Folding of apocytochrome c induced by the interaction with negatively charged lipid micelles proceeds via a collapsed intermediate state

Unfolded apocytochrome c acquires an alpha-helical conformation upon interaction with lipid. Folding kinetic results below and above the lipid's CMC, together with energy transfer measurements of lipid bound states, and salt-induced compact states in solution, show that the folding transition of apocytochrome c from the unfolded state in solution to a lipid-inserted helical conformation proceeds via a collapsed intermediate state (I(C)). This initial compact state is driven by a hydrophobic collapse of the polypeptide chain in the absence of the heme group and may represent a heme-free analogue of an early compact intermediate detected on the folding pathway of cytochrome c in solution. Insertion into the lipid phase occurs via an unfolding step of I(C) through a more extended state associated with the membrane surface (I(S)). While I(C) appears to be as compact as salt-induced compact states in solution with substantial alpha-helix content, the final lipid-inserted state (Hmic) is as compact as the unfolded state in solution at pH 5 and has an alpha-helix content which resembles that of native cytochrome c.     

Activation of Cytochrome C Peroxidase Function Through Coordinated Foldon Loop Dynamics upon Interaction with Anionic Lipids

Cardiolipin (CL) is a mitochondrial anionic lipid that plays important roles in the regulation and signaling of mitochondrial apoptosis. CL peroxidation catalyzed by the assembly of CL-cytochrome c (cyt c) complexes at the inner mitochondrial membrane is a critical checkpoint. The structural changes in the protein, associated with peroxidase activation by CL and different anionic lipids, are not known at a molecular level. To better understand these peripheral protein-lipid interactions, we compare how phosphatidylglycerol (PG) and CL lipids trigger cyt c peroxidase activation, and correlate functional differences to structural and motional changes in membrane-associated cyt c. Structural and motional studies of the bound protein are enabled by magic angle spinning solid state NMR spectroscopy, while lipid peroxidase activity is assayed by mass spectrometry. PG binding results in a surface-bound state that preserves a nativelike fold, which nonetheless allows for significant peroxidase activity, though at a lower level than binding its native substrate CL. Lipid-specific differences in peroxidase activation are found to correlate to corresponding differences in lipid-induced protein mobility, affecting specific protein segments. The dynamics of omega loops C and D are upregulated by CL binding, in a way that is remarkably controlled by the protein:lipid stoichiometry. In contrast to complete chemical denaturation, membrane-induced protein destabilization reflects a destabilization of select cyt c foldons, while the energetically most stable helices are preserved. Our studies illuminate the interplay of protein and lipid dynamics in the creation of lipid peroxidase-active proteolipid complexes implicated in early stages of mitochondrial apoptosis.     

Unfolding and refolding of cytochrome c driven by the interaction with lipid micelles

Binding of native cyt c to L-PG micelles leads to a partially unfolded conformation of cyt c. This micelle-bound state has no stable tertiary structure, but remains as alpha-helical as native cyt c in solution. In contrast, binding of the acid-unfolded cyt c to L-PG micelles induces folding of the polypeptide, resulting in a similar helical state to that originated from the binding of native cyt c to L-PG micelles. Far-ultraviolet (UV) circular dichroism (CD) spectra showed that this common micelle-associated helical state (HL) has a native-like alpha-helix content, but is highly expanded without a tightly packed hydrophobic core, as revealed by tryptophan fluorescence, near-UV, and Soret CD spectroscopy. The kinetics of the interaction of native and acid-unfolded cyt c was investigated by stopped-flow tryptophan fluorescence. Formation of H(L) from the native state requires the disruption of the tightly packed hydrophobic core in the native protein. This micelle-induced unfolding of cyt c occurs at a rate approximately 0.1 s(-1), which is remarkably faster in the lipid environment compared with the expected rate of unfolding in solution. Refolding of acid-unfolded cyt c with L-PG micelles involves an early highly helical collapsed state formed during the burst phase (<3 ms), and the observed main kinetic event reports on the opening of this early compact intermediate prior to insertion into the lipid micelle.     

