The Escherichia coli isc operon encodes key proteins involved in the biosynthesis of iron-sulfur (Fe-S) clusters. Whereas extensive studies of most ISC proteins have revealed their functional properties, the role of IscX (also dubbed YfhJ), a small acidic protein encoded by the last gene in the operon, has remained in question. Previous studies showed that IscX binds iron ions and interacts with the cysteine desulfurase (IscS) and the scaffold protein for cluster assembly (IscU), and it has been proposed that IscX functions either as an iron supplier or a regulator of Fe-S cluster biogenesis. We have used a combination of NMR spectroscopy, small-angle X-ray scattering (SAXS), chemical cross-linking, and enzymatic assays to enlarge our understanding of the interactions of IscX with iron ions, IscU, and IscS. We used chemical shift perturbation to identify the binding interfaces of IscX and IscU in their complex. NMR studies showed that Fe(2+) from added ferrous ammonium sulfate binds IscX much more avidly than does Fe(3+) from added ferric ammonium citrate and that Fe(2+) strengthens the interaction between IscX and IscU. We found that the addition of IscX to the IscU-IscS binary complex led to the formation of a ternary complex with reduced cysteine desulfurase activity, and we determined a low-resolution model for that complex from a combination of NMR and SAXS data. We postulate that the inhibition of cysteine desulfurase activity by IscX serves to reduce unproductive conversion of cysteine to alanine. By incorporating these new findings with results from prior studies, we propose a detailed mechanism for Fe-S cluster assembly in which IscX serves both as a donor of Fe(2+) and as a regulator of cysteine desulfurase activity.
The Escherichia coli isc operon encodes key proteins involved in the biosynthesis of iron-sulfur (Fe-S) clusters. Whereas extensive studies of most ISC proteins have revealed their functional properties, the role of IscX (also dubbed YfhJ), a small acidic protein encoded by the last gene in the operon, has remained in question. Previous studies showed that IscX binds iron ions and interacts with the cysteine desulfurase (IscS) and the scaffold protein for cluster assembly (IscU), and it has been proposed that IscX functions either as an iron supplier or a regulator of Fe-S cluster biogenesis. We have used a combination of NMR spectroscopy, small-angle X-ray scattering (SAXS), chemical cross-linking, and enzymatic assays to enlarge our understanding of the interactions of IscX with iron ions, IscU, and IscS. We used chemical shift perturbation to identify the binding interfaces of IscX and IscU in their complex. NMR studies showed that Fe(2+) from added ferrous ammonium sulfate binds IscX much more avidly than does Fe(3+) from added ferric ammonium citrate and that Fe(2+) strengthens the interaction between IscX and IscU. We found that the addition of IscX to the IscU-IscS binary complex led to the formation of a ternary complex with reduced cysteine desulfurase activity, and we determined a low-resolution model for that complex from a combination of NMR and SAXS data. We postulate that the inhibition of cysteine desulfurase activity by IscX serves to reduce unproductive conversion of cysteine to alanine. By incorporating these new findings with results from prior studies, we propose a detailed mechanism for Fe-S cluster assembly in which IscX serves both as a donor of Fe(2+) and as a regulator of cysteine desulfurase activity.
The iron–sulfur
(Fe–S) cluster is an ancient, yet
still abundant, protein cofactor that is essential for various biological
activities.[1] Although Fe–S clusters
assemble spontaneously from iron and sulfide ions under anaerobic
conditions, cells maintain strictly regulated machinery for Fe–S
cluster biosynthesis owing to the toxicity of free iron and sulfide
ions.[2] Prokaryotes have evolved three major
systems for Fe–S cluster biogenesis: the nitrogen fixation
(NIF), the iron–sulfur cluster (ISC), and the sulfur utilization
factor (SUF) systems.[2] Of these, the ISC
system is responsible for assembling and supplying Fe–S clusters
to the majority of iron–sulfur proteins involved in metabolic
processes.[3] Higher eukaryotes make use
of an orthologous set of ISC proteins for Fe–S cluster biosynthesis
in their mitochondria.[4,5]The biosynthesis of iron–sulfur
proteins consists of two
steps: (i) the assembly of clusters on the scaffold protein and (ii)
the transfer of the assembled cluster to an apo-iron–sulfur
protein.[3] In Escherichia
coli, cluster assembly involves IscU as the scaffold
protein; sulfur is produced by the transformation of cysteine to alanine
catalyzed by the cysteine desulfurase (IscS);[6] electrons are provided by reduced ferredoxin upon its interaction
with IscS;[7,8] and iron ions are donated by a presumed
iron protein. In E. coli, cluster transfer
involves a DnaJ-type cochaperone (HscB), which binds to IscU containing
an assembled Fe–S cluster and targets the complex to a DnaK-type
chaperone bound to ATP (HscA:ATP). Cluster transfer from IscU to a
target apoprotein occurs in a subsequent process involving ATP hydrolysis.[9,10] The scaffold protein (IscU) is metamorphic in that it adopts two
different conformations (S and D) that are interconvertible and stabilized
differentially by molecular interactions.[11−13] Initial interaction
with IscS stabilizes the D-state of IscU, which does not bind metals
and whose unligated cysteinyl thiol groups are free to pick up sulfur
produced by the cysteine desulfurase. Upon cluster assembly, IscU
converts to the S-state[13] and binds preferentially
to the cochaperone (HscB), which targets the complex to the ATP-bound
chaperone (HscA:ATP). Fe–S cluster release and transfer involves
the conversion of IscU back to its D-state through preferential interaction
of this state with the ADP bound chaperone (HscA:ADP). Finally, exchange
of the ADP bound to HscA with ATP releases IscU.[12]It has been assumed that Fe–S cluster biosynthesis
is highly
regulated. Currently, the best understood mechanism of regulation
is by bacterial frataxin (CyaY), a protein not encoded by the E. coliisc operon. CyaY has been
shown to inhibit in vitro Fe–S cluster reconstitution
by forming a complex with IscS.[14,15] We demonstrated that
the binding of CyaY to IscS inhibits the interaction of IscU with
IscS, thus blocking this key step in cluster assembly.[7] Another potential regulator of cluster biosynthesis is
IscX, the ∼7.7 kDa protein encoded by the last gene in the isc operon. Structural studies have shown that IscX (also
called YfhJ) adopts a compact α-helical structure that exposes
several acidic residues that mediate iron binding.[16,17] Previous studies also reported that IscX binds directly to IscS
and suggested that it may play a role in Fe–S cluster assembly.[17,18] Intriguingly, bioinformatic analysis of genomes from various organisms
found that the IscX gene co-occurs with that for IscS, whereas it
correlates poorly with the presence of the gene for CyaY. The fact
that some eukaryotes that lack CyaY have orthologs of IscX, suggested
that these two proteins might have redundant functions.[17]We show here that IscX acts as a regulator
of Fe–S cluster
assembly. By combining results from NMR spectroscopy, small-angle
X-ray scattering (SAXS), and chemical crossing-linking experiments
we confirmed the previously identified interaction between IscX and
IscS, identified a separate interaction between IscX and IscU, and
demonstrated that the three proteins form a ternary complex. Analysis
of the cysteine desulfurase activity of IscS revealed that the enzyme
is active in both the IscU–IscS and IscX–IscS binary
complexes but is greatly diminished in the IscX–IscU–IscS
ternary complex. We found, furthermore, that the addition of IscX
inhibits the assembly of Fe–S clusters on IscU in an in vitro Fe–S cluster assembly reaction. Thus, IscX
and CyaY inhibit cluster assembly by very different mechanisms. We
propose a mechanism for Fe–S cluster assembly that incorporates
these and earlier findings.
