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Journal of Bacteriology, June 2004, p . 3903-3910, Vol . 186,
No . 12
Structural Basis for Iron Binding and Release by a Novel Class of Periplasmic
Iron-Binding Proteins Found in Gram-Negative Pathogens
Stephen R . Shouldice,1 Robert J . Skene,2
Douglas R . Dougan,2 Gyorgy Snell,2 Duncan E . McRee,3
Anthony B . Schryvers,1* and Leslie W . Tari3*
Department of Microbiology and Infectious Diseases, University of Calgary,
Calgary, Alberta, Canada T2N 4N1,1 Syrrx Inc.,2
ActiveSight, San Diego, California 921213
Received 8 January 2004/ Accepted 2 March 2004
We have determined the 1.35- and 1.45-Å structures, respectively, of
closed and open iron-loaded forms of Mannheimia haemolytica
ferric ion-binding protein A . M . haemolytica is the causative
agent in the economically important and fatal disease of cattle
termed shipping fever . The periplasmic iron-binding protein of this
gram-negative bacterium, which has homologous counterparts in many
other pathogenic species, performs a key role in iron acquisition
from mammalian host serum iron transport proteins and is essential
for the survival of the pathogen within the host . The ferric (Fe3+)
ion in the closed structure is bound by a novel asymmetric
constellation of four ligands, including a synergistic carbonate
anion . The open structure is ligated by three tyrosyl residues and a
dynamically disordered solvent-exposed anion . Our results clearly
implicate the synergistic anion as the primary mediator of global
protein conformation and provide detailed insights into the molecular
mechanisms of iron binding and release in the periplasm .
Iron is an essential nutrient for almost all living bacteria (7) .
By changing the coordinating ligands and protein environment around
iron, its redox potential can be made to vary between –300 and +700
mV, making it uniquely suited to participate in a wide range of
electron transfer reactions involved in intermediary metabolism (3) .
For example, iron is a key component of a number of essential
metabolic enzymes, including the cytochromes and ribonucleotide
reductase . Consequently, iron is essential for the virulence of many
bacterial pathogens (5, 12) . Although
it is the fourth most abundant element in the earth's crust,
iron is inaccessible as a component of insoluble hydroxides in the
environment . In mammals, iron is also inaccessible to pathogens
because it is sequestered by high-affinity iron-binding proteins
(transferrins [Tf], lactoferrins [Lf], ferritin, hemoglobin, and
hemopexin) . Therefore, pathogenic bacteria have been forced to evolve
elaborate strategies to engage in a tug-of-war with the mammalian
host for this precious metal .
Mannheimia haemolytica (previously known as Pasteurella haemolytica)
is a gram-negative coccobacillus that is an opportunistic pathogen
of cattle, sheep, and other ruminants (28) . It causes a
life-threatening hemorrhagic pneumonia, termed shipping fever or
pneumonic pasteurellosis, in cattle that is responsible for the
deaths of at least 1% of North American feedlot cattle . In order to
survive in the iron-limited environment present in the host, M.
haemolytica and other pathogenic gram-negative bacteria from
the Pasteurellaceae and Neisseriaceae families have
developed high-affinity iron acquisition systems in which iron
transport into the bacterial cell is initiated by outer membrane
proteins specific for the Tf and Lf (14,
22, 24, 25) . The
heterodimeric Tf bacterial outer membrane receptor is composed of two
proteins, Tf binding protein A (TbpA) and the extrinsic lipoprotein
TbpB . Upon binding the host protein, the ferric ion is removed by the
receptor proteins and transported through the TonB-dependent integral
membrane protein TbpA . TbpA is proposed to form a ß-barrel
and function as a gated porin requiring the presence of a functional
TonB protein for the translocation of iron into the periplasmic space
(6) .
After crossing the outer membrane, the iron is transported into
the cell by an ATP binding cassette (ABC) pathway specific for iron .
