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PDBsum entry 2vm3
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Oxidoreductase
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PDB id
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2vm3
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Contents |
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* Residue conservation analysis
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Enzyme class:
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E.C.1.7.2.1
- nitrite reductase (NO-forming).
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Reaction:
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nitric oxide + Fe(III)-[cytochrome c] + H2O = Fe(II)-[cytochrome c] + nitrite + 2 H+
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nitric oxide
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+
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Fe(III)-[cytochrome c]
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+
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H2O
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=
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Fe(II)-[cytochrome c]
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+
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nitrite
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+
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2
×
H(+)
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Cofactor:
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Cu cation or Fe cation; FAD
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Cu cation
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or
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Fe cation
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FAD
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Molecule diagrams generated from .mol files obtained from the
KEGG ftp site
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DOI no:
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J Mol Biol
378:353-361
(2008)
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PubMed id:
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Crystallography with online optical and X-ray absorption spectroscopies demonstrates an ordered mechanism in copper nitrite reductase.
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M.A.Hough,
S.V.Antonyuk,
R.W.Strange,
R.R.Eady,
S.S.Hasnain.
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ABSTRACT
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Nitrite reductases are key enzymes that perform the first committed step in the
denitrification process and reduce nitrite to nitric oxide. In copper nitrite
reductases, an electron is delivered from the type 1 copper (T1Cu) centre to the
type 2 copper (T2Cu) centre where catalysis occurs. Despite significant
structural and mechanistic studies, it remains controversial whether the
substrates, nitrite, electron and proton are utilised in an ordered or random
manner. We have used crystallography, together with online X-ray absorption
spectroscopy and optical spectroscopy, to show that X-rays rapidly and
selectively photoreduce the T1Cu centre, but that the T2Cu centre does not
photoreduce directly over a typical crystallographic data collection time.
Furthermore, internal electron transfer between the T1Cu and T2Cu centres does
not occur, and the T2Cu centre remains oxidised. These data unambiguously
demonstrate an 'ordered' mechanism in which electron transfer is gated by
binding of nitrite to the T2Cu. Furthermore, the use of online multiple
spectroscopic techniques shows their value in assessing radiation-induced redox
changes at different metal sites and demonstrates the importance of ensuring the
correct status of redox centres in a crystal structure determination. Here,
optical spectroscopy has shown a very high sensitivity for detecting the change
in T1Cu redox state, while X-ray absorption spectroscopy has reported on the
redox status of the T2Cu site, as this centre has no detectable optical
absorption.
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Selected figure(s)
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Figure 1.
Fig. 1. Combined spectroscopic and crystallographic
measurements on an AxNiR crystal. (a) Optical spectra of AxNiR
crystals. The crystal prior to X-ray exposure shows an
absorption spectrum with a peak at 595 nm, characteristic of
T1Cu(II) in oxidised AxNiR (solid line). This peak is no longer
present at the end of the collection of the first 1.90 Å
resolution crystallographic dataset (dotted line), indicating
that the T1Cu centre has been reduced during the experiment. (b)
XAS spectrum measured following the collection of the AxNiR2
crystal structure (dotted line). The solid line spectrum is from
a similar crystal, which had not been exposed to X-ray radiation
prior to the XAS scan. A small shift in the edge to lower energy
is apparent, consistent with photoreduction of the T1Cu site,
but the spectrum indicates that T2Cu is still in the Cu(II)
form. Inset: XAS spectra of the crystal following the AxNiR2
data collection (red line) compared with oxidised (solid black
line) and reduced (dashed black line) AxNiR solutions, and XAS
spectra of the ‘oxidised’ AxNiR crystal spectrum (blue line)
and a ‘fully reduced’ AxNiR crystal following exposure to a
dose of 3 × 10^7 Gy of 1.37 Å X-rays (green line) in
which the ‘edge-shoulder’ feature attributed to reduced T2Cu
is clearly present. Note that the ‘oxidised’ crystal has
undergone some X-ray-induced reduction of the T1Cu site during
the XAS data collection. The X-ray dose for solution data is
more than an order of magnitude less than on the
crystallographic beamline.
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Figure 4.