Experimental Procedures
Expression
and Purification of Proteins
We used previously
described procedures to prepare samples of IscS,[13] CyaY,[7] Fdx,[7] and unlabeled and uniformly 15N-labeled IscU.[11,19] The procedures used to prepare unlabeled and 15N-labeled
IscX are presented in the Supporting Information.
NMR Spectroscopy
The buffer used for NMR samples contained,
unless stated otherwise, 20 mM Tris·HCl pH 7.5, 0.5 mM EDTA,
150 mM NaCl, and 5 mM dithiothreitol (DTT) with 7% D2O,
0.7 mM DSS, and 0.02% sodium azide. All NMR spectra were acquired
at 25 °C on 600 or 900 MHz Varian VNMRS spectrometers (Agilent)
equipped with z-gradient cryogenic probes. Raw data
were processed with NMRPipe,[20] and data
were analyzed with the SPARKY[21] software
suite.Previously assigned NMR signals from IscX (BMRB; accession
number 6776)[17] were checked and extended
by reference to a 3D 1H-1H NOESY 15N-HSQC data set obtained with 0.8 mM [U-15N]-IscX. We
were able to assign the backbone 1HN-15N signals from all nonprolyl residues except M1, G2, F29, T30, and
E51.The IscX titration experiments were conducted by adding
0.2 mM
IscS, 0.4 mM IscU, 0.4 mM CyaY, or 0.4 mM Fdx to a sample of 0.2 mM
[U-15N]-IscX. 2D 15N-TROSY-HSQC spectra of the
[U-15N]-IscX sample were recorded before and after addition
of the previously specified proteins.To measure the NMR signal
perturbations of [U-15N]-IscX
and [U-15N]-IscU upon addition of unlabeled IscU and IscX,
respectively, we started with a sample containing 0.2 mM [U-15N]-IscX/IscU. We collected a 2D 15N-TROSY-HSQC spectrum
before and after adding an aliquot of unlabeled IscU/IscX. We continued
adding aliquots of unlabeled IscU/IscX and collecting a spectrum,
until the peak movement appeared to saturate. The final concentrations
of the unlabeled proteins were 0.8 mM. We quantified the perturbations
(ΔδNH) of assigned signals by the equation:
ΔδNH = [(ΔδH)2 + ((ΔδN)/6)2]1/2.The titration experiments of [U-15N]-IscX with Fe2+ or Fe3+ were carried out as follows. A sample
containing 0.5 mM [U-15N]-IscX, 20 mM Tris·HCl pH
7.5, 150 mM NaCl, 0.7 mM DSS, and 0.02% sodium azide in 7% D2O/93% H2O was prepared in an anaerobic chamber (O2 level <5 ppm; Coy Laboratory). The sample was transferred
to an airtight NMR tube (Wilmad) in the anaerobic chamber. Subsequent
samples were prepared in the anaerobic chamber by addition of aliquots
of either ferrous ammonium sulfate (for titration with Fe2+) or ferric ammonium citrate (for titration with Fe3+).
2D 15N-TROSY-HSQC spectra were acquired with each sample.The titration experiment of IscX with IscU in the presence of Fe2+ was initiated by collecting a 2D 15N-TROSY-HSQC
spectrum of a sample containing 0.2 mM [U-15N]-IscX and
0.6 mM ferrous ammonium sulfate in 20 mM Tris·HCl pH 7.5, 150
mM NaCl, and 5 mM DTT with 7% D2O, 0.7 mM DSS, and 0.02%
sodium azide. The sample was prepared anaerobically. After obtaining
the first spectrum, IscU was added anaerobically to the sample to
achieve a concentration of 0.6 mM, and a 2D 15N-TROSY-HSQC
spectrum was taken.
SAXS Data Acquisition and Analysis
Protein samples
for SAXS were dialyzed extensively against 20 mM Tris·HCl pH
7.5, 150 mM NaCl buffer prior to data collection. The protein complexes
investigated in this study were prepared by mixing the proteins in
equimolar ratios. We initially attempted to purify each protein complex
by gel filtration chromatography (HiLoad 16/60 Superdex 200, GE Healthcare);
however, each mixture, with the exception of IscU–IscS, eluted
from the column as its individual protein components. Prior to SAXS
data collection, all protein samples and dialysate buffer were filtered
through a 0.2 μm filter to remove any small particles or aggregates
in solution. SAXS data for each protein complex were collected at
a minimum of three concentrations ranging from 1.3 to 10.0 mg/mL.
We did not observe significant interparticle interactions for any
of the concentrations used in our SAXS studies.SAXS experiments
were carried out both at Sector 12-ID of the Advanced Photon Source
(APS), Argonne National Laboratory, and on a Bruker Nanostar benchtop
SAXS system at the National Magnetic Resonance Facility at Madison
(NMRFAM). Synchrotron data at the APS were recorded with an X-ray
radiation energy of 14 keV. The sample to detector distance was ∼2
m allowing for simultaneous collection of q-ranges
(q = 4πsin θ/λ) for SAXS (0.004
> q > 0.522 Å–1) and
WAXS
(0.990 > q > 2.860 Å–1) data.