Within the periplasm, the ferric ion is complexed by ferric
ion-binding protein A (FbpA) (9, 18) . FbpA
shuttles the iron to an inner membrane complex consisting of two
proteins, the inner transmembrane FbpB and the cytoplasmic ATPase
FbpC . The energy for the transport of iron across the inner membrane
is provided by the hydrolysis of ATP by the inner membrane-associated
proteins . Pathways analogous to the one described above are
also utilized in gram-negative bacteria for the uptake of iron from
siderophores and heme, as well as for the import of amino acids,
sugars, and other nutrients (10, 19) .
Several outer membrane and periplasmic protein components of
different ABC transport pathways responsible for iron uptake have
been well characterized biochemically and structurally (10,
19) . However, there is still considerable debate surrounding
the detailed molecular mechanisms of iron translocation across
the outer membrane and the mechanics of iron acquisition and release
by the periplasmic iron-binding proteins .
Recently, we were able to determine the 1.2-Å iron-free and
formate-bound structure of M . haemolytica FbpA (MhFpbA)
(apo-MhFbpA) (27), revealing a new class of periplasmic
iron-binding proteins . In the same study, we were able to assign
putative iron- and anion-binding residues and identified 21 bacterial
homologs with apparently identical machinery for binding ferric
ions and synergistic anions . To understand how MhFbpA binds a ferric
ion, we sought to determine the crystal structure of the iron-loaded
form of the protein . Here, we present two high-resolution structures
of MhFbpA complexed with iron (MhFbpAFe) and iron-carbonate
(MhFbpAFeCO3) . The mode of ferric ion binding is novel and
unexpected . Our results also reveal that MhFbpA is able to bind a
single iron atom while the protein is in an open conformation and in
the absence of a discretely bound synergistic anion, which is a
highly unusual observation for characterized ferric ion transport
proteins . The synergistic anion appears to play a key role in
inducing large-scale global conformational changes in the protein .
Our present results, analyzed in combination with the structure of
apo-MhFbpA, allow us to propose models detailing the molecular
mechanisms of iron uptake and release for this iron-binding protein
class in the periplasm of gram-negative bacteria .
Crystallization. MhFbpA was expressed in Escherichia coli
and purified as described previously (27) . All
protein samples were concentrated to 30 mg/ml in 10 mM Tris buffer
(pH 7.5) with 10 mM sodium bicarbonate . The two crystal forms of the
iron-loaded MhFbpA were grown by vapor diffusion by the hanging drop
method . The new MhFbpA samples were initially screened around the
crystallization conditions that had previously been determined for
the apo-MhFbpA structure (15) . Since these
conditions had proved successful for the same protein, they served as
a starting point in attempts to obtain an iron-loaded crystal form .
Crystals of the closed holoprotein (MhFbpAFeCO3) were
grown at 4°C by the hanging drop technique with 4-µl drops containing
15 mg of the FbpA/ml, 0.05 M HEPES (pH 7.5), 4.25% isopropanol, 8.5%
polyethylene glycol (PEG) 4000, and 7.5% glycerol . The drops were
equilibrated against a 1-ml reservoir containing 0.1 M HEPES (pH
7.5), 8.5% isopropanol, 17% PEG 4000, and 15% glycerol .
Diffraction-quality orange crystals typically appeared within 1 week
in these crystallization experiments and belonged to the orthorhombic
space group C2221 . Similarly, crystals of the open
iron-loaded form (MhFbpAFe) were grown with hanging drops (4 µl) at
4°C . These drops contained 15 mg of the FbpA/ml, 11% PEG 3350, and
0.1 M citrate (pH 8.2) . These drops were also equilibrated against a
1-ml reservoir containing 22% PEG 3350 and 0.2 M citrate (pH 8.2) .
Diffraction-quality orange crystals belonging to the monoclinic space
group P21 appeared within 4 to 5 days in these
crystallization experiments .
