Increasing concentrations of chloride were found to increase the resolution between two visible absorbance spectral transitions associated with acidification of ferricytochrome c. Analysis of a variety of spectral and viscosity measurements indicates that protonation of a single group having an apparent pK of 2.1 +/- 0.2 and an intrinsic pK of about 5.3 displaces the methionine ligand without significantly perturbing the native globular conformation. Analysis of methylated ferricytochrome c suggests that protonation of a carboxylate ion, most likely a heme propionate residue, is responsible for displacement of the methionine ligand. Addition of a proton to a second group having an apparent pK of 1.2 +/- 0.1 displaces the histidine ligand and unfolds the protein from a globular conformation into a random coil. It is most likely that the second protonation occurs on the imidazole ring of the histidine ligand itself. Chloride is proposed to perturb these transitions by ligation in the fifth coordination position of the heme ion. Such ligation stabilizes a globular conformation of ferricytochrome c at pH 0.0 and 25 degrees.
The forkhead family of transcription factors (Fox) controls gene transcription during key processes such as regulation of metabolism, embryogenesis, and immunity. Structurally, Fox proteins feature a conserved DNA-binding domain known as forkhead. Interestingly, solved forkhead structures of members from the P subfamily (FoxP) show that they can oligomerize by three-dimensional domain swapping, whereby structural elements are exchanged between adjacent subunits, leading to an intertwined dimer. Recent evidence has largely stressed the biological relevance of domain swapping in FoxP, as several disease-causing mutations have been related to impairment of this process. Here, we explore the equilibrium folding and binding mechanism of the forkhead domain of wild-type FoxP1, and of two mutants that hinder DNA-binding (R53H) and domain swapping (A39P), using size-exclusion chromatography, circular dichroism, and hydrogen-deuterium exchange mass spectrometry. Our results show that domain swapping of FoxP1 occurs at micromolar protein concentrations within hours of incubation and is energetically favored, in contrast to classical domain-swapping proteins. Also, DNA-binding mutations do not significantly affect domain swapping. Remarkably, equilibrium unfolding of dimeric FoxP1 follows a three-state N2 ↔ 2I ↔ 2U folding mechanism in which dimer dissociation into a monomeric intermediate precedes protein unfolding, in contrast to the typical two-state model described for most domain-swapping proteins, whereas the A39P mutant follows a two-state N ↔ U folding mechanism consistent with the second transition observed for dimeric FoxP1. Also, the free-energy change of the N ↔ U in A39P FoxP1 is ∼2 kcal⋅mol(-1) larger than the I ↔ U transition of both wild-type and R53H FoxP1. Finally, hydrogen-deuterium exchange mass spectrometry reveals that the intermediate strongly resembles the native state. Our results suggest that domain swapping in FoxP1 is at least partially linked to monomer folding stability and follows an unusual three-state folding mechanism, which might proceed via transient structural changes rather than requiring complete protein unfolding as do most domain-swapping proteins.
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