Protein and buffer samples were loaded separately into a 1 mm thick
capillary and flowed back and forth during data collection. Data were
collected as a series of 1 s exposures for a total exposure time of
20 s. The data sets were converted to 1D scattering profiles and averaged
post removal of any scattering profiles that differed significantly—usually
as the result of bubble formation.The Bruker Nanostar system
was equipped with a rotating anode (Cu)
Turbo X-ray Source and a Vantec-2000 (2048 × 2048 pixel) detector
(Bruker AXS). The sample-to-detector distance was set at ∼1
m allowing for the detection range: 0.012 > q >
0.240
Å–1. Sample and buffer scattering data were
collected for 4 h with frames recorded every hour. Each frame was
compared to check for radiation damage, and none was detected over
the course of the experiments. The SAXS data sets were then averaged
and converted to 1D scattering profiles for further analysis.Buffer background subtraction for the SAXS data recorded at the
APS was guided by use of the corresponding WAXS data and carried out
with IGOR PRO (WaveMetrics) software. After buffer subtraction, the
ATSAS[22] software suite was used to process
the SAXS data. The radius of gyration (Rg) for each protein and protein complex reported in this study was
determined by using the Guinier approximation in the q range, such that qmax·Rg < 1.3. The software package GNOM[23] was used to obtain pairwise distance distribution functions
for each protein and protein complex. Dmax was varied in increments of 2 Å until the pairwise distance
distribution function dropped off smoothly to zero. The Rg values determined from GNOM were in very good agreement
with those determined by the Guinier approximation (Figure S1). The output from GNOM was then used in conjunction
with DAMMIF to generate 20 independent ab initio dummy
atom models to gauge the molecular shape of each protein complex.[24] Given prior knowledge of similar complexes with
IscS,[15,25] we imposed P2 symmetry
in our structural calculations. Most of the 20 models for each complex
exhibited excellent agreement with the experimental scattering curve
(χ2 < 1). However, ∼40% of the models for
IscU–IscS exhibited distortions inconsistent with the known
structures of IscU and IscS; we excluded these structures upon visual
inspection. The variation in the IscU–IscS shape models could
be due to the dynamic nature of IscU upon binding IscS or a lack of P2 symmetry. The final accepted models had a normalized
spatial discrepancy (NSD) of <1. When we did not enforce P2 symmetry, all models were in excellent agreement (average
NSD of 0.78) and were nearly identical to the accepted models achieved
by enforcing P2 symmetry for each complex (IscX–IscS,
IscU–IscS, IscX–IscU–IscS). We used DAMAVER[26] to average the individual shape models in generating
the reported shape models for each complex.We used the software
package SASREF[27] to carry out rigid-body
modeling simulations of the binary and ternary
complexes of IscS, IscU, and IscX. The restraints used in docking
simulations were derived from NMR data reported here and in previous
studies.[15,25] Specifically, IscX was restrained to localize
about the positively charged binding patch on IscS (residues 220–223),
and IscU was restrained to localize in the region of IscS as determined
from point mutation studies that influenced binding interactions.[15] The CRYSOL[28] software
suite was used to compare the models resulting from the rigid-body
modeling simulations to experimental data.We used the recently
proposed χfree2 statistic[29] to validate the models
derived from rigid-body modeling simulations
and the ScÅtter software package (http://www.bioisis.net/tutorial) to calculate χfree2 with 5000 selection rounds. The effects of
weak complex formation were investigated using the “minimal
ensemble search” (MES) ensemble selection algorithm.[30] The structure pool used in deriving ensembles
contained monomeric and dimeric structures of IscX, IscU, and IscS,
the structure of the IscX–IscU complex derived from NMR chemical
shift perturbations, and the complexes of IscX–IscU, IscU–IscS,
and IscX–IscU–IscS derived from rigid-body modeling
simulations.
Cross-Linking Experiments
The cross-linking
experiments
to identify interactions among IscX, IscU, and IscS were initiated
in solutions containing various combinations of the three proteins
at 1 mg/mL along with excess DTT. After a 10–20 min incubation,
the solvent in each sample was exchanged to 50 mM HEPES·NaOH
pH 7.5 by employing a zeba spin desalting column (Thermo Scientific).
Each sample was incubated with 20-fold Sulfo-SMCC (Thermo Scientific)
for 1 h at ambient temperature. Sulfo-SMCC is an amine-to-sulfhydryl
chemical cross-linker whose reactive groups are separated by 0.83
nm. Each cross-linking reaction was quenched by adding excess Tris
and DTT, and the product was analyzed by SDS-PAGE. The band corresponding
to the IscX–IscU–IscS ternary complex was excised and
analyzed further by mass spectrometry, which confirmed the expected
mass of the ternary complex (data not shown).
Cysteine Desulfurase Activity
Assay
The assay was initiated
by anaerobically preparing 1 mL reaction mixtures containing 50 mM
Tris·HCl at pH 7.5, 5 mM DTT, 125 μM ferrous ammonium sulfate,
and 0.5 μM IscS alone and with other proteins (IscX, CyaY, IscU,
IscU + IscX, or IscU + CyaY). The concentration of IscU (25 μM)
was set as a 50-fold excess over IscS to mimic the conditions of the
Fe–S cluster reconstitution experiment (see below). IscX and
CyaY were added at two different concentrations: one equivalent to
the concentration of IscS and another equivalent to that of IscU.
Sulfide production was initiated by the addition of l-cysteine
to an initial concentration of 125 μM. After 20 min anaerobic
incubation at ambient temperature, 300 μL of the reaction mixture
was diluted to 800 μL, and 100 μL of 20 mM N,N-dimethyl-p-phenylenediamine
in 7.2 N HCl and 100 μL of 30 mM FeCl3 in 1.2 N HCl
were added to quench the reaction and to convert sulfide to methylene
blue. The quenched reaction was incubated for 20 min, and then the
absorbance at 670 nm was measured and used to estimate the amount
of sulfide by comparison to a standard curve obtained from known concentrations
of Li2S.
In Vitro Assembly of Fe–S Clusters
on IscU
Fe–S
cluster assembly experiments were conducted in an anaerobic chamber
(Coy Laboratory). The reaction mixture contained 0.5 μM IscS,
25 μM IscU, 5 mM DTT, and 125 μM ferrous ammonium sulfate
in a 50 mM Tris·HCl buffer at pH 7.5. We also investigated the
effects of added IscX or CyaY on this Fe–S assembly reaction.
Cluster assembly reactions were initiated by the addition of 125 μM l-cysteine. The mixtures were transferred to 1 cm path length
cuvettes, which were capped with rubber septa, and the Fe–S
cluster assembly reaction was monitored by following the absorbance
at 456 nm.
Results
IscX Binds IscS and Participates
in an IscX–IscU–IscS
Ternary Complex; However, IscX, CyaY, and Fdx Compete for an Overlapping
Binding Site on IscS
We interpreted the 2D 15N-TROSY-HSQC
spectrum of [U-15N]-IscX (Figure 1A) in terms of the assigned chemical shifts deposited in the BMRB.[17] We also collected a 3D 1H-1H NOESY–15N-HSQC spectrum of [U-15N]-IscX
to confirm and extend the resonance assignments. The addition of unlabeled
IscS led to broadening of signals from [U-15N]-IscX (Figure 1B) as consistent with the formation of a high molecular
weight complex. A set of these IscX peaks (R9, I11, A14, D17, V60,
W61, D63, and E64) broadened noticeably in advance of the others upon
the addition of 0.5 equiv IscS (data not shown). The IscX residues
affected corresponded to those in the previously proposed interaction
face with IscS.[17]
Figure 1
IscX–IscS complex
accommodates subsequent binding of IscU,
whereas added CyaY or Fdx displace IscX from IscS. (A) 2D 15N-TROSY-HSQC spectrum of [U-15N]-IscX. (B) The addition
of 1 equiv of unlabeled IscS to the sample shown in A led to the broadening
of most of the 2D 15N-TROSY-HSQC signals from [U-15N]-IscX as expected for the formation of an IscX–IscS complex.
(C) 2D 15N-TROSY-HSQC spectrum of the sample in B following
the addition of 2 equiv of unlabeled IscU. Further broadening of the
signals from [U-15N]-IscX are consistent with the formation
of an IscX–IscU–IscS ternary complex. (D) Results from
the chemical cross-linking experiment used to investigate the formation
of protein–protein complexes. Different combinations of IscS
(S), IscU (U), and IscX (X) were incubated with a chemical cross-linker,
and the products were analyzed by SDS PAGE. The mixture containing
all three proteins (lane 7) showed a band corresponding to the expected
mass of the ternary complex (XUS). The other mixtures (lane 2: IscU
alone, lane 3: IscS alone, lane 4: IscX alone, lane 5: IscU + IscS,
lane 6: IscX + IscS) yielded bands corresponding the expected masses
of the labeled species (U2, dimeric IscU; US, IscU–IscS;
XS, IscX–IscS); bands corresponding to most of these species
were also observed in the cross-linked mixture of the three proteins
(lane 7). Lane 1 shows the control mixture of the three proteins untreated
with cross-linker. (E) The addition of 2 equiv of unlabeled CyaY to
the sample shown in B partially restored the 2D 15N-TROSY-HSQC
signals from unbound [U-15N]-IscX, indicating that CyaY
displaces IscX bound to IscS. (F) The addition of 2 equiv of unlabeled
Fdx to the sample shown in B yielded 2D 15N-TROSY-HSQC
signals corresponding to unbound [U-15N]-IscX, indicating
that Fdx displaces IscX from IscS.