Crystal harvesting and data collection. The crystals were
harvested by scooping them with a nylon loop . Because the closed
iron-loaded crystals were grown in a cocktail that already contained
15% glycerol in the reservoir, no further addition of cryoprotectant
was made prior to cooling the crystals in liquid nitrogen . However,
for the open iron-loaded form, the crystals were dipped into a
cryoprotectant solution containing 30% (vol/vol) ethylene glycol, 22%
PEG 3350, and 0.2 M citrate (pH 8.2) for
30
s before they were cooled in liquid nitrogen . All X-ray data sets
were collected for single crystals at 100 K by using cryomounting
procedures . The crystals were maintained at 100 K during data
collection by use of a nitrogen gas stream . Diffraction data for both
forms of MhFbpA crystals were collected by using a QUANTUM4 ADSC
detector on Beamline 5.03 at the ALS Berkeley Laboratory, Berkeley,
Calif., with a wavelength of 1.0 Å . The data for all experiments were
reduced and scaled by using the HKL2000 suite (23) .
The individual data-processing statistics for the MhFbpA crystals are
reported in Table 1 .
| TABLE 1 . X-ray data collection and refinement statistics
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Structure solution and refinement. In order to determine the
structures of the MhFbpA by molecular replacement, the coordinates of
the 1.2-Å wild-type apo-MhFbpA (Protein Data Bank code 1Q35) were
used as the search model . The formate anions and all of the water
molecules were removed from the model . Since the structure of
apo-MhFbpA was in a closed conformation compared with the open
iron-loaded form found here, two independent search models comprising
the N- and C-terminal domains of the protein had to be positioned
independently to solve that structure . For both structures, the
program MolRep from the CCP4 suite of programs was used to perform
the molecular replacement (11) . Iterative cycles
of manual refitting of the models with the program XtalView/Xfit (20)
made use of maps created with ARP/wARP 5.2 (21),
and refinement with Refmac5 (29) was carried out
to complete and correct the models . Restrained refinement with a
maximum-likelihood target function and isotropic temperature factors
was carried out . During the later stages of refinement, difference
maps (|Fo| – |Fc| maps) were utilized to place
the bound ethylene glycol, carbonate, ferric ion, and water molecules
when required .
Structure analysis. The refined coordinates of MhFbpA in
complex with iron-carbonate and iron alone have been deposited in the
Protein Data Bank (codes 1SI0 and 1SI1) . Ramachandran plots of the
two structures reveal the satisfactory location of all residues in
allowed regions of conformational space . The DALI server was used to
find structurally similar proteins in the fold classification
based on structure-structure alignment in the Proteins database (16) .
Overview of MhFbpA structure. All structurally characterized
bacterial periplasmic ligand-binding proteins to date adopt two basic
protein folds despite low sequence homology within the protein class
(10) . MhFbpA belongs to the transferrin
superfamily, adopting the more common of the two periplasmic binding
protein folds (Fig . 1) . The MhFbpA fold has also
been observed in the periplasmic ferric ion-binding proteins from
Neisseria (NgFbpA) (1) and Haemophilus (HiFbpA)
(8) . MhFbpA possesses two asymmetric globular
/ß
domains connected by a pair of antiparallel ß-strands . The
Fe3+ ion-binding site resides at the bottom of a deep cleft
between the two globular domains . The domain-spanning ß-strands
also reside at the base of the iron binding cleft, acting as flexible
hinges that allow the two domains to rotate with respect to one
another . The interdomain rotations generally correspond with the
opening and closing of the binding cleft in response to the presence
of bound ligand in a Venus flytrap-like manner .
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FIG . 1 . Stereo ribbon diagram of MhFbpA structure . MhFbpA possesses two
/ß
domains linked by a ß-strand hinge.
-Helices
are shown in purple, and ß-strands are shown in cyan . The relative
positions of the iron (orange sphere), carbonate, and iron-binding
residues are shown.