Protein oxidation of cytochrome C by reactive halogen species enhances its peroxidase activity

Reactive halogen species (RHS; X(2) and HOX, where X represents Cl, Br, or I) are metabolites mediated by neutrophil activation and its accompanying respiratory burst. We have investigated the interaction between RHS and mitochondrial cytochrome c (cyt c) by using electrospray mass spectrometry and electron spin resonance (ESR). When the purified cyt c was reacted with an excess amount of hypochlorous acid (HOCl) at pH 7.4, the peroxidase activity of cyt c was increased by 4.5-, 6.9-, and 8.6-fold at molar ratios (HOCl/cyt c) of 2, 4, and 8, respectively. In comparison with native cyt c, the mass spectra obtained from the HOCl-treated cyt c revealed that oxygen is covalently incorporated into the protein as indicated by molecular ions of m/z = 12,360 (cyt c), 12,376 (cyt c + O), and 12,392 (cyt c + 2O). Using tandem mass spectrometry, a peptide (obtained from the tryptic digests of HOCl-treated cyt c) corresponding to the amino acid sequence MIFAGIK, which contains the methionine that binds to the heme, was identified to be involved in the oxygen incorporation. The location of the oxygen incorporation was unequivocally determined to be the methionine residue, suggesting that the oxidation of heme ligand (Met-80) by HOCl results in the enhancement of peroxidase activity of cyt c. ESR spectroscopy of HOCl-oxidized cyt c, when reacted with H(2)O(2) in the presence of the nitroso spin trap 2-methyl-2-nitrosopropane (MNP), yielded more immobilized MNP/tyrosyl adduct than native cyt c. In the presence of H(2)O(2), the peroxidase activity of HOCl-oxidized cyt c exhibited an increasing ability to oxidize tyrosine to tyrosyl radical as measured directly by fast flow ESR. Titration of both native cyt c and HOCl-oxidized cyt c with various amounts of H(2)O(2) indicated that the latter has a decreased apparent K(m) for H(2)O(2), implicating that protein oxidation of cyt c increases its accessibility to H(2)O(2). HOCl-oxidized cyt c also displayed an impaired ability to support oxygen consumption by the purified mitochondrial cytochrome c oxidase, suggesting that protein oxidation of cyt c may break the electron transport chain and inhibit energy transduction in mitochondria.     

Equilibrium amide hydrogen exchange and protein folding kinetics

The classical Linderstrøm-Lang hydrogen exchange (HX) model is extended to describe the relationship between the HX behaviors (EX1 and EX2) and protein folding kinetics for the amide protons that can only exchange by global unfolding in a three-state system including native (N), intermediate (I), and unfolded (U) states. For these slowly exchanging amide protons, it is shown that the existence of an intermediate (I) has no effect on the HX behavior in an off-pathway three-state system (IUN). On the other hand, in an on-pathway three-state system (UIN), the existence of a stable folding intermediate has profound effect on the HX behavior. It is shown that fast refolding from the unfolded state to the stable intermediate state alone does not guarantee EX2 behavior. The rate of refolding from the intermediate state to the native state also plays a crucial role in determining whether EX1 or EX2 behavior should occur. This is mainly due to the fact that only amide protons in the native state are observed in the hydrogen exchange experiment. These new concepts suggest that caution needs to be taken if one tries to derive the kinetic events of protein folding from equilibrium hydrogen exchange experiments.     

A two-process model describes the hydrogen exchange behavior of cytochrome c in the molten globule state with various extents of acetylation

Acetylation of Lys residues of horse cytochrome c steadily stabilizes the molten globule state in 18 mM HCl as more Lys residues are acetylated [Goto and Nishikiori (1991) J. Mol. Biol. 222, 679-686]. The dynamic features of the molten globule state were characterized by hydrogen/deuterium exchange of amide protons, monitored by mass spectrometry as each deuteration increased the protein mass by 1 Da. Electrospray mass spectrometry enabled us to monitor simultaneously the exchange kinetics of more than seven species with a different number of acetyl groups. One to four Lys residue-acetylated cytochrome c showed almost no protection of the amide protons from rapid exchange. The transition from the unprotected to the protected state occurred between five and eight Lys residue-acetylated species. For species with more than nine acetylated Lys residues, the exchange kinetics were independent of the extent of acetylation, and 26 amide protons were protected at 60 min of exchange, indicating the formation of a rigid hydrophobic core with hydrogen-bonded secondary structures. The apparent transition to the protected state required a higher degree of acetylation than the conformational transition measured by circular dichroism, which had a midpoint at about four acetylated residues. This difference in the transitions suggested a two-process model in which the exchange occurs either from the protected folded state or from the unprotected unfolded state through global unfolding. On the basis of a two-process model and with the reported values of the exchange and stability parameters, we simulated the exchange kinetics of a series of acetylated cytochrome c species. The simulated kinetics reproduced the observed kinetics well, indicating validity of this model for hydrogen exchange of the molten globule state.     