IscX–IscS complex
accommodates subsequent binding of IscU,
whereas added CyaY or Fdx displace IscX from IscS. (A) 2D 15N-TROSY-HSQC spectrum of [U-15N]-IscX. (B) The addition
of 1 equiv of unlabeled IscS to the sample shown in A led to the broadening
of most of the 2D 15N-TROSY-HSQC signals from [U-15N]-IscX as expected for the formation of an IscX–IscS complex.
(C) 2D 15N-TROSY-HSQC spectrum of the sample in B following
the addition of 2 equiv of unlabeled IscU. Further broadening of the
signals from [U-15N]-IscX are consistent with the formation
of an IscX–IscU–IscS ternary complex. (D) Results from
the chemical cross-linking experiment used to investigate the formation
of protein–protein complexes. Different combinations of IscS
(S), IscU (U), and IscX (X) were incubated with a chemical cross-linker,
and the products were analyzed by SDS PAGE. The mixture containing
all three proteins (lane 7) showed a band corresponding to the expected
mass of the ternary complex (XUS). The other mixtures (lane 2: IscU
alone, lane 3: IscS alone, lane 4: IscX alone, lane 5: IscU + IscS,
lane 6: IscX + IscS) yielded bands corresponding the expected masses
of the labeled species (U2, dimeric IscU; US, IscU–IscS;
XS, IscX–IscS); bands corresponding to most of these species
were also observed in the cross-linked mixture of the three proteins
(lane 7). Lane 1 shows the control mixture of the three proteins untreated
with cross-linker. (E) The addition of 2 equiv of unlabeled CyaY to
the sample shown in B partially restored the 2D 15N-TROSY-HSQC
signals from unbound [U-15N]-IscX, indicating that CyaY
displaces IscX bound to IscS. (F) The addition of 2 equiv of unlabeled
Fdx to the sample shown in B yielded 2D 15N-TROSY-HSQC
signals corresponding to unbound [U-15N]-IscX, indicating
that Fdx displaces IscX from IscS.We investigated whether other proteins active in Fe–S
cluster
assembly, namely IscU, CyaY, and Fdx, affect formation of the IscX–IscS
complex. Previous studies had shown that IscX, IscS, and IscU form
a ternary complex, whereas CyaY and IscX were found to compete for
a conserved positively charged binding site on IscS.[25] We found that the addition of IscU perturbed the NMR spectrum
of [U-15N]-IscX mixed with an equivalent amount of IscS
(Figure 1C), as expected for a ternary complex.
Chemical cross-linking experiments also were consistent with an IscX–IscU–IscS
ternary complex (Figure 1D). On the other hand,
the addition of CyaY (Figure 1E) or Fdx (Figure 1F) to the mixture of [U-15N]-IscX and
IscS restored sharp peaks of free [U-15N]-IscX, indicating
that CyaY, Fdx, and IscX compete for overlapping binding sites on
IscS.
SAXS Studies Provide a Low-Resolution Model for the IscX–IscU–IscS
Ternary Complex
Investigations of the complexes between IscS
and its binding partners pose a challenge owing to the disparity in
molecular mass between IscS (90 kDa homodimer) and IscU (28 kDa for
two molecules) or IscX (14 kDa for two molecules). This challenge
is exacerbated by their relatively weak binding interactions. The
dissociation constants for IscS and its binding partners are in the
low μM range: IscU (1.5 μM), Fdx (1.5 μM), and CyaY
(23 μM).[8,15]Before examining the ternary
complex, we investigated the IscS homodimer alone and its binary complexes
(IscU–IscS, IscX–IscS, Fdx–IscS, and CyaY–IscS).
The IscU–IscS complex had been studied previously by SAXS,[15] NMR,[13] and X-ray
crystallography.[25] Previous SAXS studies[15] revealed that the IscU–IscS complex is
elongated relative to the IscS homodimer with the maximum end-to-end
distance (Dmax) expanding from ∼110
to 130 Å. Further, the radius of gyration of the complex (36
Å) was greater than that of the IscS homodimer (31 Å).[15] Our results confirmed these observations (Figures 2 and S1; Table S1). To further verify formation of the
IscU–IscS complex, we also determined its molecular mass by
SAXS. The molecular mass of globular proteins typically is determined
from SAXS data by reference to zero angle scattering intensities (I(0)) obtained as a function of concentration for globular
protein standards, such as lysozyme or BSA.[31] In addition to this approach, we used the new SAXS invariant parameter
(Vc)[29] to determine
the molecular mass of the complex. Whereas the zero angle scattering I(0) method requires the species to be globular, the Vc approach works with both compact and disordered
molecules. The I(0) and Vc approaches yielded molecular masses for the IscS homodimer of 88
and 81 kDa, respectively, both lower than the theoretical value of
90 kDa. This discrepancy could be the result of inherent errors in
each technique (∼10%) or to the presence of monomeric IscS.
Next, we applied the I(0) and Vc approaches to the IscS–IscU complex and obtained molecular
masses of 102 and 92 kDa, respectively. Both methods yielded molecular
masses larger than for the IscS homodimer but smaller than the theoretical
value of 118 kDa; again the discrepancy could reflect incomplete IscS–IscU
complex formation owing to the low association constant. To explore
the influence of incomplete complex formation on the observed SAXS
data, we simulated the population-weighted linear combination of the
scattering of each particle in the mixture (Figure
S2). We also used the minimal ensemble search (MES) algorithm[30] to study the impact of weak complex formation
on our experimental data for the IscU–IscS complex (Figure S3). Ensembles of size 1–4 were
selected from a pool of structures that would be present in the scenario
of weak complex formation. Regardless of the allowed ensemble size,
the IscU–IscS structure was selected over competing structures
by >90%. These results indicate that the observed scattering profile
is largely influenced by that of the IscU–IscS complex. Our
simulations indicated that, whereas incomplete complex formation does
alter the observed scattering profile, the derived Rg, Dmax, and pairwise distance
distributions still serve to define the binding interface, even at
levels of IscS–IscU complex formation as low as 60%. Thus,
SAXS can provide detailed structural information about these weak
complexes.
