6.7.3: Iron-sulfur Proteins and Models (Part 3)
- Page ID
- 300956
\( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)
\( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)
\( \newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\)
( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\)
\( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)
\( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\)
\( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)
\( \newcommand{\Span}{\mathrm{span}}\)
\( \newcommand{\id}{\mathrm{id}}\)
\( \newcommand{\Span}{\mathrm{span}}\)
\( \newcommand{\kernel}{\mathrm{null}\,}\)
\( \newcommand{\range}{\mathrm{range}\,}\)
\( \newcommand{\RealPart}{\mathrm{Re}}\)
\( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)
\( \newcommand{\Argument}{\mathrm{Arg}}\)
\( \newcommand{\norm}[1]{\| #1 \|}\)
\( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)
\( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\AA}{\unicode[.8,0]{x212B}}\)
\( \newcommand{\vectorA}[1]{\vec{#1}} % arrow\)
\( \newcommand{\vectorAt}[1]{\vec{\text{#1}}} % arrow\)
\( \newcommand{\vectorB}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)
\( \newcommand{\vectorC}[1]{\textbf{#1}} \)
\( \newcommand{\vectorD}[1]{\overrightarrow{#1}} \)
\( \newcommand{\vectorDt}[1]{\overrightarrow{\text{#1}}} \)
\( \newcommand{\vectE}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{\mathbf {#1}}}} \)
\( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)
\( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)
\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)Fe4S4 Ferredoxins (including HiPIPs)
We now turn our attention to proteins containing the Fe4S4 center. Historically, within this class a strong distinction was made between the "ferredoxins," which are low-potential (as low as -600 mV in chloroplasts) iron-sulfur proteins, and the "HiPIPs" = High Potential Iron Proteins, which have positive redox potentials (as high as +350 mV in photosynthetic bacteria). Although the HiPIP designation is still useful, proteins of both high and low potential are considered ferredoxins, whose key defining feature is the presence of iron and acid-labile sulfide.13
The Fe4S4 proteins participate in numerous electron-transfer functions in bacteria, and in some organisms (such as Clostridium) are the immediate electron donors for the nitrogenase and/or hydrogenase enzymes. The function of the HiPIPs seems obscure at present. In addition, Fe4S4 centers have been shown or postulated to occur in numerous microbial, plant, and mammalian redox enzymes, including nitrate reductase,104 sulfite reductase,24 trimethylamine dehydrogenase,105 succinate dehydrogenase,73,106 hydrogenase, and, possibly, in altered forms, nitrogenase. Table 7.1 lists some of the Fe4S4 ferredoxins and their properties.
In the Fe2S2 ferredoxins, combined spectroscopic, analytical, and model-system work led to an unequivocal assignment of the structural nature of the active site long before the crystallography was done. In contrast, for Fe4S4 systems and in particular the 8Fe-8S = 2Fe4S4 systems from bacteria, the initial chemical suggestions were fallacious, and even the number and stoichiometry of the clusters were in doubt. In these cases, crystallography provided the definitive structural information.
The first indication of the presence of the "thiocubane" structure came in 1968, when a 4-Å resolution study107 indicated a compact cluster of potentially tetrahedral Fe4 shape in the HiPIP from Chromatium vinosum. This finding did not lead to much excitement, since it was not yet appreciated that HiPIPs and ferredoxins were structurally similar. In 1972, the high-resolution structure solution of both Chromatium HiPIP108 and the 8Fe ferredoxin from Peptococcus aerogenes (formerly Microbacter aerogenes)101 confirmed the presence of virtually identical thiocubane clusters in the two proteins.108 Moreover, the structures for both oxidized and reduced HiPIP were deduced, and these revealed that the Fe4S4 cluster remained intact during the redox interconversion.109 Subsequently, four-iron clusters have been crystallographically confirmed in an Fe4S4 ferredoxin from Bacillus thermoproteolyticus,110,110a in Azotobacter vinelandii ferredoxin I (also previously called Shethna Fe-S protein II), which also contains a 3Fe-4S cluster,111,112 in the active form of aconitase,113 and in sulfite reductase, where the cluster is probably bridged by cysteine sulfur to a siroheme.