Mapping protein energy landscapes with amide hydrogen exchange and mass spectrometry: I. A generalized model for a two-state protein and comparison with experiment

Protein amide hydrogen exchange (HDX) is a convoluted process, whose kinetics is determined by both dynamics of the protein and the intrinsic exchange rate of labile hydrogen atoms fully exposed to solvent. Both processes are influenced by a variety of intrinsic and extrinsic factors. A mathematical formalism initially developed to rationalize exchange kinetics of individual amide hydrogen atoms is now often used to interpret global exchange kinetics (e.g., as measured in HDX MS experiments). One particularly important advantage of HDX MS is direct visualization of various protein states by observing distinct protein ion populations with different levels of isotope labeling under conditions favoring correlated exchange (the so-called EX1 exchange mechanism). However, mildly denaturing conditions often lead to a situation where the overall HDX kinetics cannot be clearly classified as either EX1 or EX2. The goal of this work is to develop a framework for a generalized exchange model that takes into account multiple processes leading to amide hydrogen exchange, and does not require that the exchange proceed strictly via EX1 or EX2 kinetics. To achieve this goal, we use a probabilistic approach that assigns a transition probability and a residual protection to each equilibrium state of the protein. When applied to a small protein chymotrypsin inhibitor 2, the algorithm allows complex HDX patterns observed experimentally to be modeled with remarkably good fidelity. On the basis of the model we are now in a position to begin to extract quantitative dynamic information from convoluted exchange kinetics.     

Secondary structure changes stabilize the reactive-centre cleaved form of SERPINs. A study by 1H nuclear magnetic resonance and Fourier transform infrared spectroscopy.

Proteinase inhibitor members of the SERPIN superfamily are characterized by the presence of a proteolytically sensitive reactive-site loop. Cleavage within this region results in a conformational transition from an unstable "stressed" native protein to a more stable "relaxed" cleaved molecule. In order to identify the principal molecular aspects of this transition, 1H nuclear magnetic resonance (n.m.r.) and FT-IR spectroscopy were applied to the study of four SERPINs. 1H n.m.r. spectra of approximately 20 high-field ring-current-shifted methyl signals exhibited slightly different chemical shifts in the native and cleaved forms of alpha 1-antitrypsin (alpha 1-AT), alpha 1-antichymotrypsin (alpha 1-ACT) and C1 inhibitor (C1-INH), but not ovalbumin, between 20 degrees C and 90 degrees C. Ring current calculations based on crystal co-ordinates for cleaved alpha 1-AT and alpha 1-ACT and native ovalbumin showed that these signals originate from highly localized interactions between different buried residues corresponding to alpha-helix and beta-sheet segments of the SERPIN fold. The small shift changes correspond to small relative conformational side-chain rearrangements of about 0.01 nm to 0.05 nm in the protein hydrophobic core, i.e. the tertiary structure interactions in the two forms of the SERPIN fold are well-preserved, and changes in this appear unimportant for the stabilization found after reactive centre cleavage. Fourier transform infrared (FT-IR) spectroscopic studies of the amide I band showed that the native and cleaved forms of alpha 1-AT, alpha 1-ACT and C1-INH contain 28% to 36% alpha-helix and 38% to 44% beta-sheet. Second derivative FT-IR spectra using H2O and 2H2O buffers revealed very large differences in the amide I band between the native and cleaved forms of alpha 1-AT, alpha 1-ACT and C1-INH, but not for ovalbumin. The alpha-helix band was most sensitive to 1H-2H exchange, while the beta-sheet bands were not, and greater amounts of antiparallel beta-sheet were detected in the cleaved form. 1H n.m.r. showed that polypeptide amide 1H-2H exchange was greater in the native forms of alpha 1-AT, alpha 1-ACT and C1-INH than in their cleaved forms, whereas for ovalbumin it was unchanged. The FT-IR and 1H-2H exchange data show that alterations in the secondary structure are central to the stabilization of the cleaved SERPIN structure.(ABSTRACT TRUNCATED AT 400 WORDS)     