Figure 2
Structural models from SAXS data. (A) Experimental SAXS data (circles)
recorded for IscS (blue), IscU + IscS (purple), IscX + IscS (red),
and IscX + IscU + IscS (green). Fits of the molecular models for IscS
(PDB 1P3W) and
those determined from rigid-body modeling to experimental SAXS are
plotted as solid lines. (B) Pairwise distance distribution functions
derived from experimental SAXS data (solid-lines) for IscS (blue),
IscU + IscS (purple), IscX + IscS (red), and IscX + IscU + IscS (green)
compared to those derived from the rigid-body modeling derived structures
(dashed-lines). (C) Molecular models of IscS (black, PDB 1P3W), IscU–IscS
(purple), IscX–IscS (red), and IscX–IscU–IscS
(green) determined from rigid-body modeling simulations. The structures
used for each complex component in the rigid-body modeling simulations
were: IscS (blue; PDB 1P3W),[32] IscU (purple; PDB 2L4X),[33] and IscX (red; PDB 2BZT).[17] The resulting
structures from rigid-body modeling are overlaid with ab initio shape models determined from the SAXS data with DAMMIF.[24]
Structural models from SAXS data. (A) Experimental SAXS data (circles)
recorded for IscS (blue), IscU + IscS (purple), IscX + IscS (red),
and IscX + IscU + IscS (green). Fits of the molecular models for IscS
(PDB 1P3W) and
those determined from rigid-body modeling to experimental SAXS are
plotted as solid lines. (B) Pairwise distance distribution functions
derived from experimental SAXS data (solid-lines) for IscS (blue),
IscU + IscS (purple), IscX + IscS (red), and IscX + IscU + IscS (green)
compared to those derived from the rigid-body modeling derived structures
(dashed-lines). (C) Molecular models of IscS (black, PDB 1P3W), IscU–IscS
(purple), IscX–IscS (red), and IscX–IscU–IscS
(green) determined from rigid-body modeling simulations. The structures
used for each complex component in the rigid-body modeling simulations
were: IscS (blue; PDB 1P3W),[32] IscU (purple; PDB 2L4X),[33] and IscX (red; PDB 2BZT).[17] The resulting
structures from rigid-body modeling are overlaid with ab initio shape models determined from the SAXS data with DAMMIF.[24]In contrast to IscU, the addition of IscX to the IscS homodimer
did not result in a significant change in the Dmax or Rg values (Figures 2 and 3; Table S1). These results are consistent with IscX binding
near the dimerization interface of IscS rather than elongating the
complex like IscU (Figure 3).
Figure 3
Comparison of results
from SAXS experiments for several complexes
involving IscS. (A) Cartoon representations of the IscX–IscS,
IscU–IscS, Fdx–IscS,[8] CyaY–IscS,[15] and IscX–IscU–IscS complexes.
(B) Experimentally determined radius of gyration for IscS and the
complexes depicted in A. (C) Experimentally determined Dmax for IscS and the complexes depicted in A. (D) Distance
distribution functions determined from experimental SAXS data from
IscS and the complexes depicted in A.
Comparison of results
from SAXS experiments for several complexes
involving IscS. (A) Cartoon representations of the IscX–IscS,
IscU–IscS, Fdx–IscS,[8] CyaY–IscS,[15] and IscX–IscU–IscS complexes.
(B) Experimentally determined radius of gyration for IscS and the
complexes depicted in A. (C) Experimentally determined Dmax for IscS and the complexes depicted in A. (D) Distance
distribution functions determined from experimental SAXS data from
IscS and the complexes depicted in A.CyaY, Fdx, and IscX are each reported to bind to same conserved
positively charged patch at the IscS homodimer interface (Figure 3).[8,15] As with the IscX–IscS
binary complex, we observed no significant change in the Dmax or Rg values upon formation
of the binary CyaY–IscS and Fdx–IscS complexes (Figure 3B,C). We also identified congruent changes in the
distance distribution function for all three complexes relative to
the IscS homodimer (Figure 3D). With the exception
of CyaY–IscS, the molecular masses determined from SAXS data
by the I(0) approach, as with the IscU–IscS
complex, were systematically ∼20% lower than the corresponding
theoretical values (Table S1). Again, this
probably is a consequence of the complexes not being saturated owing
to the weak binding affinities. The related binding sites shown by
SAXS are all consistent with the competitive binding interplay among
IscX, CyaY, and Fdx, as observed here by NMR. Thus, our SAXS and NMR
data strongly support that all three proteins bind to and compete
for a similar site on IscS.SAXS experiments on a mixture of
IscS, IscU, and IscX revealed
an expansion in both Dmax and Rg relative to the IscS homodimer with values
of 130 and 35 Å, respectively (Figure 3B,C). Identification of the ternary complex cannot simply be made
by comparing changes in the Dmax or Rg relative to the IscS homodimer because similar
changes were observed for the IscU–IscS complex. Interestingly,
inspection of the distance distribution function of the IscS, IscU,
IscX mixture revealed a hybrid of the changes observed for the binary
complexes IscU–IscS and IscX–IscS (Figures 2 and 3). Here the distance
distribution function of the complex showed an expansion of Dmax (130 Å) from that of the IscS homodimer
(105 Å). This expansion of Dmax is
consistent with IscU binding on the periphery of the IscS homodimer
when in the ternary complex. The distance distribution function of
the ternary complex relative to the IscU–IscS complex had an
expansion of the most probable distance (Figure 3D), suggesting that IscX occupies the same binding site in the ternary
complex as in the binary complex. Similar to the binary complexes,
the molecular mass of the ternary complex calculated from the SAXS
data was ∼20% below the theoretical value. As with the binary
complexes, we used simulations to validate the ability of SAXS to
detect the presence of an unsaturated ternary complex and found that
the overall shape of the scattering curve was constant at saturation
levels above 50% (Figure S2). Furthermore,
the Porod volumes measured for each complex were consistent with ternary
complex formation: IscX–IscU–IscS yielded a larger Porod
volume than either of the binary complexes (IscX–IscS or IscU–IscS)
(Table S1).Assuming that the known
structures of IscS, IscX, and IscU are
mostly maintained upon forming a complex, we used the SASREF[27] software package to carry out rigid-body modeling
simulations to generate molecular models of each complex (IscU–IscS,
IscX–IscS, and IscX–IscU–IscS) consistent with
our experimental SAXS data. The docking simulations used the interaction
sites determined here by NMR and by previous structural and mutagenesis
studies as structural restraints. First, we carried out SAXS-based
rigid-body modeling simulations of the X-ray structure of IscS (1P3W)[32] and docked two models for IscU, the NMR structure of apo-IscU
(2L4X),[33] and the NMR structure of Zn2+:IscU
(1Q48).[34] Both yielded similar good fits with values of
0.9 and 0.6, respectively, and
each had a value of 1.1. The apo-IscU–IscS
complex showed excellent agreement between the structural model and
experimental data (Figure 2A), and the structural
model was also consistent with the ab initio shape
model (Figure 2B). The largest deviations between
the theoretical and experimental scattering curves for IscU–IscS
were at higher angles (q > 0.15 Å–1), as expected for a weak complex with incomplete saturation. We
also fit the IscU–IscS crystal structure (3LVL)[25] to the experimental SAXS data, and it showed excellent
agreement with and values of 0.8 and 1.0, respectively.