In all the proteins characterized to date, the Fe4S4 clusters adopt the thiocubane structure,108 which is discussed at greater length in the section on models. The clusters are usually bound to their proteins by four cysteine residues. As shown in Figure 7.11, in the P. aerogenes protein the two Fe4S4 clusters are bound by cysteines numbered 8, 11, 14, 18, 35, 38, 41, and 45.101,114 The presence of the Cys-x-x-Cys unit is again apparent. However, this sequence seems prominent in all Fe-S proteins, and so is not specific for a particular Fe-S site. At first glance one might expect one cluster to be bound by cysteines 8,11,14, and 18, the other by cysteines 35, 38, 41, and 45. Actually, one cluster is bound by cysteines 8, 11, 14, and 45, the other by cysteines 35, 38, 41, and 18. The binding of a given cluster by cysteine residues from different portions of the polypeptide chain apparently helps stabilize the tertiary structure of the protein and brings the two clusters into relatively close proximity, the center-center distance being 12 Å.114
The C. pasteurianum protein displays weak magnetic coupling, which leads to an unusual EPR spectrum115 consistent with the 12-Å cluster-cluster separation. However, the redox potentials for the two sites seem virtually identical at -412 mV, thus allowing the 8Fe ferredoxin to deliver two electrons at this low redox potential.115 Significant sequence identity indicates the likelihood that other 8Fe ferredoxins, such as the well-studied one from C. pasteurianum,116-118 have quite similar structures.
The thiocubane unit of Fe4S4 proteins can exist in proteins in at least three stable oxidation states. This so-called three-state modeI74,109,119,120 contrasts dramatically with the situation for Rd(1Fe), Fe2S2, and Fe3S4 systems, in which only two oxidation states are accessible through simple electron transfer for each center. For the thiocubane structure, the three accessible states can be designated Fe4S43+, Fe4S42+, and Fe4S4+, corresponding to [Fe(III)2Fe(II)], [Fe(III)2Fe(II)2], and [Fe(III)Fe(II)3] valence-state combinations, respectively. It is crucial to note that, in sharp contrast to the Fe2S2 and Fe3S4 sites, the oxidation states are not localized in the Fe4S4 clusters. In most cases, each Fe atom behaves as if it had the same average oxidation level as the other Fe atoms in the cluster. The redox interconversion of the Fe4S4 sites is shown in Figure 7.12. The Fe4S43+ \(\rightleftharpoons\) Fe4S42+ couple is the high-potential redox couple characteristic of HiPIPs; the Fe4S42+ \(\rightleftharpoons\) Fe4S4+ couple is responsible for the low-potential process characteristic of the classical ferredoxins. In any given protein under physiological conditions, only one of the two redox couples appears to be accessible and functional.
Both the Fe4S4+ and the Fe4S43+ states of the thiocubane cluster are paramagnetic and display characteristic EPR spectra (Figure 7.6C,D). The Fe4S43+ site in reduced ferredoxins46,48,49,119 displays a rhombic EPR signal (Figure 7.6C) with g = 1.88, 1.92, and 2.06. The oxidized form of low-potential ferredoxins is EPR-silent, and attempts to "superoxidize" it to achieve the Fe4S43+ state invariably lead to irreversible cluster decomposition, probably through a 3Fe-4S structure. The Fe4S43+ signal is usually referred to as the HiPIP signal (Figure 7.6D) and shows distinct g values at 2.04(g\(\perp\)) and 2.10(g\(\parallel\)); it is present in oxidized HiPIP but absent in reduced HiPIP.46,119 Reduction of HiPIP to a "super-reduced" state apparently occurs under partially denaturing conditions in aqueous DMSO.108 The observed axial EPR signal with g = 1.94 and 2.05 is assigned to the Fe4S4+ state characteristic of reduced ferredoxins. This result108 is consistent with structural and spectroscopic identity of the HiPIP and Fd sites, as required by the three-state model of the Fe4S4 proteins (Figure 7.12).
In Fe4S4 centers at each level of oxidation, electronic transitions give rise to characteristic visible and UV spectra, although the delocalized nature of the electronic states makes detailed assignment difficult. MCD spectra of clusters in the three states of oxidation are clearly distinguishable from each other and from MCD of Fe2S2 clusters.43,119 MCD, magnetic susceptibility, and Mössbauer spectra provide evidence that the S = \(\frac{1}{2}\) state, whose EPR signal is so distinct in reduced ferredoxins, may coexist at higher T with S = \(\frac{3}{2}\) and perhaps even higher spin states. Indeed, recent studies with model systems121,122 and theoretical treatments123,124 clearly support the ability of the Fe4S4 cluster to display a number of spin states that are in labile equilibria, which are influenced, perhaps quite subtly, by local structural conditions. The iron protein of nitrogenase also displays this behavior.
