Originally published In Press as doi:10.1074/jbc.M203358200 on June 26, 2002
J. Biol. Chem., Vol. 277, Issue 37, 34229-34238, September 13, 2002
Cobalt Substitution of Mouse R2 Ribonucleotide Reductase as a
Model for the Reactive Diferrous State
SPECTROSCOPIC AND STRUCTURAL EVIDENCE FOR A FERROMAGNETICALLY
COUPLED DINUCLEAR COBALT CLUSTER*
Kari R.
Strand
,
Solveig
Karlsen§, and
K. Kristoffer
Andersson
¶
From the
Department of Biochemistry, University of
Oslo, P. O. Box 1041, Blindern, Oslo N-0316, and the
§ Department of Chemistry, University of Oslo, P. O. Box
1033, Blindern, Oslo N-0315, Norway
Received for publication, April 8, 2002, and in revised form, June 26, 2002
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ABSTRACT |
The R2 dimer of mouse ribonucleotide
reductase contains a dinuclear iron-oxygen cluster and tyrosyl
radical/subunit. The dinuclear diferrous form reacts with dioxygen to
generate the tyrosyl radical essential for the catalytic reaction that
occurs at the R1 dimer. It is important to understand how the
reactivity toward oxygen is related to the crystal structure of the
dinuclear cluster. For the mouse R2 protein, no structure has been
available with a fully occupied dinuclear metal ion site. A cobalt
substitution of mouse R2 was performed to produce a good model for the
very air-sensitive diferrous form of the enzyme. X-band EPR and light absorption studies (
550 nm = 100 mM
1 cm
1/Co(II)) revealed a
strong cooperative binding of cobalt to the dinuclear site. In
perpendicular mode EPR, the axial signal from mouse R2 incubated with
Co(II) showed a typical S = 3/2 Co(II) signal, and its
low intensity indicated that the majority of the Co(II) bound to R2 is
magnetically coupled. In parallel mode EPR, a typical integer spin
signal (Ms = ±3) with g ~ 12 is
observed at 3.6 K and 10 K, showing that the two Co(II) ions
(S = 3/2) in the dinuclear site are ferromagnetically
coupled. We have solved the 2.4 Å crystal structure of the
Co(II)-substituted R2 with a fully occupied dinuclear cluster. The
bridging Co(II) carboxylate ligand Glu-267 adopts an altered
orientation compared with its counterpart Glu-238 in Escherichia
coli R2. This might be important for proper O2
activation of the more exposed native diferrous site in mouse R2
compared with E. coli R2.
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INTRODUCTION |
The enzyme ribonucleotide reductase
(RNR)1 catalyzes the
conversion of ribonucleotides to deoxyribonucleotides, providing the cell with the essential building blocks for DNA synthesis and repair
(1, 2). A common feature for all RNRs isolated so far is a similar
reaction mechanism involving free radicals and redox-active cysteines.
The RNR enzymes can be grouped into three major classes based on the
mechanism used for radical generation and on structural differences
(3-6). RNR from mouse belongs to class Ia. RNRs in this class
are composed of
2
2 tetramers. The
2 dimers are called R1, and each subunit hosts an active
site and binding sites for allosteric effectors. Each subunit of the
2 dimers (called R2) contains a µ-oxo-bridged diferric
center (iron-oxygen cluster) (7) and a free tyrosyl radical in its active form. Upon binding of the substrate to the R1 protein, the
enzymatic reaction is initiated. The radical originating from the
tyrosyl radical of the R2 protein is transferred 35-40 Å to the
active site cysteines in the R1 protein (5, 7-11). This radical or
hydrogen atom is proposed to be propagated via a conserved chain of
hydrogen-bonded amino acid residues within the R2 and the R1 proteins.
Mutations of the amino acids in this chain lead to either a decreased
or a total loss of enzyme activity, which supports this radical
transport pathway (12-14).
RNR isolated from Escherichia coli is so far the best
characterized enzyme and prototype of class Ia. For mammalian RNRs, the
mouse enzyme may serve as a better model because there are a number of
significant differences between the E. coli enzyme and RNR
in higher organisms (7, 15). The sequence identity between mouse R2 and
E. coli R2 is only about 25% (15), although the identity is
higher among the eukaryotic R2 proteins (60-82%) (16). The newly
characterized human p53R2, which is possibly important in DNA repair,
also shows large sequence similarity to the mouse R2 protein (17,
18).
The three-dimensional structure of mouse RNR R2 has been determined at
2.3 Å resolution (16). The x-ray structure of Kauppi et al.
(16) showed that the iron center of mouse R2 had a more water-exposed and less hydrogen-bonding environment around the metal
site than in E. coli R2. So far it has only been possible to
crystallize the R2 mouse protein at pH 4.7, and at this pH only one of
the metal binding sites is occupied by iron. Structures of the
biologically relevant diferric and diferrous forms of the E. coli R2 enzyme have been solved. Both structures showed fully occupied di-iron sites (8, 19). No crystal structure has been published
on the active form harboring a tyrosyl radical. In this paper, we
present a model for the diferrous form of mouse R2, the form that
reacts with dioxygen and forms the essential tyrosyl radical and the
µ-oxo-diferric cluster (20-22). The diferrous form of R2 is
difficult to work with because it is very O2-sensitive. Substitution studies with other divalent metals that are less air-sensitive can provide useful information about this biological relevant form of the enzyme. In this study, Co(II) was chosen because
cobalt ions exhibit characteristic spectra depending on ligand
environments and thus provide the electronic structure for the metal
ion site of mouse R2 (23, 24). Analogous studies where the metal ion
cluster has been replaced have provided significant structural
information for many metalloproteins, among which are manganese-
(25-27) and cobalt- (28) substituted R2 RNRs. The x-ray manganese
structures have served as good models for the reduced form of the
E. coli R2 enzyme.
Among the isolated and characterized non-corrin-cobalt-containing
enzymes, the most relevant for comparison with R2 is the methionine
aminopeptidases isolated from E. coli. The x-ray
structure revealed a dinuclear cobalt site with carboxylate and
histidine ligands (29). This rich carboxylate coordination environment is very similar to the carboxylate-bridged dinuclear iron centers we
find in the iron-oxygen proteins such as class I R2 RNR, methane monooxygenase hydroxylase (MMOH), and acyl-carrier-protein
9-desaturase, which are all capable of activating
dioxygen for subsequent oxidation chemistry. However, this is not the
case for the cobalt-containing methionine aminopeptidases, which from E. coli requires two Co(II) atoms for hydrolytic activity to
cleave the N terminus from newly translated polypeptide chains.