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At the topological level, MhFbpA is similar to HiFbpA and NgFbpA . The
-carbon
atoms of MhFbpAFeCO3 superimpose on the
-carbons
of the iron-loaded forms of HiFbpA and NgFbpA with root mean
square deviations of approximately 2.3 Å . As members of the
transferrin superfamily of folds, MhFbpA, HiFbpA, and NgFbpA also
share a lesser but significant degree of structural and topological
similarity with the N and C lobes of human Tf, which has led to the
adoption of the moniker "bacterial transferrins" for HiFbpA and
NgFbpA (13) . However, while MhFpbA shares a similar
overall fold with the other iron-chelating members of the transferrin
superfamily, it differs from the other superfamily members in
its iron coordination scheme and anion-binding mode . MhFbpA is also
unique among the other characterized ferric ion transport proteins in
that its global protein conformation appears to be mediated primarily
by the anion, not the ferric ion .
Ferric ion coordination. Although the global protein
conformations of the MhFbpAFe and MhFbpAFeCO3 structures
are dramatically different, both utilize the same protein residues in
ferric ion binding . In both structures, the ferric ion is coordinated
by three tyrosines, Tyr142, Tyr198, and Tyr199, from the C-terminal
domain in nearly identical constellations (Fig . 2) .
The three tyrosinate anions act to neutralize the +3 charge on the
ferric ion . The tyrosine hydroxyls form a distorted trigonal plane on
the side of the ferric ion facing the C-terminal domain,
approximately parallel to the C-terminal face of the binding cleft .
In the MhFbpAFeCO3 structure, a carbonate anion is
positioned on the opposite side of the ferric ion, where it
coordinates the ferric ion in a bidentate fashion with the plane of
the carbonate lying perpendicular to the plane described by the
tyrosine hydroxyl groups . Bidentate coordination of iron by a
carbonate anion is also observed in Lf and Tf (4) .
Collectively, the three tyrosyl residues and the carbonate anion
surround the ferric ion in an asymmetric manner, suggesting that the
interaction between the ferric ion and the protein is predominantly
electrostatic in nature .
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FIG . 2 . Stereoviews of the iron-binding site of MhFbpA . (A) Electron
density maps of the iron-loaded closed form (green for the 2Fo-Fc
map contoured at 1 ,
magenta for the Fo-Fc map contoured at 5
obtained with the reflection data after refinement of the model in which
the carbonate molecule was omitted, and red for the Fo-Fc
map contoured at 5
obtained with the reflection data after refinement of the model in which
the iron atom [orange sphere] was omitted) . (B) Potential hydrogen
bonding interactions are shown as green dotted lines . The iron ligand
residues are shown with red bonds to the iron atom . (C) Electron density
maps of the iron-loaded open form (green for the 2Fo-Fc
map contoured at 1 ,
blue for the Fo-Fc map contoured at 3 ,
and red for the Fo-Fc map contoured at 5
obtained with the reflection data after refinement of the model in which
the iron atom was omitted) . (D) Potential hydrogen bonding interactions
are shown as green dotted lines . The iron ligand residues are shown with
red bonds to the iron atom.
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In the MhFbpAFe structure, the N- and C-terminal domains are rotated
away from one another, moving the carbonate binding site away from
the ferric ion and exposing one side of the ferric ion to solvent .
Despite the opening of the binding cleft, the ferric ion remains
coordinated by Tyr142, Tyr198, and Tyr199 . On the solvent-exposed
side of the ferric ion, we observed moderately strong (>3 ),
continuous difference electron density within coordination distance
of the iron, which extends towards the N-terminal domain and a
carbonate binding Arg10 residue . However, since the density was too
indistinct to reliably fit water molecules or organic ions, it was
left unassigned . Since the crystals of MhFbpAFe were grown in the
presence of high concentrations of citrate (see Materials and
Methods), we postulate that the difference electron density around
the iron arises from dynamically and/or statically disordered
citrate . The distances between the ferric ion coordinating tyrosine
hydroxyl groups in both structures and the ferric ion (all
metal-ligand distances were not restrained during refinement) were
identical within the experimental error, averaging 1.97 Å . At 1.97 Å,
the tyrosyl-iron coordination distances observed in the title
structures fall into the range that is typically observed in
structurally characterized iron transport proteins, including Lf (2),
Tf (15), HiFbpA (8), and NgFbpA (1) .
