Global Structure Analysis of Acid-Unfolded Myoglobin with Consideration to Effects of Intermolecular Coulomb Repulsion on Solution X-ray Scattering†

Unfolding simulations of holomyoglobin from four mammals: identification of intermediates and β-sheet formation from partially unfolded states

Myoglobin (Mb) is a centrally important, widely studied mammalian protein. While much work has investigated multi-step unfolding of apoMb using acid or denaturant, holomyoglobin unfolding is poorly understood despite its biological relevance. We present here the first systematic unfolding simulations of holoMb and the first comparative study of unfolding of protein orthologs from different species (sperm whale, pig, horse, and harbor seal). We also provide new interpretations of experimental mean molecular ellipticities of myoglobin intermediates, notably correcting for random coil and number of helices in intermediates. The simulated holoproteins at 310 K displayed structures and dynamics in agreement with crystal structures (R g ~1.48-1.51 nm, helicity ~75%). At 400 K, heme was not lost, but some helix loss was observed in pig and horse, suggesting that these helices are less stable in terrestrial species. At 500 K, heme was lost within 1.0-3.7 ns. All four proteins displayed exponentially decaying helix structure within 20 ns. The C- and F-helices were lost quickly in all cases. Heme delayed helix loss, and sperm whale myoglobin exhibited highest retention of heme and D/E helices. Persistence of conformation (RMSD), secondary structure, and ellipticity between 2-11 ns was interpreted as intermediates of holoMb unfolding in all four species. The intermediates resemble those of apoMb notably in A and H helices, but differ substantially in the D-, E- and F-helices, which interact with heme. The identified mechanisms cast light on the role of metal/cofactor in poorly understood holoMb unfolding. We also observed β-sheet formation of several myoglobins at 500 K as seen experimentally, occurring after disruption of helices to a partially unfolded, globally disordered state; heme reduced this tendency and sperm-whale did not display any sheet propensity during the simulations.

Thermodynamic and structural properties of the acid molten globule state of horse cytochrome C

To understand the stabilization, folding, and functional mechanisms of proteins, it is very important to understand the structural and thermodynamic properties of the molten globule state. In this study, the global structure of the acid molten globule state, which we call MG1, of horse cytochrome c at low pH and high salt concentrations was evaluated by solution X-ray scattering (SXS), dynamic light scattering, and circular dichroism measurements. MG1 was globular and slightly (3%) larger than the native state, N. Calorimetric methods, such as differential scanning calorimetry and isothermal acid-titration calorimetry, were used to evaluate the thermodynamic parameters in the transitions of N to MG1 and MG1 to denatured state D of horse cytochrome c. The heat capacity change, ΔC(p), in the N-to-MG1 transition was determined to be 2.56 kJ K(-1) mol(-1), indicating the increase in the level of hydration in the MG1 state. Moreover, the intermediate state on the thermal N-to-D transition of horse cytochrome c at pH 4 under low-salt conditions showed the same structural and thermodynamic properties of the MG1 state in both SXS and calorimetric measurements. The Gibbs free energy changes (ΔG) for the N-to-MG1 and N-to-D transitions at 15 °C were 10.9 and 42.2 kJ mol(-1), respectively.

The kinetic and equilibrium molten globule intermediates of apoleghemoglobin differ in structure

An important question in protein folding is whether molten globule states formed under equilibrium conditions are good structural models for kinetic folding intermediates. The structures of the kinetic and equilibrium intermediates in the folding of the plant globin apoleghemoglobin have been compared at high resolution by quench-flow pH-pulse labeling and interrupted hydrogen/deuterium exchange analyzed in dimethyl sulfoxide. Unlike its well studied homolog apomyoglobin, where the equilibrium and kinetic intermediates are quite similar, there are striking structural differences between the intermediates formed by apoleghemoglobin. In the kinetic intermediate, formed during the burst phase of the quench-flow experiment, protected amides and helical structure are found mainly in the regions corresponding to the G and H helices of the folded protein, and in parts of the E helix and CE loop regions, whereas in the equilibrium intermediate, amide protection and helical structure are seen in parts of the A and B helix regions, as well as in the G and H regions, and the E helix remains largely unfolded. These results suggest that the structure of the molten globule intermediate of apoleghemoglobin is more plastic than that of apomyoglobin, so that it is readily transformed depending on the solution conditions, particularly pH. Thus, in the case of apoleghemoglobin at least, the equilibrium molten globule formed under destabilizing conditions at acid pH is not a good model for the compact intermediate formed during kinetic refolding experiments. Our high-precision kinetic analysis also reveals an additional slow phase during the folding of apoleghemoglobin, which is not observed for apomyoglobin. Hydrogen exchange pulse-labeling experiments show that the slow-folding phase is associated with residues in the CE loop, which probably forms non-native structure in the intermediate that must be resolved before folding can proceed to completion.