In this study we report the first crystal structure of a fully occupied
dinuclear site of mouse R2 RNR at pH 6. A structure at this pH is more
physiologically relevant than the previous structure at pH 4.7. It also
gives new insights into the structure and spectroscopic properties of
the reduced diferrous center of mouse R2. Our EPR studies show that the
cobalt atoms in the dinuclear site are ferromagnetically coupled in
contrast to cobalt-substituted E. coli R2 (28). Several
other non-corrin-cobalt enzymes other than methionine aminopeptidases
have been isolated and characterized (prolidase, nitrile hydratase,
glucose isomerase, methylmalonyl-CoA carboxytransferase, aldehyde
decarbonylase, lysine 2,3-aminomutase, and bromoperoxidase) (30), and
the ferromagnetic coupled dinuclear Co(II) cluster in mouse R2 can
serve as a model for active dinuclear cobalt-containing proteins.
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EXPERIMENTAL PROCEDURES |
Protein--
The cloned mouse R2 apoprotein was prepared as
reported by Mann et al. (21). The apoR2 protein obtained
after purification was pretreated with hydroxyurea and EDTA and passed
down a 10-ml Sephadex G-25 column to remove all iron and reduce the
tyrosyl radical before reconstitution with Co(II). The protein
concentration was determined using a Bio-Rad protein assay (31) or the
molar extinction coefficient
280-310 nm = 124 mM
1 cm
1/90 kDa (R2 dimer)
(21).
UV-Visible Measurements--
Optical absorption spectra were
collected on a Hewlett-Packard 8452 diode array spectrophotometer.
EPR Measurements--
The EPR spectra were recorded at X-band on
a Bruker ESP 300E, fitted with a Bruker ER4116DM dual mode cavity and
an Oxford ESR 900 helium flow cryostat. The signals were measured at
different microwave powers to prevent power saturation. They were
quantitated by comparing double integrals of spectra with high spin
Co(II) in either 50 mM Tris-HCl, pH 7.6, 20% glycerol or 100 mM MES, pH 6.0, 1.2 M NaCl, 20% glycerol
depending on which pH the cobalt substitution of R2 was performed. The
spectra were recorded under identical non-saturating microwave power.
Crystallization and X-ray Data Collection--
The R2 crystals
were grown in hanging drops as described earlier (32) using 7.5 mg/ml
protein in the presence or absence of 3.8 equivalents of Co(II)/R2
dimer and 0.1 M sodium acetate buffer, pH 4.7, containing
1.2 M NaCl. Diffraction below 3 Å resolution was observed
at BM01A (Swiss-Norwegian Beamline, SNBL) and a dataset to 2.2 Å resolution was collected at ID14-1 at European Synchrotron Radiation
Facilities (ESRF), Grenoble, France. Map interpretation showed binding
only of mononuclear cobalt in site 2 (the site farthest away from the
tyrosyl radical site Tyr-177; see Fig. 7B). To increase the
binding of cobalt, the crystals of apoR2 were soaked in 5 mM CoCl2 for 3 h, and the pH was increased
gradually to about 6 by adding 1 M sodium acetate. Sodium
ascorbate (2 mM) was added to the solution to prevent
oxidation of the Co(II) ions. One crystal was transferred to a
cryosolution of 25% glycerol, 5 mM Co(II), and 2 mM sodium ascorbate and flash-frozen in liquid nitrogen. A
2.4 Å dataset was collected on a MAR CCD detector at beamline ID14-3
at ESRF in Grenoble. The 120 frames were measured, processed in DENZO,
and merged in Scalepack (33) and gave 99.3% completeness (15,274 unique reflections) between 30.0 and 2.4 Å resolution, a
Rmerge of 9.5% and I/
I
value of 9.6.
Refinement and Model Building--
Although our
cobalt-substituted R2 and apoR2 proteins were crystallized using the
same conditions as for the iron-reconstituted mouse R2 protein reported
by Kauppi and co-workers (16, 32), the cell dimensions (space group
C2221, one monomer in the asymmetric unit) were shorter.
Therefore, the molecular replacement technique had to be used for the
structure determination. The R2 protein (PDB 1XSM) was used as
search model, and all water molecules and the single iron ion were
deleted. The rotation and translation searches were carried out with
the CNS program package (34).
After the rigid body refinement, simulated annealing and positional
refinement in CNS electron density maps (Fo-Fc
and 2Fo-Fc) showed well defined electron
density at an 8-
level for the cobalt ions in the proposed metal
center in the protein. The program O (35) was used for map inspection
and model building. The cobalt ions were included in the coordinate
file, and 113 water molecules were added in several iterations to the
model and refined in CNS. Only water molecules with well defined
density and reasonable hydrogen bond geometry were chosen. The
refinement brought R and Rfree based
on 5% of the data down to 21.8 and 29.7%, respectively.
The 65-352-residue model of the Co(II)-substituted R2 protein refined
to 2.4 Å showed good stereochemistry with deviations from ideal
geometry of 0.024 Å for bond lengths, 2.1° for bond angles, and
21.8° for dihedral angles. In the CNS package (34), the mean
coordinate error was estimated to be 0.31 Å for the entire structure.
The program PROCHECK (36) estimated that 89.0% of the nonglycine and
proline residues were in the most favored regions, whereas 9.5 and
1.5% were found either in other allowed or in generously allowed
regions, respectively. Four amino acids (Arg-79, Phe-81, Arg-149, and
Glu-307) in the latter mentioned region are all in flexible loops at
the surface of the protein and have high temperature factors. The
coordinates for the structures of mono-Co(II)-R2 and
di-Co(II)-R2 are deposited in the Protein Data Bank and have been
assigned PDB ID 1h0o.pdb and 1h0n.pdb, respectively.
 |
RESULTS AND DISCUSSION |
EPR Evidence for Formation of a Magnetically Coupled Dinuclear
Co(II) Cluster--
In this study, we have substituted the natural
iron cluster with cobalt. We chose Co(II) because it would make a good
model for the native dinuclear ferrous cluster of the enzyme. The mouse apoR2 protein after purification was pretreated with hydroxyurea and
EDTA to remove all iron before incubation with Co(II). Aqueous solutions of Co(II) are readily oxidized to Co(III). The air-sensitive Co(II) buffer solutions were made fresh just before use. Unlike the
very air-sensitive diferrous R2 protein, the cobalt-containing form of
mouse R2 (Co(II)-R2) shows no difference in oxidation state whether the
reconstitution was performed aerobically or anaerobically (data not
shown). Unless otherwise indicated, all of the work represented in this
paper is done aerobically. This apparent insensitivity to dioxygen is
consistent with reports of other cobalt-substituted proteins such as
the anaerobic prepared cobalt-substituted R2 protein from E. coli (28). This protein did not appear to bind or activate dioxygen.
