic intermediate forms during the dead-time of the experiment (20 ms). This intermediate has a considerable amount of secondary structure and unpolar clusters in its molecular structure but has no rigid tertiary structure.

Compact state of a protein molecule with pronounced small-scale mobility: bovine alpha-lactalbumin.

We describe a novel physical state of a protein molecule which is nearly as compact as the native state and has pronounced secondary structure, but differs from the native state by the large increase of thermal fluctuations (in particular, by the large mobility of side groups). This state has been characterized in detail for the acid form of bovine alpha-lactalbumin as a result of the study of physical properties of this state by a large variety of different methods (hydrodynamics, diffuse X-ray scattering, circular dichroism and infrared spectra, polarization of the luminescence, proton magnetic resonance, deuterium exchange and microcalorimetry). It has been shown that bovine alpha-lactalbumin can be transformed into a similar state by thermal denaturation. This process is thermodynamically two state (i.e. all-or-none transition), which means that this state differs from the native one by a phase transition of the first order.