Amide proton exchange in proteins by EX1 kinetics: studies of the basic pancreatic trypsin inhibitor at variable p2H and temperature

With the use of one-dimensional 1H nuclear magnetic resonance, two-dimensional correlated spectroscopy, and two-dimensional nuclear Overhauser enhancement spectroscopy, the exchange mechanisms for numerous individual amide protons in the basic pancreatic trypsin inhibitor (BPTI) were investigated over a wide range of p2H and temperature. Correlated exchange under an EX1 regime was observed only for the most slowly exchanging protons in the central hydrogen bonds of the antiparallel beta-sheet and only over a narrow range of temperature and p2H, i.e., above ca. 55 degrees C and between p2H 7 and 9, where the opening rates of the structure fluctuations which promote the exchange of these protons are of the order 0.1 min-1. At p2H below 7, the exchange of this most stable group of protons is uncorrelated and is governed by an EX2 mechanism. At p2H above 9, the exchange is also uncorrelated and occurs via either EX2 or EX1 processes promoted by strictly local structure fluctuations. For all other backbone amide protons in BPTI, the exchange was found to be uncorrelated and by an EX2 mechanism under all conditions of p2H and temperature where quantitative measurements could be obtained with the methods used, i.e., for kex approximately less than 5 min-1. From these observations with BPTI it can be concluded that the amide proton exchange in globular proteins is quite generally via EX2 processes, with rare exceptions for measurements with extremely stable protons at high temperature and basic p2H. This emphasizes the need for further development of suitable concepts for the structural interpretation of EX2 amide proton exchange [Wagner, G. (1983) Q. Rev. Biophys. 16, 1-57; Wagner, G., Stassinopoulou, C. I., & Wüthrich, K. (1984) Eur. J. Biochem. 145, 431-436] and for more detailed investigations of the intrinsic exchange rates for solvent-exposed amide protons in the "open" states of a protein [Roder, H., Wagner, G., & Wüthrich, K. (1985) Biochemistry (following paper in this issue)].     

Folding of apocytochrome c in lipid micelles: formation of alpha-helix precedes membrane insertion.

Apocytochrome c, which in aqueous solution is largely unstructured, acquires a highly alpha-helical structure upon interaction with lipid. The alpha-helix content induced in apocytochrome c depends on the lipid system, and this folding process is driven by both electrostatic and hydrophobic lipid-protein interactions. The folding kinetic mechanism of apocytochrome c induced by zwitterionic micelles of lysophosphatidylcholine (L-PC), predominantly driven by hydrophobic lipid-protein interactions, was investigated by fluorescence stopped-flow measurements of Trp 59 and fluorescein-phosphatidylethanolamine-(FPE) labeled micelles, in combination with stopped-flow far-UV circular dichroism. It was found that formation of the alpha-helical structure of apocytochrome c precedes membrane insertion. The unfolded state in solution (U(W)) binds to the micelle surface in a helical conformation (I(S)) and is followed by insertion into the lipid micelle, i.e., formation of the final helical state H(L). Binding of apocytochrome c to the lipid micelle (U(W) --> I(S)) is concurrent with formation of a large fraction (75-100%, depending on lipid concentration) of the alpha-helical structure of the final lipid-inserted state H(L). The highly helical intermediate I(S) is formed on the time scale of 3-12 ms, depending on lipid concentration, and inserts into the lipid micelle (I(S) --> H(L)) in the time range of approximately 200 ms to >1 s, depending on lipid-to-protein ratio. The final lipid-inserted helical state H(L) in L-PC micelles has an alpha-helix content approximately 65% of that of cytochrome c in solution and has no compact stable tertiary structure as revealed by circular dichroism results.     