Incubation of R2 with a Large Excess of Cobalt--
The
reconstitution was first made at pH 7.6 by the aerobic addition of 10 molar excess of Co(II)/apoR2 dimer (typical [R2] was 0.2-0.5
mM). This yielded a pink cobalt R2 derivative within seconds. The sample was passed down a small Sephadex G-25 column at
4 °C to remove any unbound cobalt from the protein. The EPR spectrum
at 4 K of the gel-filtered Co(II)-R2 sample had a broad signal from 50 to 370 mT, typical of Co(II) high spin S = 3/2 (Fig.
1, dotted line).

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Fig. 1.
Evidence for EPR-silent Co(II) in
Co(II)-R2. At 10 K, X-band EPR spectra of Co(II)-R2, pH 7.6 (dotted line), and Co(II)-R2 denatured (1.4 M
HCl, 12 h at room temperature) (solid line) are shown.
The protein concentration was 0.2 mM. Instrumental
conditions: microwave frequency, 9.6 GHz; microwave power, 0.2 mW;
modulation, 1.0 mT.
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Systems with S > 1/2 can be described by the spin
Hamiltonian (23, 24, 28, 37-40)
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(Eq. 1)
|
in which
is the Bohr magneton, B is the applied
magnetic field, g is the Landé matrix, D is
the axial zero-field splitting parameter, and E is the
rhombic zero field splitting parameter. |E/D| ranges between 0 and 1/3.
|E/D| = 0 corresponds to the fully axial
case, and |E/D| = 1/3 is the fully
rhombic case.
The observed broad axial X-band EPR signal from Co(II)-R2 is typical
for the lowest Kramers doublet (Ms = ± 1/2)
from S = 3/2 high spin mononuclear Co(II) species. The
signal has a geff at ~170 mT
(g ~ 4.1) with a gmax value
at ~ 5.4 and a signal at g = 2.02 over a
temperature range from 3.6 to 30 K. The g values of the
Co(II)-R2 sample are close to the theoretical axial S = 3/2 g values at 4.0, 4.0, and 2.0. Different traces
of Co(II) low spin (S = 1/2) impurities are observed
above g = 2. No tyrosyl radical was generated during
the aerobic reaction of apoR2 with Co(II) (Fig. 1, dotted
line).
A full occupancy of the native µ-oxo-diferric binding site will give
a binding stoichiometry of 4 metal ions/R2 dimer. Quantitation of the
observed broad axial gmax ~ 5.4 EPR signal
from the gel-filtered Co(II)-R2 sample against Co(II) in buffer showed
that about 15-20% of the expected metal binding sites were occupied
with EPR-active Co(II). To rule out the presence of EPR-silent Co(III),
a reduction of the protein with dithionite was performed. This gave no
change in the observed EPR signal (data not shown). The Co(II)-R2
sample was acid denatured (1.4 M HCl, 12 h at room
temperature). The EPR spectrum of the acid-denatured Co(II)-R2 sample
(Fig. 1, solid line) showed an increase in the intensity of
the Co(II) S = 3/2 EPR signal compared with the
intensity from the Co(II)-R2, pH 7.6, sample (Fig. 1, dotted
line). Assuming that the intensity of the Co(II) signal after acid
denaturation represents all Co(II) bound to R2, the results suggest
that 80% of the metal binding sites in the Co(II)-R2 sample at pH 7.6 was occupied with EPR-silent Co(II). The EPR spectra of Co(II) in
buffer did not change in shape or intensity when HCl was added. These
results imply that the majority of the Co(II) atoms bound to R2 at pH
7.6 interact with each other to form a magnetically coupled dinuclear
site that cannot be detected by perpendicular mode X-band EPR. The binding ratio of cobalt to R2 indicates that most of the available metal sites are occupied with magnetically coupled cobalt atoms in the
gel-filtered Co(II)-R2 sample.
The Formation of the Dinuclear Co(II) Cluster--
The formation
of the perpendicular mode X-band EPR-silent metal site at pH 7.6 can be
followed by preparing EPR samples with an increasing ratio of Co(II) to
apoR2 without gel filtration. The EPR spectra from the titration of R2
with 1-8 equivalents Co(II) are identical in shape to the spectrum
observed from the gel-filtered Co(II)-R2 sample, although with
different intensities (Fig. 2,
B and C). When the ratio of the concentration of
added Co(II) to apoR2 reached the level at which formation of
magnetically coupled dinuclear cobalt sites becomes possible, the
relative intensity of the gmax = 5.4 Co(II)
S = 3/2 EPR signal from the cobalt-substituted R2 will
no longer be comparable in intensity with that of a buffer sample of
CoCl2 of identical concentration (Fig. 2, A and
B). Thus, a quantitation of the Co(II) EPR signal of a
sample containing 4 equivalents of cobalt/R2 dimer shows that the
intensity drops to about 60% of the EPR signal from the same amount of
cobalt in buffer. This means that about 40% of the cobalt bound to R2
is EPR-silent, and 60% behaves as Co(II) in buffer.

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Fig. 2.
The EPR-active Co(II) in Co(II)-R2 at pH 7.6 and 6.0. At 0.2 mW and 10 K, the X-band EPR spectra of 1.8 mM Co(II) in 50 mM Tris-HCl, pH 7.6, 20%
glycerol (* 0.2) (A), 4 equivalents of Co(II)-R2 dimer (4 Co(II)-R2) in the same buffer as A (B), and 6 equivalents of Co(II)-R2 dimer (6 Co(II)-R2) in the same buffer as
A are shown (C). At 127 µW, 3.8 K, the X-band
EPR spectra of 1.8 mM Co(II) in 0.1 M MES, 1.2 M NaCl, pH 6.0 (* 0.2) (D) and 6 equivalents of
Co(II)/R2 dimer (6 Co(II)-R2) in the same buffer as D
(E) are shown. [R2] = 0.3 mM in all samples.
Instrumental conditions: microwave frequency, 9.6 GHz; modulation, 1.0 mT.