However, MhFbpA differs from other characterized human and bacterial
ferric ion transport proteins in a number of key aspects (Fig.
2 and 3) . MhFbpA utilizes only
three protein residues, instead of four, to coordinate iron and, with
the inclusion of the anion, coordinates iron exclusively with oxygen
atoms in the inner coordination sphere . MhFbpA is the only
characterized ferric transport protein to utilize three tyrosine
residues in iron coordination and ferric ion charge neutralization
(all others utilize two tyrosines and an aspartate or glutamate to
achieve the same end) . MhFbpA utilizes only five coordinating
moieties, which are disposed in an asymmetric fashion around the
metal atom, to ligate iron, while all other superfamily members
coordinate iron with a total of six ligands and an octahedral
coordination sphere . Finally, we have observed that MhFbpA is able to
ligate iron without an ordered, protein-bound synergistic anion .
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FIG . 3 . Coordination of ferric ion . The geometry for the coordination of
a ferric ion in MhFbpA (A), Tf (B), and HiFbpA or NgFbpA (C) is
illustrated.
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A comparison of the UV-visible absorption properties of MhFbpA (17)
to those of Tf and NgFbpA (13) also serves to highlight
its uniqueness . Iron-loaded MhFbpA possesses a peak visible
absorbance at 419 nm, which is significantly blue shifted compared to
the same parameter from Tf and HiFbpA ( 480
nm) (13) . Since the effects of anions on peak
visible absorbance maxima are small (on the order of 5 to 10 nm) (13),
the 61-nm blue shift in the visible absorbance maximum is most likely
caused by the coordination of the ferric ion by an additional
tyrosine .
The role of carbonate in mediating protein conformation. As
shown in Fig . 2 and 4, carbonate plays an
important role in iron binding and global protein conformation in
MhFbpA . The carbonate anion binds in a basic pocket in the N-terminal
domain and has its charge compensated for by a pair of arginine
residues (Arg10 and Arg101) . In a classic example of molecular
recognition, the full hydrogen bonding potential of the carbonate is
utilized through main chain and side chain hydrogen bonding
interactions with Gln11 as well as hydrogen bonding interactions with
Arg10 and Arg101 . The two carbonate oxygens that coordinate iron do
so in a slightly asymmetric manner, with coordination distances
of 2.10 and 2.20 Å, respectively . The asymmetry is likely due to a
partial preference for a carbonate resonance form which places a
greater partial negative charge on the carbonate oxygen positioned
near the bottom of the binding cleft . The oxygen has the largest
number of close contacts with positively charged groups, as it
simultaneously interacts with Arg10, Arg101, and the Fe3+
ion .
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FIG . 4 . Conversion from the closed to the open form of MhFbpA . (A) C
traces comparing the iron-loaded closed and iron-loaded open forms of
the protein . The N-terminal (green) and C-terminal (blue) domains are
colored differently to clarify visualization of the domain movements .
The domain reorganization can be characterized by two hinge-bending
movements: a 25° opening of the N and C lobes through an axis parallel
to the ligand-binding cleft, and a 15° rotation through a perpendicular
axis through Gly285 . The iron atom (yellow sphere) and the carbonate
anion are also shown . (B) Comparison of iron-apo-formate and
holo-carbonate structures . H bonds are shown as green dotted lines .
Formate and carbonate utilize virtually identical binding modes with
respect to Arg10, Arg101, and most surrounding elements . Both structures
globally adopt closed protein conformations . However, the additional
oxygen atom from the carbonate anion faces the solvent-exposed side of
the binding pocket, twisting the Gln11 side chain around so that it H
bonds with carbonate, which in turn induces a movement in the loop
containing Asp36 so that it covers the binding pocket and sequesters the
ferric ion from solvent.