Ionic strength dependence of cytochrome c structure and Trp-59 H/D exchange from ultraviolet resonance Raman spectroscopy

Ultraviolet resonance Raman spectra are reported for cytochrome c (cyt c) in FeII and FeIII oxidation states at low (0.005 M) and high (0.9-1.5 M) ionic strength. With 200-nm excitation the amide band intensities are shown to remain constant, establishing that redox state and ionic strength have no influence on the alpha-helical content. The tyrosine 830/850-cm-1 doublet, however, shows a loss in 830-cm-1 intensity at I = 0.005 M for the FeIII protein, suggesting a weakening or a loss of H-bonding from an internal tyrosine, probably Tyr-48, which is H-bonded to a heme propionate group in cyt c crystals. Excitation profiles of tryptophan peak at approximately 229 nm for both FeII and FeIII forms of cyt c, but at approximately 218 nm for aqueous tryptophan. The approximately 2200-cm-1 red shift of the resonant electronic transition is attributed to the Trp-59 residue being buried and H-bonded. Consistent with this Trp environment, the H-bond-sensitive 877-cm-1 Trp band is strong and sharp, and the 1357/1341-cm-1 doublet has a large intensity ratio, approximately 1.5, for both FeII and FeIII cyt c. The 877-cm-1-band frequency shifts to 860 cm-1 when the Trp indole proton is replaced by a deuteron. This band was used to show that Trp H/D exchange in D2O is much faster for FeIII than FeII cyt c. The half-time for exchange at room temperature is estimated to be approximately 30 and approximately 5 h, respectively, for FeII and FeIII when examined at I = 0.005.(ABSTRACT TRUNCATED AT 250 WORDS)     

Monitoring the positioning of short polycationic peptides in model lipid bilayers by combining hydrogen/deuterium exchange and electrospray ionization mass spectrometry

Electrospray ionization mass spectrometry (ESI-MS) was used to analyze the hydrogen/deuterium exchange properties of the mastoparan peptide Apoica-MP during interactions with lipid vesicle membranes. Synthetic peptide was incorporated into large unilamellar vesicles (LUVs) of L-alpha-phosphatidylcholine (PC), resulting in proteoliposomes which were then diluted with D2O. After quenching deuteration by the addition of formic acid the H/D exchange was directly analyzed by ESI-MS. This strategy was used to investigate the architecture of the peptide in the membranes of PC LUVs. The deuterated peptide ions were analyzed under collision-induced dissociation (CID) mass spectrometry, which permitted the location of deuterons at the amide sites along the peptide backbone. Intramolecular hydrogen scrambling was investigated both in the free peptide and in its proteoliposome form. Some scrambling was observed for the free peptide; however, almost no scrambling occurred in the amide hydrogens of the peptide backbone embedded in the membrane. The CID spectra suggest that the N-terminal moiety of the peptide lies on the polar side of the lipid membrane, while the C-terminal region is embedded in the membrane. The protocol described here may be reliably applied to investigate the interaction of mastoparans with bilayer lipid systems.     

Investigation of secondary and tertiary structural changes of cytochrome c in complexes with anionic lipids using amide hydrogen exchange measurements: an FTIR study.