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To quantify the observed EPR signal, the D value has to be
positive. The microwave power saturation behavior at different temperatures can give a D value using the method of Makinen
and co-workers (37, 38). Fig. 3,
A and B, shows the effect of microwave power
saturation at 3.6 and 5.8 K of the gmax signal from samples where 4 and 6 equivalents of cobalt/R2 dimer were added,
respectively. Fig. 3B also shows the behavior of
identical concentrations of Co(II) in buffer at 3.6 K (50 mM Tris-HCl, pH 7.6, 20% glycerol). Table
I summarizes the EPR relaxation
parameters of the gmax signal from the different
samples at different temperatures. The parameters of the saturation
curves in terms of microwave power at half-saturation
P1/2 and b are summarized in Table I. The parameter b describes the contribution of nonhomogeneous
broadening (41) to the saturation curve as shown in Equation 2,
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(Eq. 2)
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where I is the EPR amplitude and P is the
microwave power.

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Fig. 3.
Microwave power saturation of the
gmax 5.4 component of the Co(II) signals. Continuous
traces are computer fits (Equation 2). [R2] = 0.5 mM in
all samples. EPR microwave power saturation curves of A are
4 equivalents of Co(II)/apoR2 at 3.6 K ( ) and 5.8 K ( ).
B, 6 equivalents of Co(II)/apoR2 at 3.6 K ( ) and 5.8 K
( ) and 3 mM Co(II) in buffer ( ) at 3.6 K (50 mM Tris-HCl, pH 7.6, 20% glycerol).
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Table I
Microwave power saturation P1/2 values of the gmax 5.4 component at 3.6 and 5.8 K of Co(II)-substituted R2 and Co(II) in
buffer (50 mM Tris-HCl, pH 7.6, 20% glycerol
P1/2 and b values were estimated from
computer fitting of the microwave saturation curves. The
P1/2 values do change slightly with
b = 1; letting b float improves the fitting.
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The P1/2 values were estimated to 0.2-0.3 mW at
3.6 K and 8-16 mW at 5.8 K with b ~ 0.7 or
b = 1 for both Co(II)-R2 samples. The
P1/2 for the Co(II) in buffer was estimated to
0.3 mW at 3.6 K. The saturation behaviors of the three samples are
similar (Table I). In the Co(II)-R2 samples, there might be a small
fraction of mononuclear Co(II) bound to R2. Integration of the EPR
signal under nonsaturating conditions demonstrates a 20-30% decrease at 5.8 K compared with 3.6 K. A negative D value
would have increased the EPR-active Co(II) signal when the temperature
was increased. Taken together with the microwave saturation behavior
this shows a positive D value for the EPR-active species in
Co(II)-R2 (37, 38). The acid-treated Co(II)-R2 also has EPR properties
identical to the high spin EPR-active Co(II) in Co(II)-R2 and in buffer (data not shown). The observed cobalt signals in all three of these
samples have similar positive and large D values. This
validates the quantitation of the EPR-active Co(II) in Co(II)-R2. It
also shows that the majority of the EPR-active Co(II) present in mouse Co(II)-R2 is very similar to Co(II) in buffer.
Fig. 4 presents the amount of EPR-active
Co(II) in the Co(II)-R2 samples (dotted line) when
increasing amounts of Co(II) are added to apoR2. At 100%, all Co(II)
added is EPR-active, whereas lower values show the presence of
EPR-silent cobalt. With 1 equivalent of Co(II)/R2 dimer, ~ 90% of
the cobalt is EPR-active. Addition of more equivalents of Co(II)
decreases the intensity of the signal compared with the same amount of
cobalt in buffer. This demonstrates the formation of the dinuclear
cobalt site that is magnetically coupled and may therefore be
EPR-silent in perpendicular mode. The lowest relative amount of
EPR-active Co(II) and a nearly saturated cluster is at ~ 6 equivalents of Co(II) added per R2 dimer. Adding 8 equivalents of
Co(II)/R2 dimer gave an EPR signal with ~ 60% intensity
compared with the same amount of Co(II) in buffer. If R2 is saturated
when 8 equivalents of Co(II) is added per R2 dimer this should give an
intensity of the observed S = 3/2 Co(II) EPR signal
corresponding to ~ 50% of the signal observed for the same amount of Co(II) in buffer. The result indicates nearly saturated dinuclear sites with ~ 4 equivalents of EPR-silent dinuclear
Co(II)/R2 dimer when 8 equivalents are added. The titration illustrates that the affinity for Co(II) is low, and more than 4 Co(II)/R2 dimer is
needed to occupy fully the four well defined metal binding sites in the
mouse R2 dimer.

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Fig. 4.
Formation of the dinuclear Co(II) cluster
followed by EPR and light absorption. The dotted line
represents the EPR-active Co(II) in Co(II)-R2 when different amounts of
Co(II) are added to apoR2 ([R2] = 0.5 mM). 100% is when
all Co(II) added to R2 is EPR-active. The solid line
represents the sigmoidal fitting of the data of the
A550 nm absorption band intensity when different
amounts of Co(II) are added to apoR2 (using the program Origin 6.1;
OriginLab Corporation, www.OriginLab.com). Similar fittings are
obtained using a four-binding Adair equation (with four largely
different binding constants), a cooperative equation or a Hill equation
with the Hill coefficient in the range from 4 to 4.7 (using the program
GraFit Version 4 and nonlinear regression, Erithacus Software Limited,
www.erithacus.com/grafit).
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Light Absorption Spectra of Co(II)-R2--
The visible spectrum of
the fully occupied Co(II)-R2 (Fig.
5A, solid line) is
clearly red shifted and more intense than the spectrum of Co(II) in
buffer solution (Fig. 5A, dotted line). The
induction of this red shift was followed spectrophotometrically by
adding increasing amounts of cobalt to the apoR2 protein (Figs. 4 and
5B). The appearance of the 550 nm absorption maximum was not
significant until the addition of 2-3 equivalents of cobalt/R2 dimer
and saturated by ~ 7 equivalents of Co(II)/R2 dimer. The creation of the dinuclear cluster observed by EPR also confirmed this
low affinity for cobalt. The affinity toward cobalt is lower for mouse
R2 compared with that reported for cobalt-substituted E. coli R2 where there is saturation with 4 equivalents of Co(II)/R2 dimer (28).

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Fig. 5.
