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PDBsum entry 1d70
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References listed in PDB file
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Key reference
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Title
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Solution structure of a DNA octamer containing the pribnow box via restrained molecular dynamics simulation with distance and torsion angle constraints derived from two-Dimensional nuclear magnetic resonance spectral fitting.
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Authors
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U.Schmitz,
I.Sethson,
W.M.Egan,
T.L.James.
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Ref.
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J Mol Biol, 1992,
227,
510-531.
[DOI no: ]
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PubMed id
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Abstract
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The DNA octamer [d(GTATAATG].[(CATATTAC)], containing the prokaryotic upstream
consensus recognition sequence, has been examined via proton homonuclear
two-dimensional nuclear Overhauser effect (2D NOE) and double-quantum-filtered
correlation (2QF-COSY) spectra. All proton resonances, except those of H5' and
H5" protons, were assigned. A temperature dependence study of
one-dimensional nuclear magnetic resonance (NMR) spectra, rotating frame 2D NOE
spectroscopy (ROESY), and T1 rho measurements revealed an exchange process that
apparently is global in scope. Work at lower temperatures enabled a
determination of structural constraints that could be employed in determination
of a time-averaged structure. Simulations of the 2QF-COSY cross-peaks were
compared with experimental data, establishing scalar coupling constant ranges of
the individual sugar ring protons and hence pucker parameters for individual
deoxyribose rings. The rings exhibit a dynamic equilibrium of N and S-type
conformers with 80 to 100% populations of the latter. A program for iterative
complete relaxation matrix analysis of 2D NOE spectral intensities, MARDIGRAS,
was employed to give interproton distances for each mixing time. According to
the accuracy of the distance determination, upper and lower distance bounds were
chosen. The distance bounds define the size of a flat-well potential function
term, incorporated into the AMBER force-field, which was employed for restrained
molecular dynamics calculations. Torsion angle constraints in the form of a
flat-well potential were also constructed from the analysis of the sugar pucker
data. Several restrained molecular dynamics runs of 25 picoseconds were
performed, utilizing 184 experimental distance constraints and 80 torsion angle
constraints; three different starting structures were used: energy minimized
A-DNA, B-DNA, and wrinkled D-DNA, another member of the B-DNA family.
Convergence to similar structures obtained with root-mean-square deviations
between resulting structures of 0.37 to 0.92 A for the central hexamer of the
octamer. The average structure from the nine different molecular dynamics runs
was subjected to final restrained energy minimization. The resulting final
structure was in good agreement with the structures derived from different
molecular dynamics runs and exhibited a substantial improvement in the 2D NOE
sixth-root residual index in comparison with the starting structures. An
approximation of the structure in the terminal base-pairs, which displayed
experimental evidence of fraying, was made by maintaining the structure of the
inner four base-pairs and performing molecular dynamics simulations with the
experimental structural constraints observed for the termini.(ABSTRACT TRUNCATED
AT 400 WORDS)
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Figure 6.
Figure 6. Distibution f ntraresidue bold umbers)
and nterresidue plain numbers) NOE-drived distance
restraints for [d(GTATAATG]*[dCATATTAC)] (double-
headed rrows indicate ross-strand restraints nvolving
adenine H-2 and H-l' rotons etween denoted residues).
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Figure 9.
Figure 9. Stereo view of MD-FIN cyan) ncluding l elix axis (black) with a uperposition of the global helix
axis of rMD-A (red).
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The above figures are
reprinted
by permission from Elsevier:
J Mol Biol
(1992,
227,
510-531)
copyright 1992.
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Headers
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