The structure of cytochrome c bound to anionic lipid membranes composed of dimyristoyl, dipalmitoyl, or dioleoyl phosphatidylglycerols, or of bovine heart cardiolipin, has been investigated by Fourier transform infrared spectroscopy. Only small changes in secondary structure, as registered by the amide I band of cytochrome c, were observed upon binding at temperatures below that of denaturation of the protein, and these were not coupled to the thermotropic phase transitions of the lipid. The denaturation temperature of the protein decreased by approximately 25-30 degrees upon binding, in a progression which correlated with that of the lipid phase transition temperatures, being approximately 7 degrees lower for complexes with dioleoyl than with dipalmitoyl phosphatidylglycerol. Large changes in the amide proton exchange characteristics, as monitored by the spectral shifts in the amide I band of the protein in D2O, were observed on binding cytochrome c to the lipid membranes. For the slowly exchanging population, the amide deuteration rates of the free protein were nearly independent of temperature, whereas those of the bound protein increased by up to two orders of magnitude over the temperature range from 10 to 40 degrees C. In addition, the extent of exchange differed between the bound and unbound protein. A structural transition in the bound protein was detected as a discontinuous step in Arrhenius plots of the deuterium exchange rates which occurred at a temperature in the region of 22 to 29 degrees C, depending on the lipid, far below that of denaturation. The temperature of this transition was determined by the physical state of the lipid, being 7 degrees lower for the lipids in the fluid state than for those in the gel state, and, for complexes with dimyristoyl phosphatidylglycerol, occurred at an intermediate temperature, being controlled by the lipid chain-melting transition at 27-28 degrees C. These results provide evidence for a coupling of the tertiary structure of the membrane-bound protein with the physical state of the membrane lipids.     

Beyond the EX1 limit: probing the structure of high-energy states in protein unfolding

Hydrogen exchange kinetics in native solvent conditions have been used to explore the conformational fluctuations of an immunoglobulin domain (CD2.domain1). The global folding/unfolding kinetics of the protein are unaltered between pH 4.5 and pH 9.5, allowing us to use the pH-dependence of amide hydrogen/deuterium exchange to characterise conformational states with energies up to 7.2kcal/mol higher than the folded ground state. The study was intended to search for discreet unfolding intermediates in this region of the energy spectrum, their presence being revealed by the concerted exchange behaviour of subsets of amide groups that become accessible at a given free energy, i.e. the spectrum would contain discreet groupings. Protection factors for 58 amide groups were measured across the pH range and the hydrogen-exchange energy profile is described.More interestingly, exchange behaviour could be grouped into three categories; the first two unremarkable, the third unexpected. (1) In 33 cases, amide exchange was dominated by rapid fluctuation, i.e. the free energy difference between the ground state and the rapidly accessed open state is sufficiently low that the contribution from crossing the unfolding barrier is negligible. (2) In 18 cases exchange is dominated by the global folding transition barrier across the whole pH range measured. The relationship between hydroxyl ion concentration and observed exchange rate is hyperbolic, with the limiting rate being that for global unfolding; the so-called EX1 limit. For these, the free energy difference between the folded ground state and any rapidly-accessed open state is too great for the proton to be exchanged through such fluctuations, even at the highest pH employed in this study. (3) For the third group, comprising five cases, we observe a behaviour that has not been described. In this group, as in category 2, the rate of exchange reaches a plateau; the EX1 limit. However, as the intrinsic exchange rate (k(int)) is increased, this limit is breached and the rate begins to rise again. This unintuitive behaviour does not result from pH instability, rather it is a consequence of amide groups experiencing two processes; rapid fluctuation of structure and crossing the global barrier for unfolding. The boundary at which the EX1 limit is overcome is determined by the equilibrium distribution of the fluctuating open and closed states (K(O/C)) and the rate constant for unfolding (k(u)). This critical boundary is reached when k(int)K(O/C)=k(u). Given that, in a simple transition state formalism: k(u)=K(#)k' (where K(#) describes the equilibrium distribution between the transition and ground state and k' describes the rate of a barrierless rearrangement), it follows that if the pH is raised to a level where k(int)=k', then the entire free energy spectrum from ground state to transition state could be sampled.     