Fig. 4. Re-examination of nitrite-soaked crystal structures
of NiR. (a) Electron density maps suggesting the presence of
Cu-bound NO at the T2Cu site of nitrite-soaked AcNiR (PDB
accession code 2bwi^2). The 2F[o] − F[c] map contoured at 1σ
is shown in cyan, where the model includes 0.35 occupancy of
NO[2 ]^−, 0.25 occupancy of NO and 0.25 occupancy of water.
The F[o] − F[c] omit map contoured at 4σ, calculated by
omitting NO from the model, is shown in red, suggesting a
significant fraction of NO at this site. (b) The structure of
AcNiR with endogenously bound NO[2 ]^− and NO (PDB accession
code 2bw5^2). NO was removed from the model for the calculation
of the F[o] − F[c] omit map (red; contoured at 4σ). (c) 2F[o]
− F[c] electron density map contoured at 1σ showing
Cu-coordinated NO in the structure of nitrite-soaked RsNiR (PDB
accession code 2dws^31). NO is modelled with an occupancy of 0.7.
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The above figures are
reprinted
by permission from Elsevier:
J Mol Biol
(2008,
378,
353-361)
copyright 2008.
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Figures were
selected
by the author.
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Literature references that cite this PDB file's key reference
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PubMed id
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Reference
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D.H.Juers,
and
M.Weik
(2011).
Similarities and differences in radiation damage at 100 K versus 160 K in a crystal of thermolysin.
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J Synchrotron Radiat,
18,
329-337.
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R.L.Owen,
B.A.Yorke,
J.A.Gowdy,
and
A.R.Pearson
(2011).
Revealing low-dose radiation damage using single-crystal spectroscopy.
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J Synchrotron Radiat,
18,
367-373.
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E.F.Garman
(2010).
Radiation damage in macromolecular crystallography: what is it and why should we care?
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Acta Crystallogr D Biol Crystallogr,
66,
339-351.
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M.Weik,
and
J.P.Colletier
(2010).
Temperature-dependent macromolecular X-ray crystallography.
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Acta Crystallogr D Biol Crystallogr,
66,
437-446.
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P.Carpentier,
A.Royant,
M.Weik,
and
D.Bourgeois
(2010).
Raman-assisted crystallography suggests a mechanism of X-ray-induced disulfide radical formation and reparation.
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Structure,
18,
1410-1419.
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PDB codes:
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E.F.Garman,
and
C.Nave
(2009).
Radiation damage in protein crystals examined under various conditions by different methods.
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J Synchrotron Radiat,
16,
129-132.
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J.McGeehan,
R.B.Ravelli,
J.W.Murray,
R.L.Owen,
F.Cipriani,
S.McSweeney,
M.Weik,
and
E.F.Garman
(2009).
Colouring cryo-cooled crystals: online microspectrophotometry.
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J Synchrotron Radiat,
16,
163-172.
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R.L.Owen,
A.R.Pearson,
A.Meents,
P.Boehler,
V.Thominet,
and
C.Schulze-Briese
(2009).
A new on-axis multimode spectrometer for the macromolecular crystallography beamlines of the Swiss Light Source.
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J Synchrotron Radiat,
16,
173-182.
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S.Brenner,
D.J.Heyes,
S.Hay,
M.A.Hough,
R.R.Eady,
S.S.Hasnain,
and
N.S.Scrutton
(2009).
Demonstration of proton-coupled electron transfer in the copper-containing nitrite reductases.
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J Biol Chem,
284,
25973-25983.
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S.Ghosh,
A.Dey,
Y.Sun,
C.P.Scholes,
and
E.I.Solomon
(2009).
Spectroscopic and computational studies of nitrite reductase: proton induced electron transfer and backbonding contributions to reactivity.
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J Am Chem Soc,
131,
277-288.
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R.W.Strange,
and
M.C.Feiters
(2008).
Biological X-ray absorption spectroscopy (BioXAS): a valuable tool for the study of trace elements in the life sciences.
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Curr Opin Struct Biol,
18,
609-616.
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The most recent references are shown first.
Citation data come partly from CiteXplore and partly
from an automated harvesting procedure. Note that this is likely to be
only a partial list as not all journals are covered by
either method. However, we are continually building up the citation data
so more and more references will be included with time.
Where a reference describes a PDB structure, the PDB
codes are
shown on the right.
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