Cobalt-dependent formation of the
pink chromophore in R2. A, visible absorption spectra of
Co(II) in 50 mM Tris-HCl, pH 7.6, 20% glycerol ([Co(II)] = 24 mM) (dotted line), and R2 saturated with
cobalt ([R2] = 0.5 mM) (solid line). Molar
absorptivity is given per Co(II). B, Co(II) titration of
apoR2. Visible absorption spectra of apoR2 in the presence of 1 (. . . . . ), 2 (×), 3 ( ), 4 ( ), 5 ( ), 7 ( ), and 8 (- - -) molar equivalents of Co(II) ion/R2 dimer are shown.
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The formation of the 550 nm chromophore when cobalt binds to apoR2 can
be fitted to a sigmoidal binding model (Fig. 4, solid line).
This indicates a strong cooperative interaction between the protein and
the dinuclear Co(II) center. The dinuclear site is formed concomitantly
with a strong 550 nm absorption. Possibly both Co(II) ions contribute
to the observed pink color because both binding sites of Co(II) have
almost the same geometry (see below, Fig. 7B). The affinity
for the dinuclear Co(II) cluster is low because 2 mM Co(II)
is needed for half-saturation of 0.5 mM R2. Co(II) binding
to R2 followed by light absorption at pH 7.6 corresponds well with the
EPR behavior because both demonstrate the presence of a fully occupied
dinuclear site at 7-8 equivalents of Co(II)/R2 dimer.
Comparison with the Cobalt-substituted R2 from E. coli--
The
anaerobic cobalt-substituted R2 from E. coli showed a pink
color and had a very similar absorption spectra regarding intensity and
max to what we have observed for the Co(II)-substituted
R2 from mouse (28). The EPR spectrum of Co(II)-R2 from E. coli is typical for S = 3/2 high spin mononuclear
Co(II) species, and the intensity of the signal is consistent with the
Co(II) atoms not being magnetically coupled when bound to the R2
protein. More hyperfine structure and the presence of a rhombic
component are seen for the EPR-active Co(II) in the cobalt-substituted
E. coli R2 than we observe for the cobalt-substituted mouse
R2 at pH 7.6. This is probably due to the fact that the EPR-active
Co(II) observed for mouse R2 is mostly Co(II) in buffer and not
mononuclear cobalt bound to R2 as in E. coli R2. For our
cobalt-substituted mouse R2 protein, most of the cobalt was silent in
perpendicular mode EPR.
Evidence for a Ferromagnetically Coupled Dinuclear Cobalt Cluster
in R2--
The EPR and light absorption studies of Co(II)-R2 were
performed at pH 7.6. In this paper, we present the first crystal
structure of a fully occupied metal site in mouse R2 at pH 6 (see
below, Fig. 7). At pH above that, the crystals dissolve in the buffer. To be able to compare the EPR and light absorption results with the
crystal structure, we prepared a Co(II)-R2 EPR sample as close to
crystal conditions as possible. The EPR spectrum of the Co(II)-R2 prepared in 0.1 M MES, pH 6.0, 1.2 M NaCl, 20%
glycerol, did show an EPR signal of high spin Co(II) S = 3/2, similar to what we observed when the sample was prepared at pH
7.6, although with a more pronounced shoulder at ~ 100 mT and
possible hyperfine structure (Figs. 2E and
6A). At pH 6.0, the intensity
of the S = 3/2 signal is also low compared with that of
identical concentrations of cobalt in buffer (Fig. 2, D and
E). This shows that if the reconstitution is carried out at
pH 7.6 or 6.0, most of the cobalt bound to R2 will form magnetically
coupled dinuclear sites. In addition, the pH 6.0 sample
contains a low field perpendicular mode EPR signal at g ~ 9.2, both at 127 µW (Fig. 2E) and more clearly visible
at 10 mW (Fig. 6A), where Co(II) in buffer is partially
saturated. The g ~ 9.2 signal is not clearly visible even at a microwave power of 10 mW for the sample prepared at pH 7.6 (data not shown).

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Fig. 6.
The presence of an integer spin EPR signal.
A, the X-band EPR spectra of 6 Co(II)-R2 at pH 6.0, [R2] = 0.3 mM, 10 mW, 3.8 K, perpendicular mode EPR at 9.6 GHz.
B, same sample as in A, 127 µW, 3.8 K, parallel
mode EPR at 9.4 GHz (four accumulations). C, same sample as
in A, 0.5 mW, parallel mode EPR at 9.4 GHz, 3.8 K
(solid line) and 10 K (dotted line).
D, same sample as in A, 127 µW, parallel mode
EPR at 9.4 GHz, 3.8 K, (solid line, four accumulations) and
8 Co(II)-R2 at pH 7.6, 127 µW, parallel mode EPR at 9.4 GHz, 3.8 K,
[R2] = 0.5 mM (dotted line, four
accumulations). All spectra were obtained with a 1.0 mT modulation
amplitude.
|
|
In parallel mode EPR, the only signal observed for the Co(II)-R2
samples prepared at both pH 7.6 and 6.0 at 3.8 K is a low field signal
at g ~ 12 (Fig. 6, B and D).
The parallel mode EPR signal can be described as a broad negative peak,
expanding from 20 to 120 mT at X-band. The Co(II) S = 3/2 signal
is no longer EPR-active as expected. The g ~ 12 signal is strong enough to be observed below 0.1 mW. The shape of the
parallel mode signal as well as the shift in g value
compared with the signal observed in perpendicular mode EPR is typical
for integer spin signals (42, 43). The integer spin signal observed for
the diferrous form of the mouse R2 protein showed a similar behavior
(44).
The intensity of the g ~ 12 integer spin signal at pH 6.0 decreased when the temperature rose to 10 K (Fig. 6C) and
was hardly observed at higher temperatures, indicating that the signal
arises from a ground-state transition. The observed g value
at 12 is the expected theoretical geff value for
an Ms = ± 3 transition. We assign the signal to
arise from the Ms = ± 3 ground state spin system that would arise from a ferromagnetic coupling of the two high
spin S = 3/2 Co(II) ions in the dinuclear cobalt site.
Both ferromagnetic and antiferromagnetic coupling are observed in other
dinuclear cobalt-substituted proteins. A ferromagnetic-coupled dinuclear cobalt center was observed in a Co(II)-substituted hemocyanin (45) and a Co(II)-substituted aminopeptidase from Aeromonas proteolytica (46). The cobalt-substituted dinuclear form of aminopeptidase from A. proteolytica showed that most of the
Co(II) added to the protein has no mononuclear S = 3/2
EPR signal. A signal with a g value ~ 12 was observed
in parallel mode EPR. This signal is very similar to what we observe
for the cobalt-substituted mouse R2. Bennett and Holz (46)
assign this signal to a S = 3 spin system that would
arise from a ferromagnetic coupling of two high spin S = 3/2 Co(II) ions in the active site of the aminopeptidase (46).