Lastly,
we explored the ability of SAXS to decipher the bound conformation
of IscU at the resolution used in our study. NMR studies from our
laboratory have shown that IscS binds preferentially to the D-state
of IscU,[13] which lacks secondary structure,[12] contains two cis-peptidyl-prolyl
peptide bonds not present in the S-state,[35] but is not fully unfolded.[36] Rigid-body
modeling simulations of IscU with varying extents of structure revealed
that the bound conformation of IscU cannot be determined reliably
by SAXS alone (Figure S4). Rather, we can
only confirm that IscU binds to IscS in at least a semicompact manner.The model generated for the IscX–IscS complex was in good
agreement with the experimental SAXS data (Figure 2) with and values of 1.0 and 1.1, respectively.
The
largest deviations between the theoretical and experimental SAXS data
were at higher angles (q > 0.15 Å–1) consistent with weak complex formation. Our molecular model is
consistent with IscX binding to the positive patch of IscS that exists
at its homodimer interface.Finally, the model generated for
the IscX–IscU–IscS
ternary complex was in good agreement with the experimental SAXS data
(Figure 2) with and values of 0.7 and 0.8, respectively.
As
with the IscX–IscS and IscU–IscS complexes, the largest
deviations between the theoretical and experimental SAXS data were
at higher angles (q > 0.15 Å–1) consistent with weak complex formation (Figure 2). Also, the molecular model obtained from rigid-body modeling
was in good agreement with the ab initio shape model.
We also carried simulations using the MES algorithm to determine if
the ternary complex model could be distinguished from a mixture of
binary complexes between IscX–IscS and IscU–IscS (Figure S5). The simulations of experimental and
synthetic data showed that the best fit was to the ternary complex
model. The binary complex model was a close second, but it can be
invalidated on the grounds that the species selected in fitting this
model failed to satisfy the law of mass action. Evidence for ternary
complex formation from our NMR and chemical cross-linking experiments
confirmed that the model that best fit the SAXS data is likely to
be true. This model defines the positions of IscX and IscU on the
IscS homodimer and excludes direct interaction between IscX and IscU
in the ternary complex.
IscX interacts with IscU
Although
an interaction between
IscX and IscU was reported a decade ago on the basis of an affinity
chromatography assay,[18] this complex has
not been characterized further. We have used NMR spectroscopy to confirm
this interaction and to identify residues in the interaction surface
(Figure 4). The addition of unlabeled IscU
led to broadening of cross peaks in the 1H-15N HSQC spectrum of [U-15N]-IscX assigned to K25, R28,
D31–H33, W35, Q47, S49, N50, I53, E55, L59, and L62 (colored
red in Figure 5AB). Another set of backbone 1HN-15NH peaks from [U-15N]-IscX exhibited significant shifts (ΔδNH > 0.04 ppm); these were assigned to I11, E13, D17, A18,
D21, D23, T26, Q34, D38, A48, K52, L54, I57, L58, E64, and A65 (colored
blue in Figure 5B). Similarly, the addition
of unlabeled IscX led to broadening of cross peaks in the 1H-15N HSQC spectrum of [U-15N]-IscU assigned
to R15, V32–A34, L43, Q44, K59, A94, E96, V102–I104,
C106–I108, and A110–I114 (colored red in Figure 5CD). An additional set of peaks from [U-15N]-IscU exhibited significant shifts (ΔδNH > 0.04 ppm); these were assigned to N16, G18, E25, S29–M31,
E54, A56–F58, T74, K80, A85–A87, N90, T91, L97, and
D120 (colored blue in Figure 5D). Notably,
only the signals from the S-state of IscU were perturbed by the titration
with IscX, indicating that this interaction involves the more structured
state of IscU. Consistent with preferential binding to the S-state,
the addition of a 2-fold excess of IscX led to a 15% increase in %S
= [S]/([S] + [D]) as determined from the relative intensities of the 1H-15N peaks from K128 assigned to the two states.[12]
Figure 4
NMR evidence for the interaction between IscX and IscU.
(A) 2D 15N-TROSY-HSQC spectrum of [U-15N]-IscX
alone (red)
overlaid with the spectrum of [U-15N]-IscX following the
addition of 4 equiv of unlabeled IscU (blue). (B) 2D 15N-TROSY-HSQC spectrum of [U-15N]-IscU alone (red) overlaid
with the spectrum of [U-15N]-IscU following the addition
of 4 equiv of unlabeled IscX (blue). The sets of peaks from [U-15N]-IscX and [U-15N]-IscU that broadened considerably
upon addition, respectively, of unlabeled IscU and IscX likely correspond
to residues in the contact regions.
Figure 5
NMR evidence for the surfaces by which IscX and IscU interact.
(A) Perturbation of the 15NH-1HN signals (ΔδNH) of [U-15N]-IscX, resulting from the addition of 4 equiv of IscU. Red triangles
denote residues whose chemical shift changes could not be followed
because of severe line broadening. (B) Results from panel A mapped
onto the structure of IscX (PDB 2BZT)[17] with the
following color code: gray, not affected; blue, significantly shifted
(ΔδNH > 0.04 ppm); red, broadened; black,
not
assigned or overlapped. (C) Perturbation of the 15NH-1HN signals of [U-15N]-IscU
resulting from the addition of 4 equiv IscX. Red triangles denote
residues whose chemical shift changes could not be followed because
of severe line broadening. (D) Results from panel C mapped onto the
structure of IscU (PDB 2L4X)[33] with the same color
code used for panel B.
NMR evidence for the interaction between IscX and IscU.
(A) 2D 15N-TROSY-HSQC spectrum of [U-15N]-IscX
alone (red)
overlaid with the spectrum of [U-15N]-IscX following the
addition of 4 equiv of unlabeled IscU (blue). (B) 2D 15N-TROSY-HSQC spectrum of [U-15N]-IscU alone (red) overlaid
with the spectrum of [U-15N]-IscU following the addition
of 4 equiv of unlabeled IscX (blue). The sets of peaks from [U-15N]-IscX and [U-15N]-IscU that broadened considerably
upon addition, respectively, of unlabeled IscU and IscX likely correspond
to residues in the contact regions.NMR evidence for the surfaces by which IscX and IscU interact.
(A) Perturbation of the 15NH-1HN signals (ΔδNH) of [U-15N]-IscX, resulting from the addition of 4 equiv of IscU. Red triangles
denote residues whose chemical shift changes could not be followed
because of severe line broadening. (B) Results from panel A mapped
onto the structure of IscX (PDB 2BZT)[17] with the
following color code: gray, not affected; blue, significantly shifted
(ΔδNH > 0.04 ppm); red, broadened; black,
not
assigned or overlapped. (C) Perturbation of the 15NH-1HN signals of [U-15N]-IscU
resulting from the addition of 4 equiv IscX. Red triangles denote
residues whose chemical shift changes could not be followed because
of severe line broadening. (D) Results from panel C mapped onto the
structure of IscU (PDB 2L4X)[33] with the same color
code used for panel B.An earlier NMR study reported that IscX binds both Fe2+ and Fe3+.[17] NMR spectral
changes
upon anaerobic titration of [U-15N]-IscX with ferrous ammonium
sulfate (Figures 6 and S6) confirmed formation of an IscX–Fe2+ complex.
However, the analogous experiment with a 3-fold excess of added ferric
ammonium citrate failed to show an interaction (Figures 6 and S6). The subsequent anaerobic
addition of DTT to the sample containing IscX and excess Fe3+ produced the spectral signature of IscX–Fe2+ (Figure S6). The earlier experiment added Fe3+ in the form of ferrous chloride;[17] thus the discrepancy appears to result from the inability of IscX
to compete with citrate for Fe3+.