A kinetic folding intermediate probed by native state hydrogen exchange

Stopped-flow fluorescence studies on the N-terminal domain of rat CD2 (CD2.d1) have demonstrated that folding from the fully denatured state (U) proceeds via the transient accumulation of an apparent intermediate (I) in a so-called burst phase that precedes the rate-limiting transition leading to the native state (N). A previous pH-dependent equilibrium hydrogen exchange (HX) study identified a subset of amides in CD2.d1 which, under EX2 conditions, exchange from N with free energies greater than or equal to the free energy difference between the N and I states calculated from the stopped-flow data. Under EX1 conditions the rates of HX for these amides tend towards an asymptote that matches the global unfolding rate calculated from the stopped-flow data, suggesting that exchange for these amides requires traversing the N-to-I transition state barrier. Exchange for these amides presumably occurs from exchange-competent forms comprising the kinetic burst phase therefore. To explore this idea further, native state HX (NHX) data have been collected for CD2.d1 under EX2 conditions using denaturant concentrations which span either side of the denaturant concentration where, according to the stopped-flow data, the apparent U and I states are iso-energetic. The data fit to a two-component, sub-global (sg)/global (g) NHX mechanism, yielding Delta G and m value parameters (where the m value is a measure of hydrocarbon solvation). Regression analysis demonstrates that the (m(sg), Delta G(sg)) and (m(g), Delta G(g)) values calculated for this subset of amides correspond with those describing the kinetic burst phase transition. This result confirms the ability of the NHX technique to explore the structural and energetic properties of kinetic folding intermediates.     

Characterization and calculation of a cytochrome c-cytochrome b5 complex using NMR data

To identify the binding site for bovine cytochrome b(5) (cyt b(5)) on horse cytochrome c (cyt c), cross-saturation transfer NMR experiments were performed with (2)H- and (15)N-enriched cyt c and unlabeled cyt b(5). In addition, chemical shift changes of the cyt c backbone amide and side chain methyl resonances were monitored as a function of cyt b(5) concentration. The chemical shift changes indicate that the complex is in fast exchange, and are consistent with a 1:1 stoichiometry. A K(a) of (4 +/- 3) x 10(5) M(-)(1) was obtained with a lower limit of 855 s(-)(1) for the dissociation rate of the complex. Mapping of the chemical shift variations and intensity changes upon cross-saturation NMR experiments in the complex reveals a single, contiguous interaction interface on cyt c. Using NMR data as constraints, a protein docking program was used to calculate two low-energy model complex clusters. Independent calculations of the effect of the cyt b(5) heme ring current-induced magnetic dipole on cyt c were used to discriminate between the different models. The interaction surface of horse cyt c in the current experimentally constrained model of the cyt c-cyt b(5) complex is similar but not identical to the interface predicted in yeast cyt c by Brownian dynamics and docking calculations. The occurrence of different amino acids at the protein-protein interface and the dissimilar assumptions employed in the calculations can largely account for the nonidentical interfaces.     

Intramolecular electron-transfer reaction within a diprotein complex of cytochrome c with ferrylmyoglobin modified with diethylenetriaminepentaacetic acid

Horse heart metmyoglobins modified with diethylenetriaminepentaacetic acid, metMb(DTPA)n (n=1, 2, 4, and 5), were characterized by a MALDI-TOF mass spectrometry, amino-acid sequence analysis, and UV-Vis and CD spectroscopies. The DTPA-binding sites on metMb were Lys47, Lys50, Lys87, Lys145, and Lys147 for metMb(DTPA)5, Lys47, Lys87, Lys145, and Lys147 for metMb(DTPA)4, Lys87 and Lys145 for metMb(DTPA)2, and Lys87 for metMbDTPA, respectively. The modified metMb(DTPA)n showed cytochrome c peroxidase-like activity more efficiently than native metMb: metMb(DTPA)5>metMb(DTPA)4>metMb(DTPA)2> metMbDTPA approximately equals native metMb. The first-order rate constants for the reactions of ferrylMb(DTPA)n (n=2, 4, and 5) with reduced cytochrome c [cyt c(II)] were saturated with concentrations of cyt c(II), suggesting that the electron transfer (ET) occurs within a diprotein complex. The intramolecular ET rate constants in the diprotein complex increased with increasing the number of DTPA ions. The reactions of native ferrylMb and ferrylMbDTPA with cyt c(II) obeyed a second-order rate law. A possible ET mechanism is proposed; cyt c(II) binds the DTPA-linked anionic patch around Lys87, Lys145, and Lys147 region of ferrylMb(DTPA)n.     