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The carbonate modulates the conformation of the protein globally by
affecting the relative orientations of the N- and C-terminal domains
and also causes more localized changes in elements of the N-terminal
domain in the vicinity of the ligand-binding site . The carbonate
promotes a closed conformation of the protein by stitching the N- and
C-terminal domains of MhFbpA together through hydrogen bonding
interactions . Arg10 and Gln11 from the N-terminal domain bridge to
the ferric ion through their direct interactions with carbonate . The
Gln11 side chain also forms bridging hydrogen bonds between the
carbonate and Tyr199, one of the ferric ion-coordinating tyrosines
(Fig . 2) .
A comparison of the carbonate-bound, carbonate-free and
iron-apo-formate-bound (27) structures of MhFbpA
reveals the exact nature of the carbonate-induced structural
transitions (Fig . 4) . Globally, the release of carbonate
is associated with individual large-scale movements of the N-
and C-terminal domains . The domain reorganization is described by
rotations about a pair of orthogonal axes near the domain interface
(Fig . 4) . In the MhFbpAFe structure, the domains rotate
away from one another compared to the MhFbpAFeCO3 structure
via a 25° hinge-bending motion through an axis described by the
-carbons
of Thr100 and Gly233, running along the base of the ligand-binding
cleft . Thr100 and Gly233 reside in the adjacent ß-strands connecting
the N- and C-terminal domains . A concomitant 15° hinge bending of the
N- and C-terminal domains around the Gly285 C
also distinguishes the MhFbpAFe structure from the MhFbpAFeCO3
structure . This second rotation is through an axis that is
approximately perpendicular to the floor of the ligand-binding cleft .
The hinge-bending around Gly285 appears to be necessary to keep
hydrophobic surfaces at the underside of the ligand-binding cleft
from separating and becoming solvent exposed while allowing the
ligand-binding cleft to open . Taken together, these rotations are
associated with the opening of the iron-binding cleft and increased
solvent exposure of the bound ferric ion . However, the domain
movements were also found to maintain a closed domain interface on
the underside of the ligand-binding cleft with an altered series
of polar and hydrophobic domain-domain interactions when the
structures of MhFbpAFeCO3 and MhFbpAFe were compared (Fig.
4) . It is important to note that the underside of
the ligand-binding cleft has a significant proportion of hydrophobic
residues on its interface but that the faces of the ligand-binding
cleft itself are almost entirely composed of polar residues . Thus,
based on the analysis presented above, there is likely a minimal
difference between the free energies of the open and closed
states of MhFbpA, so that the protein can readily adopt either state
in solution .
A comparison of the MhFbpAFeCO3 and apo-MhFbpA structures reveals
that the carbonate anion not only controls the relative orientations
of the N- and C-terminal domains but also plays a direct role
in stabilizing conformations of loops in the solvent-exposed regions
of the iron-binding pocket that sequester the ferric ion from solvent
(Fig . 4) . The apo-MhFbpA structure, while lacking a
ferric ion, was found to contain two formate (HCO2–)
anions disposed on opposite sites of the iron-binding pocket (27) .
Formate was present in high concentrations during crystallization . In
the overlaid structures of MhFbpAFeCO3 and apo-MhFbpA, the
oxygens of one of the formate anions superimpose almost exactly on
the pair of carbonate oxygens that face the bottom of the binding
pocket (Fig . 4) . These two oxygen ligands are sufficient
to promote a closed domain-domain interface without the assistance
of any other ligands or iron, since the structures of MhFbpAFeCO3
and apo-MhFbpA are virtually identical and superimpose with a
root mean square deviation of 0.6 Å . The structures differ
significantly only in the conformations of Gln11 and the neighboring
Asp36-Leu39 surface loop, which are disordered and poorly resolved in
the apo-MhFbpA structure . In the apo-MhFbpA structure, the amide
terminus of Gln11 points away from the iron-binding pocket and is
disordered . In the MhFbpAFeCO3 structure, however, the
Gln11 side chain is ordered and observed in two conformations: a
major conformation in which the side chain rotates towards the
ligated iron and interacts simultaneously with carbonate and Tyr199,
and a minor conformation in which the Gln11 side chain hydrogen-bonds
with Asp36 and stabilizes a conformation of the Asp36-Leu39 loop that
partially covers the ligand-binding cleft and decreases the exposure
of the iron-binding pocket to solvent . Formate lacks the third oxygen
atom necessary for the simultaneous coordination of the ferric ion
and tethering of Gln11 .