Figure 6
NMR signal perturbation
of [U-15N]-IscX upon adding
3-fold Fe3+ as ferric ammonium citrate (blue) or upon adding
3-fold Fe2+ as ferrous ammonium sulfate (purple). Residues
from IscX, whose signals are broadened beyond detection by the addition
of Fe2+ (L3, K4, L39, and E66) are marked with red triangles;
upon the addition of Fe3+, the signals from these residues
were neither broadened nor shifted.
NMR signal perturbation
of [U-15N]-IscX upon adding
3-fold Fe3+ as ferric ammonium citrate (blue) or upon adding
3-fold Fe2+ as ferrous ammonium sulfate (purple). Residues
from IscX, whose signals are broadened beyond detection by the addition
of Fe2+ (L3, K4, L39, and E66) are marked with red triangles;
upon the addition of Fe3+, the signals from these residues
were neither broadened nor shifted.We next investigated whether the IscU–IscX interaction
occurs
in the presence of Fe2+ added as ferrous ammonium sulfate.
The anaerobic addition of IscU along with Fe2+ to [U-15N]-IscX resulted in many changes to its 1HN-15NH signals. The interaction led to
a new set of signals indicating a slow process on the time scale of
NMR chemical shifts (Figure 7). Several signals
from IscX, however, were not perturbed; these were found to correspond
to residues (T6–S8, E10, G12, L15, and E40–D43) not
involved in interaction with IscU in the absence of Fe2+. The 2D 15N-TROSY-HSQC spectrum of [U-15N]-IscX
mixed with 3-fold Fe2+ and 3-fold IscU (blue, Figure 7) clearly differs from those of apo-IscX (Figure 1A), Fe2+–IscX (red, Figure 7), or IscX–IscU (blue, Figure 4A). These results appear consistent with a model in which
Fe2+ stabilizes the IscU–IscX complex but does not
change its interaction site.
Figure 7
2D 15N- HSQC spectrum of [U-15N]-IscX in
the presence of 3 equiv of ferrous ion (red) overlaid with the 2D 15N-TROSY-HSQC spectrum of [U-15N]-IscX in the presence
of 3 equiv of ferrous ion following the addition of 3 equiv of unlabeled
IscU (blue). Note that the blue spectrum is different from those of
[U-15N]-IscX alone (Figure 4A, red),
Fe2+:[U-15N]-IscX (Figure
S6D, purple), or [U-15N]-IscX–IscU (Figure 4A, blue).
2D 15N- HSQC spectrum of [U-15N]-IscX in
the presence of 3 equiv of ferrous ion (red) overlaid with the 2D 15N-TROSY-HSQC spectrum of [U-15N]-IscX in the presence
of 3 equiv of ferrous ion following the addition of 3 equiv of unlabeled
IscU (blue). Note that the blue spectrum is different from those of
[U-15N]-IscX alone (Figure 4A, red),
Fe2+:[U-15N]-IscX (Figure
S6D, purple), or [U-15N]-IscX–IscU (Figure 4A, blue).Although Fe2+ strengthens the IscU–IscX
interaction,
it does not appear to strengthen the interaction between IscX and
IscS. The addition of unlabeled IscS to [U-15N]-IscX led
to similar line broadening effects in the presence or absence of Fe2+ (data not shown).
IscX Suppresses Sulfide Production of IscS
in the Presence of
IscU
Given the various interactions between the cysteine
desulfurase (IscS) and other proteins, it was of interest to determine
their effects on its enzymatic activity. We monitored sulfide production
in the presence of a catalytic amount of IscS without and with comparable
or excess amounts of IscU, IscX, or CyaY. All of the reaction mixtures
contained excess ferrous ion, l-cysteine, and DTT to mimic
the conditions of the in vitro Fe–S cluster
assembly reaction. We observed that neither IscX nor CyaY by itself
altered the amount of sulfide produced by IscS (Figure 8). By contrast, IscU in 50-fold excess decreased sulfide production
by a factor of 2: sulfide production of IscS by itself was 44 μM
(±1 μM) after 20 min incubation, and IscU decreased it
to 19 μM (±2.7 μM). The subsequent addition of a
50-fold excess of IscX suppressed it further by an additional factor
of 2; sulfide production under these conditions was 9 μM (±0.1
μM). In comparison, the sulfide production was restored to some
extent by adding 50-fold CyaY to the sample containing 50-fold IscU.
The inhibitory effect of IscX in the presence of IscU has not been
reported previously, but the other observations are consistent with
reports that IscU decreases desulfurase activity of IscS, whereas
CyaY restores this activity,[39] and that
CyaY displaces IscU from IscS.[7]
Figure 8
Sulfide production
of reaction mixtures containing 5 mM DTT, 125
μM l-cysteine, and 125 μM ferrous ammonium sulfate
plus the protein(s) designated below the x-axis.
Sulfide was measured after incubating each mixture for 20 min at ambient
temperature.
Sulfide production
of reaction mixtures containing 5 mM DTT, 125
μM l-cysteine, and 125 μM ferrous ammonium sulfate
plus the protein(s) designated below the x-axis.
Sulfide was measured after incubating each mixture for 20 min at ambient
temperature.
We also tested whether IscX
perturbs in vitro Fe–S
cluster assembly on IscU in the presence of catalytic amount of IscS,
excess iron, l-cysteine, and DTT, as monitored by the absorbance
at 456 nm (Figure 9) or by following full UV–vis
spectra (from 900 to 300 nm; Figure S7).[13,37] We found that the addition of catalytic (red, Figures 9 and S7) or stoichiometric (blue,
Figures 9 and S7) amounts of IscX repressed Fe–S cluster assembly compared
to the control (black, Figures 9 and S7). Thus, the IscX-mediated inhibition of cysteine
desulfurase activity in the presence of IscU translates into compromised
cluster assembly. As expected,[14,39] the addition of CyaY
to the reaction mixture further slowed Fe–S cluster assembly
(green; Figures 9 and S7). Repression of Fe–S cluster assembly in this case can be
explained by the competition between CyaY and IscU for binding to
IscS.[7]
Figure 9
IscX and CyaY suppress iron–sulfur
cluster assembly. Iron–sulfur
cluster assembly on IscU was monitored by following absorbance at
456 nm. All reaction mixtures contained 0.5 μM IscS, 25 μM
IscU, 5 mM DTT, 125 μM l-cysteine, and 125 μM
ferrous ammonium sulfate: reaction mixture alone (black); reaction
mixture with added 1.5 μM IscX (red); reaction mixture with
added 25 μM IscX (blue); reaction mixture with added 25 μM
CyaY (green). The entire UV–vis spectrum for each reaction
is shown as a function of time in Figure S7.
IscX and CyaY suppress iron–sulfur
cluster assembly. Iron–sulfur
cluster assembly on IscU was monitored by following absorbance at
456 nm. All reaction mixtures contained 0.5 μM IscS, 25 μM
IscU, 5 mM DTT, 125 μM l-cysteine, and 125 μM
ferrous ammonium sulfate: reaction mixture alone (black); reaction
mixture with added 1.5 μM IscX (red); reaction mixture with
added 25 μM IscX (blue); reaction mixture with added 25 μM
CyaY (green). The entire UV–vis spectrum for each reaction
is shown as a function of time in Figure S7.