Mass spectral analysis of protein-based radicals using DBNBS. Nonradical adduct formation versus spin trapping

Protein-based radicals generated in the reaction of ferricytochrome c (cyt c) with H(2)O(2) were investigated by electrospray mass spectrometry (ESI-MS) using 3,5-dibromo-4-nitrosobenzenesulfonate (DBNBS). Up to four DBNBS-cyt c adducts were observed in the mass spectra. However, by varying the reaction conditions (0-5 molar equivalents of H(2)O(2) and substituting cyt c with its cyanide adduct which is resistant to peroxidation), noncovalent DBNBS adduct formation was inferred. Nonetheless, optical difference spectra revealed the presence of a small fraction of covalently trapped DBNBS. To probe the nature of the noncovalent DBNBS adducts, the less basic proteins, metmyoglobin (Mb) and alpha-lactalbumin, were substituted for cyt c in the cyt c/H(2)O(2)/DBNBS reaction. A maximum of two DBNBS adducts were observed in the mass spectra of the products of the Mb/H(2)O(2)/DBNBS reactions, whereas no adducts were detected following alpha-lactalbumin/H(2)O(2)/DBNBS incubation, which is consistent with adduct formation via spin trapping only. Titration with DBNBS at pH 2.0 yielded noncovalent DBNBS-cyt c adducts and induced folding of acid-denatured cyt c, as monitored by ESI-MS and optical spectroscopy, respectively. Thus, the noncovalent DBNBS-cyt c mass adducts observed are assigned to ion pair formation occurring between the negatively charged sulfonate group on DBNBS and positively charged surface residues on cyt c. The results reveal the pitfalls inherent in using mass spectral data with negatively charged spin traps such as DBNBS to identify sites of radical formation on basic proteins such as cyt c.     

Insights on the Conformational Ensemble of Cyt C Reveal a Compact State during Peroxidase Activity

Cytochrome c (cyt c) is known for its role in the electron transport chain but transitions to a peroxidase-active state upon exposure to oxidative species. The peroxidase activity ultimately results in the release of cyt c into the cytosol for the engagement of apoptosis. The accumulation of oxidative modifications that accompany the onset of the peroxidase function are well-characterized. However, the concurrent structural and conformational transitions of cyt c remain undercharacterized. Fast photochemical oxidation of proteins (FPOP) coupled with mass spectrometry is a protein footprinting technique used to structurally characterize proteins. FPOP coupled with native ion mobility separation shows that exposure to H₂O₂ results in the accumulation of a compact state of cyt c. Subsequent top-down fragmentation to localize FPOP modifications reveals changes in heme coordination between conformers. A time-resolved functional assay suggests that this compact conformer is peroxidase active. Altogether, combining FPOP, ion mobility separation, and top-down and bottom-up mass spectrometry allows us to discern individual conformations in solution and obtain a better understanding of the conformational ensemble and structural transitions of cyt c as it transitions from a respiratory role to a proapoptotic role.     

Thermodynamics of the reconstitution of tuna cytochrome c from two peptide fragments

Two peptide fragments from tuna cytochrome c (cyt c), N-fragment (residues 1-44 containing the heme) and C-fragment (residues 45-103), combine to form a 1:1 fragment complex. This was clearly proved by ion-spray mass spectrometry. It was found from CD and NMR spectra that the structure of the fragment complex formed is similar to that of an intact cyt c, although each isolated fragment itself is unstructured. Binding constants and enthalpies upon the complex formation were directly observed by isothermal titration calorimetry. Thermodynamic parameters (deltaG(o)b, deltaHb, deltaS(o)b, and deltaC(b)p)) associated with the complex formation were determined at various pHs and temperatures. DeltaHb was found to be almost independent of pH values. The change in heat capacity accompanying the complex formation (deltaC(b)p) was directly determined from the temperature dependence of deltaHb. In addition, the change in heat capacity and enthalpy upon tuna cyt c unfolding were determined by differential scanning calorimetry. Thermodynamic parameters for the unfolding/dissociation process of the fragment complex were compared with those for cyt c unfolding at pH 3.9 and 303 K. In a comparison of two unfolding processes, the heat capacity change of each was very close to the other, while both the unfolding enthalpy and entropy of the fragment complex were larger than those of tuna cyt c. These thermodynamic data suggest that the internal interactions between polar groups (hydrogen bonding) and nonpolar groups (van der Waals interactions) are preserved in the fragment complex as well as in the native state of cyt c.