The Mössbauer spectra of Fe4S4 centers of ferredoxins reveal the equivalence of the Fe sites, and quadrupole splittings and isomer shifts at averaged values for the particular combination of oxidation states present.3,51,52 Representative spectra are shown in Figure 7.7. Magnetic coupling is seen for the paramagnetic states.
Resonance Raman spectra (and IR spectra) have been extensively investigated in C. pasteurianum ferredoxin and in model compounds.57,125 Selective labeling of either thiolate sulfur or sulfide sulfur with 34S allows modes associated with the Fe4S4 core to be distinguished from modes associated with the FeSR ligands. The band at 351 cm-1 is assigned to Fe-SR stretching, and Fe4S4 modes occur at 248 and 334 cm-1 in reduced ferredoxin from C. pasteurianum. There is little difference between the oxidized and reduced spectra, although an extra band at 277 cm-1 seems present in the oxidized protein. The Fe4Se4 substituted protein has also been studied.125
As in the 1Fe and 2Fe proteins, 1H NMR spectra reveal resonances from contact-shifted-CH2-groups of cysteinyl residues.125a However, unlike the other proteins, where all states are at least weakly magnetic, only the reduced ferredoxin and the oxidized HiPIP states show contact shifts.87a,125a,b,c
EXAFS studies on proteins and on model compounds clearly identify the Fe-S distance of ~2.35 Å and an Fe-Fe distance of 2.7 Å. These distances, as expected, vary only slightly with state of oxidation.125d
Fe4S4 Models
Judging from the ease with which models of Fe4S4 are prepared under a variety of conditions and their relative stability, the Fe4S42+ core structure seems to be a relatively stable entity, a local thermodynamic minimum in the multitude of possible iron-sulfide-thiolate complexes. The initial preparation and structural characterization126,127 of the models showed that synthetic chemistry can duplicate the biological centers in far-simpler chemical systems, which can be more easily studied in great detail.
The general synthetic scheme for Fe-S clusters is shown in Figure 7.13. Many different synthetic procedures can be used to obtain complexes with the Fe4S4 core.126-138,138a,b The multitude of preparative procedures is consistent with the notion that the Fe4S42+ core is the most stable entity present and "spontaneously self-assembles" when not limited by stoichiometric constraints.
The thiocubane structure can be viewed as two interpenetrating tetrahedra of 4Fe and 4S atoms. The 4S tetrahedra are the larger, since the S-S distance is ~3.5 Å, compared with the Fe-Fe distance of ~2.7 Å. The S4 tetrahedron encloses ~2.3 times as much volume as does the Fe4 tetrahedron.128 Key distances and angles for Fe4S4(SCH2C6H5)42- given in Table 7.4 are extremely similar to those found in oxidized ferredoxin and reduced HiPIP centers in proteins.127
Table 7.4 - Structural parameters for Fe4S4(SCH2C6H5)42-.
Atomsa | Average Distances | Number of Bonds | Type |
---|---|---|---|
Fe(1)-S(3) | 2.310 (3) | 8 | Sulfide |
Fe(1)-S(2) | 2.239 (4) | 4 | Sulfide |
Fe(1)-S(5) | 2.251 ( 3) | 4 | Thiolate |
Fe(1)-Fe(2) | 2.776 (10) | 2 | |
Fe-Fe(other) | 2.732 (5) | 4 |
Atomsa | Average Distances | Number of Bonds | Type |
---|---|---|---|
Fe-S-Fe | 73.8 (3) | 12 | |
S-Fe-S | 104.1 (2) | 12 | Sulfide-Fe-Sulfide |
S-Fe-S | 111.7-117.3 | 12 | Sulfide-Fe-Thiolate |
The idealized symmetry of Fe4S42+ model systems is that of a regular tetrahedron, i.e., Td. Though the distortion of the cube is quite pronounced, all known examples of the Fe4S2+ core show distortion, which lowers the symmetry at least to D2d. In most Fe4S2+ core structures, this distortion involves a tetragonal compression, which leaves four short and eight long Fe-S bonds.