The appearance of the integer spin EPR signal was found to depend on
pH. As pH decreases from 7.6 to 6.0, the intensity of the
Ms = ±3 signal increases (Fig. 6D).
Ms = ±3 signals are difficult to quantify
because no good standard exists to enable measurement of this type of
signal. The reason why the signal is more pronounced at pH 6.0 than 7.6 is probably because of
(another zero field splitting parameter in
integer spin EPR) being higher at pH 7.6 and therefore difficult to
detect with X-band EPR (hv
0.3 cm
1). The
resonance condition for an integer spin signal is (42, 43):
|
(Eq. 3)
|
where
is the zero field splitting of the spin doublet which
gives rise to the resonance, geff is the
effective g value along a principal axis of the zero field
coordinate frame, and
is the angle between that principal axis and
the static field B. Lowering the pH to 6.0 might lead to
changes in
to below or around 0.3 cm
1 so that a
higher fraction becomes EPR-active under X-band parallel mode EPR
conditions. Such a difference in
was suggested to be the reason why
an integer spin signal in the X-band parallel EPR mode for the
diferrous form of the mouse R2 protein can be observed (44) and not for
the diferrous form of the E. coli R2.
The perpendicular mode EPR signal from the sample prepared at pH 6.0 might consist of free Co(II) in the buffer overlapping with a rhombic
signal as seen by the shoulder at 100 mT. This EPR signal resembles the
signal observed for the cobalt-substituted R2 from E. coli
protein (28) and could represent a mononuclear occupied metal site of
mouse Co(II)-R2.
X-ray Structure of Co(II)-substituted R2 from Mouse--
In the
first experiments, the mouse R2 crystals were cocrystallized with 3.8 equivalents of Co(II)/R2 dimer at pH 4.7. These conditions only led to
crystals with partially mononuclear occupancy of the metal binding site
2 (the site farthest away from the radical Tyr-177, see below). Both
EPR and light absorption data had revealed that the affinity for Co(II)
is weak. This might be because of the open structure around the metal
site leading to loss of bound cobalt into the solution as for iron or
because the cobalt is not the natural element for R2. To get fully
occupied metal centers, the 4 equivalents of Co(II)/R2 dimer had to be
increased. To find the proper conditions for a fully occupied metal
site, the crystals were studied under a microscope to determine the
incubation time and the right concentration of Co(II) to use in the
soaking solution.
In this work we managed to raise the pH in the Co(II)-R2 crystals to 6. The mono-iron mouse R2 structure was solved at pH 4.7 (16). In both
structures, only residues 65-352 of the 390 amino acids are seen in
the electron density maps, indicating that the N- and C-terminal ends
are flexible. Two peaks in the proposed metal binding site are clearly
seen in the difference-Fourier maps 2Fo-Fc
showing that the cobalt ions were bound to the protein with full
occupancies after soaking the crystals in a 5 mM Co(II) solution for 3 h at room temperature (Fig.
7A). Average temperature factors for dicobalt R2 mouse protein main chain and side chains are
36.8 and 38.2 Å2, respectively; for the site 1 cobalt ion,
37.4 Å2; and for the site 2 cobalt ion, 29.4 Å2. This shows that site 2 has a higher occupancy of
cobalt ions and less flexibility than site 1 at pH 6.

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Fig. 7.
The 2.4 Å resolution structure of the
dinuclear cobalt cluster of mouse R2. A, electron density
map (2Fo-Fc) contoured at 2
(blue) and 6 (red) for the metal binding site
in mouse Co(II)-R2. The cobalt ions are seen in green. The
figure was drawn with Bobscript (65), a modified version of Molscript
(66). B, the dicobalt center of R2 with ligands Asp-139,
Glu-170, His-173, Glu-233, His-270, Glu-267, and the radical site
Tyr-177. The cobalt-ligand interactions are marked with dotted
lines. The figure was made in Bobscript (65).
|
|
Fig. 7A shows the electron density, and Fig. 7B
shows a model of the metal ligands, the cobalt ions, and the stable
free radical site Tyr-177. All residues that make interactions with the
cobalt ions are well defined in the density map. The glutamic acids at 170 and 267 have a bidentate bridging binding mode to the cobalt ions.
The binding of Asp-139 and His-173 to the Co(II) in site 1 (Co1) and
Glu-233 and His-270 to the Co(II) in site 2 (Co2) make both metal ions
4-coordinated. The distance between the cobalt ions is 3.40 Å (Table
II).
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|
Table II
Interatomic distances (Å) in Co(II)-R2 from mouse, diferrous R2 from
E. coli, and diferrous MMOH (M. capsulatus)
|
|
Mononuclear and Dinuclear Cobalt R2 Mouse Structures--
The
protein crystallizes only at pH 4.7, and at this pH when cocrystallized
with cobalt only one of the metal sites is occupied with mononuclear
cobalt (site 2). The occupancy of only one of the metal binding sites
is the same as was observed in the first x-ray structure of mouse R2 by
Kauppi et al. (16). The mono-iron mouse R2 crystals
were soaked in a solution of ferrous salt at pH 4.7. This increased the
occupancy on the already occupied site without any detectable binding
at the second site. We managed to increase the pH in our crystals by
simultaneously soaking the crystals in a buffer solution containing
Co(II). This treatment also led to occupancy of site 1. A comparison of
the monocobalt-substituted structure at pH 4.7 and the
dicobalt-substituted structure at pH 6 of mouse R2 is presented in Fig.
8A. In the monocobalt
structure, only site 2 is occupied by cobalt ions. The cobalt atom is
4-coordinated, and the ligands are Glu-170, His-270, Glu-233, and
Glu-267. Greatest flexibility is shown by the carboxylate ligands upon
binding of the second cobalt ion. The occupation of site 1 moves
Asp-139 closer to the metal site, and a change in the orientation is
observed. The orientation of Glu-233 is also altered. In the dinuclear
structure, Glu-267 and Glu-170 make carboxylate bridges between the
cobalt ions. The histidines (at 173 and 270) do not change
significantly. They form the rigid framework of the binding site. Upon
increasing the pH to 6, we do not observe any changes in the position
of the stable radical Tyr-177 or the hydrogen bonding pattern and position of the amino acids involved in the radical transport pathway.