We have carried out a detailed analysis and comparison of three
high-resolution structural snapshots of MhFbpA in three unique
liganded states . The MhFbpAFe form represents an open conformation,
the iron-free apo-MhFbpA form represents an anion-bound closed
conformation with a solvent-exposed ferric ion-binding site, and the
MhFbpAFeCO3 form represents a fully closed conformation .
Our analysis has allowed us to characterize the precise atomic
details of ligand binding and to dissect the roles played by the
ferric ion and carbonate in mediating protein conformation . The
structural work also provides general insights into the possible
mechanisms of iron acquisition and release utilized by MhFbpA and its
homologs as part of ABC transport pathways in vivo .
It is clear from our structural analysis that the carbonate anion
acts as the trigger that switches MhFbpA between its open and closed
states . Surprisingly, we were able to observe iron ligation in both
the open and the closed forms of MhFbpA, indicating that in the
MhFbpA protein class, a specific synergistic anion may not be
essential for iron ligation . However, it is likely that the affinity
of MhFbpA for ferric ions is lower in the open state than in the
closed state . Taken together, and focusing on the periplasmic protein
component, these observations are consistent with at least two
discrete mechanisms of iron transport in pathways utilizing FbpAs in
the MhFbpA protein class to bind iron at the outer membrane and
release it at the inner membrane (Fig . 5 and
6) . A current model for iron removal from Tf and
transport across the outer membrane is depicted in Fig . 5 . The
model proposes that binding to the receptor induces conformational
changes in Tf to reduce its affinity for iron so that binding
by FbpA can drive the transport process once a channel is created by
interaction with TonB (26) . This model is supported by recent
studies with a series of HiFbpA mutants demonstrating that a
relatively high binding affinity threshold is necessary for iron
translocation (A . G . Khan, S . R . Shouldice, S . M . Kirby, R.-H . Yu,
and A . B . Schryvers, submitted for publication) . To facilitate iron
translocation across the outer membrane, it is likely that MhFbpA
docks against the outer membrane in a carbonate-bound state, which
would have maximal affinity for iron . A comparison of the MhFbpAFeCO3
and formate-bound apo-MhFbpA structures reveals that anion-bound
MhFbpA positions all of the iron-binding protein ligands within 0.5 Å
of their positions in the ferric ion-bound state . Anion-bound MhFbpA
would have a predefined high-affinity ferric ion-binding site
available to attract a ferric ion diffusing through TbpA . Accessibility
of the ferric ion-binding site to solvent is gated by the conformations
of Gln11 and the Asp36-Leu39 loop, which appear highly flexible
on the basis of our structural analysis .
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FIG . 5 . Model for the iron uptake pathway . Binding of hTf by TbpA
induces a conformational change that lowers the affinity of hTf for
iron . Interaction of TbpA with TonB provides a channel for transport
across the outer membrane . FbpA binds its synergistic anion (carbonate),
adopting a closed conformation that has a high affinity for iron . The
transport of iron across the outer membrane is driven by the
high-affinity binding of iron by FbpA . Iron release occurs by two
possible mechanisms . In path A, FbpA loses carbonate or swaps carbonate
with a different anion, adopting an open conformation which subsequently
docks to the FbpB/C inner membrane complex . In path B, carbonate removal
is mediated by FbpB . In both scenarios, iron-loaded FbpA binds to the
FbpB/C inner membrane complex and is released into the cytoplasm . Energy
for iron translocation is provided by the ATPase activity of FbpC.