Discussion
The
addition of ferrous ammonium sulfate to [U-15N]-IscX
caused the broadening beyond detection of backbone 1H-15N signals from 4 residues (L3, K4, L39, and E66) and large
chemical shifts (ΔδNH > 0.1 ppm) for signals
from 11 residues (Figure 6). Because the shifted
peaks are sharp (Figure S6), we attribute
them to conformational changes that accompany binding of Fe2+ rather than hyperfine interactions. By contrast, the addition of
excess ferric ammonium citrate had no effect on signals assigned to
L3, K4, L39, and E66 and led to no chemical shifts with ΔδNH > 0.1 ppm (Figure 6). Thus, IscX
fails to compete with citrate for binding of Fe3+, and
we attribute the slight perturbations observed to nonspecific binding.We have shown here that IscX interacts directly with the S-state
of IscU (Figures 4 and 5) and that this interaction is stabilized by Fe2+ (Figure 7). We confirmed our previous studies[7] showing that IscX forms a binary complex with IscS, which
is displaced by ferredoxin (Fdx) or bacterial frataxin (CyaY), but
not by IscU (Figure 1). We provide evidence
here for an IscX–IscU–IscS ternary complex (Figure 2). Notably, IscX was found to inhibit the cysteine
desulfurase activity of IscS in the ternary complex but not in the
IscX–IscS binary complex (Figure 8).
The inhibitory effect of IscX also manifests itself as a decrease
in the rate of cluster assembly on IscU in an in vitro Fe–S cluster assembly reaction (Figure 9). CyaY is another inhibitor of cluster assembly, but it appears
to operate by a different mechanism in that CyaY displaces IscU[7] and thereby leads to stimulation of the cysteine
desulfurase activity of IscS.[39] Because
bacterial frataxin (CyaY) inhibits Fe–S cluster biosynthesis
but not cysteine desulfurase activity, its physiological role in bacteria
may conceivably be to redirect sulfur trafficking from Fe–S
cluster biosynthesis to other sulfur-requiring mechanisms. IscS has
been shown to be essential for various other sulfur-related mechanisms.[38]The challenge is to come up with a mechanism
for Fe–S cluster
assembly that is consistent with these and previous observations.
We propose a speculative mechanism (Figure 10) that can be subject to future testing. A major stumbling block
is the unknown nature of the irondonor; on the basis of our current
findings, we assume that it is, in fact, IscX. Because we found that
ferredoxin (Fdx) displaces both IscU and IscX,[7] the first step in Fe–S cluster biosynthesis would appear
to be the binding of reduced Fdx (Fdxred) to IscS, which
would displace any bound IscX and remove inhibition of the cysteine
desulfurase reaction that converts Cys to Ala to produce S0, which is bound to C328 of IscS. Reaction between Fdxred and −S–S0 would lead to Fdxox and −S–S. Binding of IscU would displace Fdxox, and attack by
one of the Cyssulfhydryl groups of IscU on C328 would lead to transfer
of the S to IscU. IscS binds
preferentially to the D-state of IscU, the form of IscU that fails
to bind to metal ions and thus has free cysteinesulfhydryl groups.[13] Following sulfur transfer, IscX:Fe2+ is attracted to IscU:S to initiate the oxidation of Fe2+ to Fe3+ the
reduction of S to S2–, and the transfer of iron to IscU. Such a reaction
is consistent with our finding that Fe2+ binds to IscX
and strengthens its interaction with IscU, whereas Fe3+ does not interact with IscX. Also, the presence of the −S–S on one of the cysteine side
chains of IscU is expected to facilitate iron transfer. The interaction
with IscX may stabilize the S-state of IscU, which is the state that
binds metals and Fe–S clusters. We envision that the −S–S2– group binds Fe3+ as an intermediate in
cluster assembly. The NMR results presented here demonstrate that
the residues of IscU that interact with IscX are different from those
in the IscU–IscS interface.[25] We
postulate, thus, that IscX interacts at the face of IscU that is not
contacting IscS and that the binding site for IscX on IscS is too
far away to be involved in this interaction as determined from the
SAXS-based model (Figure 2C). Ligation of the
iron by two of the three Cys residues, D39, and H105 would leave the
side chain of the third cysteine residue free. After its release of
iron, IscX could move to its binding site on IscS leading to inhibition
of desulfurase activity. The second cycle would then be initiated
by the binding of Fdxred to IscS, with displacement of
both IscX and IscU with its nascent cluster. Release of IscX would
reactivate cysteine desulfurase activity and lead to a second conversion
of Cys to Ala with the production of S0, which is bound
to C328 of IscS and reduced to S by conversion of Fdxred to Fdox. Next,
IscU:S2–:Fe3+ binds to IscS, displacing
Fdxox. Attack by a free cysteine of the scaffold protein
on C328–S–S leads to the production of IscU:S2–:Fe3+:S. Subsequent interaction
with IscX:Fe2+ would lead to the reduction of S and the transfer of Fe3+ to
IscU followed by assembly of the 2Fe–2S cluster. The released
IscX would could then bind to IscS and inhibit the desulfurase reaction
until IscU[2Fe–2S] is carried away by HscB. The above mechanism
employs only proteins encoded by the isc operon.
Figure 10
Proposed
mechanism for the ISC Fe–S cluster assembly that
is mediated by IscX as an iron supplier and as a regulator of cysteine
desulfurase (IscS). The species S is bound to the sulfur of a cysteine residue of either IscS
or IscU as indicated, and S2–:Fe3+ is
bound to a cysteine residue of IscU as Cys–S–Fe–S.
See the text for details of each step.
Proposed
mechanism for the ISC Fe–S cluster assembly that
is mediated by IscX as an iron supplier and as a regulator of cysteine
desulfurase (IscS). The species S is bound to the sulfur of a cysteine residue of either IscS
or IscU as indicated, and S2–:Fe3+ is
bound to a cysteine residue of IscU as Cys–S–Fe–S.
See the text for details of each step.Eukaryotes do not have an IscX homologue. It appears that
frataxin,
which has been shown to be essential to Fe–S cluster biosynthesis,
evolved to take the place of IscX.[17] The
mechanism of eukaryotic Fe–S cluster assembly also differs
from the bacterial mechanism in that frataxin increases the activity
of the eukaryotic cysteine desulfurase (Nfs1).[37]
Authors: Filippo Prischi; Petr V Konarev; Clara Iannuzzi; Chiara Pastore; Salvatore Adinolfi; Stephen R Martin; Dmitri I Svergun; Annalisa Pastore Journal: Nat Commun Date: 2010-10-19 Impact factor: 14.919
Authors: Dulmini P Barupala; Stephen P Dzul; Pamela Jo Riggs-Gelasco; Timothy L Stemmler Journal: Arch Biochem Biophys Date: 2016-01-16 Impact factor: 4.013
Authors: Jameson R Bothe; Marco Tonelli; Ibrahim K Ali; Ziqi Dai; Ronnie O Frederick; William M Westler; John L Markley Journal: Biophys J Date: 2015-09-01 Impact factor: 4.033