Neither do we observe any changes in the acceptability and the
hydrophobicity of the environment around the metal site compared with
the structure at pH 4.7 solved by Kauppi et al. (16).

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Fig. 8.
Comparisons with mononuclear
cobalt-substituted R2. A, comparison of the binding mode of
cobalt in the mononuclear (light blue) and the dinuclear
(pink) metal center of mouse R2. The figure was made using
Molscript (66). B, the mononuclear cobalt center of mouse R2
in light blue compared with the structure of the mononuclear
iron center of mouse R2 in dark blue (PDB 1XSM). The
metal ions are seen in gray (iron) and black
(cobalt).
|
|
Comparisons of the Mononuclear Co(II) and Iron Mouse R2
Structures (Both at pH 4.7)--
The monocobalt structure is
overall similar to the previously reported mono-iron structure (16)
(Fig. 8B). The iron ion (probably Fe(III)) is located closer
to Glu-267 and has a bidentate binding mode. In the monocobalt
structure, the cobalt ion makes only one interaction with this residue.
His-270 and His-173 have similar orientations in the two structures. In
Glu-170, Glu-233, and Asp-139, small changes in the orientation are
observed. Other significant differences in the structures are only seen
in the flexible loop areas on the surface of the enzyme and probably have no influence on the formation of the active site in R2.
Structural Implications: Co(II)-R2 from Mouse Compared with the
Reduced Wild Type of E. coli R2 and MMOH--
Soluble MMOH and class I
RNR are members of the same class of iron-oxygen proteins (7). Although
the chemistry performed by the iron-oxygen proteins and their overall
structures differ markedly, some of their active sites can be
strikingly similar. Their metal sites contain carboxylate and histidine
ligands. The essential carboxylate ligands are shown to be able to
adopt several conformations that can also vary with the oxidation state
of the metals (5, 19, 25-27, 47, 48). Carboxylate shifts are believed
to be important to accommodate different redox states during redox
cycling of these kinds of centers.
The x-ray structures of the dinuclear clusters of the
cobalt-substituted mouse R2 and the diferrous R2 E. coli are
similar (Fig. 9, pink and
black structures, respectively). In both complexes, the
metal ions are 4-coordinated and have the same binding mode to their
ligands. The histidines His-173(His-118) and His-270(His-241) show very
little variation in their orientation in the different x-ray structures
(E. coli numbering in parentheses). Significant variations in the position of all of the carboxylate ligands
Glu-267/Glu-233/Asp-139/Glu-170 are observed. Compared with E. coli, both Glu-233(Glu-204) and Asp-139(Asp-84) move closer to the
metal binding sites forcing the metal atoms closer together, and
therefore the metal distance between Co1 and Co2 becomes 0.5 Å shorter
that the corresponding metal to metal distance in the diferrous wild
type E. coli (3.9 Å) (19) (Table II). This agrees well with
the EPR studies showing that the cobalt ions in mouse R2 have a strong
magnetic coupling, whereas this is not the case for the diferrous ions
in E. coli R2, which are weakly antiferromagnetically
coupled (49). The most interesting change that we observe in the
cobalt-substituted mouse structure compared with that of the reduced
wild type E. coli structure is the carboxylate shift seen
for the bridging carboxylate ligand Glu-267 compared with the E. coli counterpart Glu-238.

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Fig. 9.
Superposition of the Co(II)-R2 from mouse,
diferrous E. coli R2, and diferrous MMOH
from M. capsulatus metal sites. The dicobalt
center of mouse R2 (pink) displayed with metal-binding
ligands and Tyr-177, compared with the diferrous center of E. coli R2 (black, PDB 1XIK) and the chemically
reduced wild type MMOH from M. capsulatus (green,
PDB 1FYZ). The metal ions and water molecules are seen in gray and red,
respectively, and outlined in their respective colors. The figure was
made using Molscript (66).
|
|
Even though mouse and E. coli R2 proteins belong to the same
RNR class (class Ia), and their metal ions ligands are conserved, several differences in the behavior of these two clusters are observed.
The redox properties of the R2 protein from mouse are significantly
different from those of the R2 from E. coli. For example,
the reduced mouse R2 in glycerol exhibits an integer EPR signal with a
g value observed around 14 (44) which is not shown for the
E. coli enzyme. The mixed valence form (Fe(II)Fe(III)) of
mouse R2 can be induced by a mild chemical reduction with a 30% yield
(44, 50). In the E. coli R2 protein, this redox state is
only produced in small amounts. Even using drastic conditions as high
pH only increases the yield to ~ 5%. The coupling between the
iron atoms in the oxidized state is weaker in mouse than in E. coli (51, 52). The redox properties of the mouse R2 iron-oxygen center resemble those of MMOH. In MMOH, both the integer spin signal in
the reduced form and the mixed valence state is observed (7, 53, 54).
The x-ray structure of the dinuclear cobalt cluster in R2 from mouse
reveals that it is similar to the chemically reduced di-iron form of
MMOH from Methylococcus capsulatus (48, 55) (Fig. 9, MMOH
represented in green). The reduced structure of MMOH
contains two iron centers bridged by one µ-1,3- and one µ-1,1-carboxylate ligand. One histidine and one monodentate glutamate are coordinated to each iron, and additional water is bound to one of
the irons. Both iron atoms in the metal center are 5-coordinated. The
Glu-144 in the MMOH structure and the Glu-170 in the cobalt-substituted mouse R2 structure are in similar orientations as are the histidines (Fig. 9). MMOH has a water molecule that hydrogen bonds to
Glu-114. This water is absent in both the cobalt-substituted mouse R2
and the diferrous E. coli R2 structure. The orientation of
the carboxylate ligands in the Co(II)-R2 mouse structure resembles the
MMOH counterparts more than the E. coli counterparts do.
This might contribute to the observed 3.4 Å Co1-Co2 distance in
Co(II)-R2 being closer to the 3.3 Å Fe1-Fe2 distance in MMOH than the
3.9 Å Fe1-Fe2 distance in E. coli R2 (Table II).