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FIG . 6 . Iron removal from FbpA . In step 1, the Asp36-Leu39 loop (D36
loop) and Gln11 move to expose the carbonate anion (upside-down Y) . In
step 2, the carbonate anion is either protonated to facilitate release
or displaced by an alternate anion (citrate) . In step 3, iron is
released, possibly after reduction, which lowers binding affinity.
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The sequence of events surrounding iron release from MhFbpA almost
certainly involves the release and/or substitution of the carbonate
anion followed by the release of the bound ferric ion . As outlined in
Fig . 5, the iron- and anion-free form of MhFbpA
released from the inner membrane complex would complex with a readily
available carbonate anion in the periplasmic space prior to accepting
a ferric ion from the outer membrane receptor complex .
The first step in the iron removal process would involve the
movement of the Gln11 and the Asp36-Leu39 loop to provide access to
the anion binding and the iron binding site (Fig . 6) . This
step could occur spontaneously or be facilitated by interaction
with the FbpB/C complex at the inner membrane . The removal of the
carbonate anion could be facilitated by protonation through a
reduction in pH in the microenvironment at the FbpA/B/C interface .
The release of the carbonate anion would result in the opening of
MhFbpA and the lowering of its affinity for ferric ions . A similar
model for pH-mediated anion-iron release has been proposed for Tf in
the endosome (4) . Alternatively, the carbonate
anion could be displaced by a synergistic anion, as proposed by
Dhungana et al . (13) . As already described, we observed
difference electron density in the MhFbpAFe structure on the
solvent-exposed face of the ferric ion that impinges on the
carbonate-binding pocket . The difference electron density possibly
arises from a disordered citrate molecule . It is also possible that
the carbonate could be displaced by an acidic side chain presented
by the FbpB receptor . Since domain movement in FbpA may be restricted
when the protein is docked to FbpB, domain opening may be assisted
by a concomitant conformational change in the FbpB receptor .
Our observation of ferric ion binding in the presence of multiple
anions is interesting, since it demonstrates that MhFbpA is able to
transport iron in diverse chelation environments in vivo and may not
require a discrete synergistic anion .
Once FbpA is opened (by any mechanism), the increased solvent
exposure of the iron and the change in coordination would correspond
with a significant positive shift in the ferric ion redox potential,
as well as a lowered affinity of MhFbpA for the ferric ion . The
positive shift in the redox potential could facilitate the reduction
of the ferric ion in the opened form of MhFbpA that would further
reduce the binding affinity and thus facilitate the diffusion of
ferrous ions through the FbpBC channel . Our structural results will
have to be coupled with additional biochemical and biophysical work
to more clearly elucidate the mechanisms of iron binding and release
by this novel second class of bacterial transferrins .
This work was supported by grant 49603 from the Canadian Institutes
for Health Research . This work is based on diffraction experiments
conducted at the Advanced Light Source (ALS) . ALS is supported by the
Director, Office of Science, Office of Basic Energy Sciences,
Materials Sciences Division, of the U.S . Department of Energy under
contract no . DE-AC03-76SF00098 at Lawrence Berkeley National
Laboratory .
We also thank the staff at ALS for their excellent support .
* Corresponding author . Mailing address for Anthony B .
Schryvers: Department of Microbiology and Infectious Diseases, University of
Calgary, Calgary, AB, Canada T2N 4N1 . Phone: (858) 349-8770 . Fax: (403)
270-2772 . E-mail: schryver@ucalgary.ca .
Mailing address for Leslie W . Tari: ActiveSight Inc., 4045 Sorrento Valley
Blvd., San Diego, CA 92121 . Phone: (858) 349-8770 . Fax: (858) 455-6932 . E-mail: ltari@active-sight.com.
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