Complexes with non-S-donor peripheral ligands have been prepared and studied. The halide complexes Fe4S4X42- (X = CI-, Br-, I-) have been prepared, and serve as useful starting points for further syntheses.129-133 The complex Fe4S4(OC6H5)42- can be prepared134 from the tetrachloride (or tetrathiolate) thiocubane by reaction with NaOC6H5 (or HOC6H5). There are a few examples of synthetic Fe4S42+ cores in which the peripheral ligands are not identical. For example, Fe4S4Cl2(OC6H5)22- and Fe4S4Cl2(SC6H5)22- have structures characterized by D2d symmetry.135 The complexes Fe4S4(SC6H5)2[S2CN(C2H5)2]2- and Fe4S4(SC6H4OH)42- are similarly asymmetric, containing both four- and five-coordinate iron.136-138 The presence of five-coordinate iron in the Fe4S4 cluster is notable, since it offers a possible mode of reactivity for the cluster wherever it plays a catalytic role (such as in aconitase). Complexes with Fe4Se2+ and Fe4Te42+ cores have also been prepared.138c,d
One structural analysis of Fe4S4(SC6H5)43-, which contains the reduced Fe4S4+ core, revealed a tetragonal elongation139 in the solid state. In contrast, analysis of Fe4S4(SCH2C6H5)43- revealed a distorted structure possessing C2v symmetry.102 It would appear that the Fe4S4+ clusters maintain the thiocubane structure, but are nevertheless highly deformable. Interestingly, when the solidstate C2v structure, Fe4S4(SCH2C6H5)43-, is investigated in solution, its spectroscopic and magnetic behavior change to resemble closely those of the Fe4S4(SC6H5)43- cluster,140 which does not change on dissolution. The simplest interpretation assigns the elongated tetragonal structure as the preferred form for Fe4S4+ cores with deformation of sufficiently low energy that crystal packing (or, by inference, protein binding forces) could control the nature of the distortions in specific compounds.128 The elongated tetragonal structure has four long and eight short bonds in the core structure. The terminal (thiolate) ligands are 0.03-0.05 Å longer in the reduced structure, consistent with the presence of 3Fe(ll) and 1Fe(III) in the reduced form, compared to 2Fe(II) and 2Fe(III) in the oxidized form. There is no evidence for any valence localization.128
The oxidized Fe4S43+ core defied isolation and crystallization in a molecular complex prior to the use of sterically hindered thiolate ligands. With 2,4,6 tris(isopropyl)phenylthiolate, the Fe4S4L4- complex could be isolated and characterized.141 The structure is a tetragonally compressed thiocubane with average Fe-S and Fe-SR distances 0.02 and 0.04 Å shorter than the corresponding distances in the Fe4S4L42- complex. Again, there is no evidence for Fe inequivalence or more profound structural distortion in this 3Fe(III)-1Fe(II) cluster. Clearly, the Fe4S4 clusters have highly delocalized bonding.
Evidence from model systems using sterically hindered thiolate ligands indicates the existence of an Fe4S44+, i.e., all-ferric fully oxidized cube.142 The existence of the complete series Fe4S4[(Cy)3C6H2S]4n (Cy =cyclohexyl; n = 0, -1, -2, -3) is implied by reversible electrochemical measurements. Clearly, five different states of the Fe4S4 core—including the (at least) transient fully oxidized state and the all-ferrous fully reduced state—may have stable existence. Although only the central three states have been shown to exist in biological contexts, one must not rule out the possible existence of the others under certain circumstances.
Recently, specifically designed tridentate ligands have been synthesized that bind tightly to three of the four Fe atoms in the thiocubane structure.143,143a,b The remaining Fe atom can then be treated with a range of reagents to produce a series of subsite-differentiated derivatives and variously bridged double-cubane units. These derivatives illustrate the potential to synthesize complexes that mimic the more unusual features of Fe4S4 centers that are bound specifically and asymmetrically to protein sites. The recently synthesized complex ion [(Cl3Fe4S4)2S]4-, containing two Fe4S4 units bridged by a single S2- ligand, illustrates the potential coupling of known clusters into larger aggregates.143c
The model-system work has made an important contribution to our understanding of the Fe4S4 centers. The existence of three states, the exchange of ligands, the redox properties, the metrical details of the basic Fe4S4 unit, and the subtleties of structural distortion can each be addressed through the study of models in comparison with the native proteins.