In the reduced form of MMOH, Glu-243 has a bidentate chelating mode to
Fe2 along with monodentate bridging between the iron atoms. This
µ-(
1,
2) coordination is suggested by
Eklund et al. (5), Andersson et al. (47), and
Merkx et al. (56) to be a well suited conformation for
binding of oxygen without any large structural changes in the
di-iron-oxygen cluster. Such an orientation is also found in the
reduced MMOH mimic mutant D84E of E. coli R2 (57). The dioxygen bound state has not been trapped in R2 because the iron-oxygen species is highly reactive. In the crystal structure of the
azide-soaked R2 E. coli mutant F208A/Y122F, azide binds to
the iron farthest away from tyrosine 122 (site 2), inducing a
carboxylate shift with Glu-238 (47). In analogy with how azide binds,
oxygen is suggested to bind at site 2 and induce this carboxylate
shift. The observed conformations of the carboxylate ligand, Glu-267 in
cobalt-substituted mouse R2 resembles the MMOH counterpart Glu-243 more
than the E. coli counterpart Glu-238, this might enhance the
protein affinity for oxygen binding. Also, in an oxidized structure of
manganese-substituted wild type E. coli R2, which probably contains a mixed valence state (Mn(II)Mn(III)), a
similar carboxylate shift is observed for the bridging carboxylate
ligand Glu-238 (26). The flexibility seen in Glu-238 makes this amino acid a key residue controlling oxygen activation in E. coli
R2. A preliminary three-dimensional structure of the reduced diferrous form of the mouse R2 protein confirms an orientation of ligand Glu-267
(data not shown) related to what is seen in the structures of the
counterparts of MMOH and the azide-soaked R2 E. coli mutant F208A/Y122F. The Co(II)-R2 structure could therefore serve as a
functional model for the very air-sensitive native diferrous enzyme.
Information on reduced R2 is essential for determining the mechanism of
oxygen activation in RNR and the radical generation cycle. Such
information will also aid the interpretation of spectroscopic data. For
example, the integer spin EPR signal of the diferrous form of mouse R2
observed either with perpendicular or parallel mode EPR has been
analyzed further by using saturation magnetization (44). The two
ferrous ions were assigned the same sign and magnitude for the
D values, indicating no or weak magnetic coupling in this study. The ferromagnetic coupling of the cobalt ions in Co(II)-R2 could
support another possible interpretation of the saturation magnetization
data assuming different signs of the D values and a weak
magnetic coupling between the ferrous irons. This is consistent with
magnetic circular dichroism analysis of both the diferrous form of R2
from E. coli (49) and mouse
(58).2
The stability of the iron/radical center is the most striking
difference between the mouse and the E. coli RNR R2 proteins (5, 7). The metal site of the mouse enzyme is labile at physiological
conditions, and a continuous supply of ferrous iron and oxygen is
needed to keep the enzyme fully active (21, 59, 60). The expression of
the mouse R2 protein is normally regulated by the cell cycle (61, 62).
A novel study indicated that during low oxygen (hypoxic) conditions the
human R2 protein might be an oncoprotein (63). The first step from
resting apoR2 in the cells is binding of Fe(II) to apoprotein and the
subsequent reaction with oxygen to form the stable tyrosyl radical and
the µ-oxo-diferric center. It was suggested recently by Bollinger and
co-workers (64) that the formation of the reactive Fe(II)-R2 complex is slower than the ensuing steps in which oxidized intermediates are
formed for mouse R2. In the E. coli R2 reaction, formation of the complex is slightly faster (5-10-fold) than the final
radical-producing step. The greater flexibility seen in all of the four
carboxylate ligands of mouse R2 compared with E. coli R2
might contribute to the low affinity for Fe(II) or Co(II) and to the
fact that the Fe(II) incorporation in mouse is slower. The same R2
mouse dimer has to carry out several redox cycles, as is also the case for MMOH. For the E. coli R2 enzyme the radical iron-oxygen
cluster is stable (20) when formed, and the protein does not have to be
reloaded with iron and oxygen again to create the radical needed for
the reduction of the substrate. This might be one of the reasons why
the bridging ligand Glu-267 in mouse has an orientation more suited for
oxygen activation than that of the wild type E. coli counterpart Glu-238.
By studying the Co(II) binding properties of apoR2 by EPR and x-ray
crystallography, we show that the cobalt ions bind to the well defined
metal ion binding sites of R2. We managed to increase the pH in the
mouse R2 crystals from the previously reported 4.7 to 6. The
cobalt-substituted structure of mouse R2 is a good tool for probing the
so far unknown coordination environment of the metal ions bound to
mouse R2 and is a useful structural model of the unstable and native
diferrous form of the protein (58). The observed orientation of the
bridging ligand Glu-267 might be important for the continuous
regeneration of the more exposed metal site of native mouse R2 compared
with the E. coli R2 enzyme. This ferromagnetically coupled
cobalt center might also have relevance for other native
cobalt-containing enzymes.
 |
ACKNOWLEDGEMENTS |
We are grateful for help by the staff at
beamlines ID14-1, ID14-3, and BM01A Swiss-Norwegian Beam Line (SNBL)
at ESRF, Grenoble. We thank Professor Lars Thelander, University of
Umeå, for generously providing the E. coli strain
overproducing mouse R2.
 |
FOOTNOTES |
*
This work was supported by grants from the Norwegian
Research Council (to K. K. A.), the Norwegian Cancer Society (to
K. K. A.), European Union Training and Mobility of Researchers
Program ERBMRFXCT980207, Iron-Oxygen Protein network (to K. K. A.),
and the synchrotron group of the Oslo region founded by the Norwegian Research Council.The costs of publication of this
article were defrayed in part by the
payment of page charges. The article
must therefore be hereby marked
"advertisement" in
accordance with 18 U.S.C. Section
1734 solely to indicate this fact.
The atomic coordinates and the structure factors (code 1h0o and 1h0n) have been deposited in the Protein Data Bank, Research Collaboratory for Structural Bioinformatics, Rutgers University, New Brunswick, NJ (http://www.rcsb.org/).
¶
To whom correspondence should be addressed. Tel.:
47-2285-6625; Fax: 47-2285-4443; E-mail:
k.k.andersson@biokjemi.uio.no.
Published, JBC Papers in Press, June 26, 2002, DOI 10.1074/jbc.M203358200
2
K. R. Strand, Y.-S. Yang, K. K. Andersson, and
E. I. Solomon, manuscript in preparation.
 |
ABBREVIATIONS |
The abbreviations used are:
RNR, ribonucleotide
reductase;
CNS, crystallography NMR software;
Co(II)-R2, cobalt-containing form of mouse R2;
MES, 4-morpholineethanesulfonic
acid;
MMOH, methane monooxygenase hydroxylase;
mT, millitesla.
 |
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