1g80

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[[Image:1g80.gif|left|200px]]
 
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==NMR SOLUTION STRUCTURE OF D(GCGTACGC)2==
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The line below this paragraph, containing "STRUCTURE_1g80", creates the "Structure Box" on the page.
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<StructureSection load='1g80' size='340' side='right'caption='[[1g80]]' scene=''>
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You may change the PDB parameter (which sets the PDB file loaded into the applet)
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== Structural highlights ==
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or the SCENE parameter (which sets the initial scene displayed when the page is loaded),
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<table><tr><td colspan='2'>[[1g80]] is a 2 chain structure. Full experimental information is available from [http://oca.weizmann.ac.il/oca-bin/ocashort?id=1G80 OCA]. For a <b>guided tour on the structure components</b> use [https://proteopedia.org/fgij/fg.htm?mol=1G80 FirstGlance]. <br>
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or leave the SCENE parameter empty for the default display.
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</td></tr><tr id='method'><td class="sblockLbl"><b>[[Empirical_models|Method:]]</b></td><td class="sblockDat" id="methodDat">Solution NMR</td></tr>
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<tr id='resources'><td class="sblockLbl"><b>Resources:</b></td><td class="sblockDat"><span class='plainlinks'>[https://proteopedia.org/fgij/fg.htm?mol=1g80 FirstGlance], [http://oca.weizmann.ac.il/oca-bin/ocaids?id=1g80 OCA], [https://pdbe.org/1g80 PDBe], [https://www.rcsb.org/pdb/explore.do?structureId=1g80 RCSB], [https://www.ebi.ac.uk/pdbsum/1g80 PDBsum], [https://prosat.h-its.org/prosat/prosatexe?pdbcode=1g80 ProSAT]</span></td></tr>
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{{STRUCTURE_1g80| PDB=1g80 | SCENE= }}
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</table>
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<div style="background-color:#fffaf0;">
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'''NMR SOLUTION STRUCTURE OF D(GCGTACGC)2'''
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== Publication Abstract from PubMed ==
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==Overview==
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The coupling between the conformational properties of double-stranded DNA and its internal dynamics has been examined. The solution structures of the isomeric DNA oligomers d(GCGTACGC)(2) (UM) and d(CGCTAGCG)(2) (CTSYM) were determined with (1)H NMR spectroscopy by utilizing distance restraints from total relaxation matrix analysis of NOESY cross-peak intensities in restrained molecular dynamics calculations. The root-mean-square deviation of the coordinates for the ensemble of structures was 0.13 A for UM and 0.49 A for CTSYM, with crystallographic equivalent R(c)=0.41 and 0.39 and sixth-root residual R(x)=0.11 and 0.10 for UM and CTSYM, respectively. Both UM and CTSYM are B-form with straight helical axes and show sequence-dependent variations in conformation. The internal dynamics of UM and CTSYM were previously determined by analysis of (13)C relaxation parameters in the context of the Lipari &amp; Szabo model-free formalism. Helical parameters for the two DNA oligomers were examined for linear correlations with the order parameters (S(2)) of groups of (13)C spins in base-pairs and dinucleotide units of UM and CTSYM. Correlations were found for six interstrand base-pair parameters tip, y-displacement, inclination, buckle and stretch with various combinations of S(2) for atoms in Watson-Crick base-pairs and for two inter-base-pair parameters, rise and roll with various combinations of S(2) for atoms in dinucleotides. The correlations for the interstrand base-pair helical parameters indicate that the conformations of the deoxyribose residues of each strand are dynamically coupled. Also, the inter-base-pair separation has a profound effect on the local internal motions available to the DNA, supporting the idea that rise is a principal degree of freedom for DNA conformational variability. The correlations indicate collective atomic motions of spins that may represent specific motional modes in DNA, and that base sequence has a predictable effect on the relative order of groups of spins both in the bases and in the deoxyribose ring of the DNA backbone. These observations suggest that an important functional outcome of DNA base sequence is the modulation of both the conformation and dynamic behavior of the DNA backbone.
The coupling between the conformational properties of double-stranded DNA and its internal dynamics has been examined. The solution structures of the isomeric DNA oligomers d(GCGTACGC)(2) (UM) and d(CGCTAGCG)(2) (CTSYM) were determined with (1)H NMR spectroscopy by utilizing distance restraints from total relaxation matrix analysis of NOESY cross-peak intensities in restrained molecular dynamics calculations. The root-mean-square deviation of the coordinates for the ensemble of structures was 0.13 A for UM and 0.49 A for CTSYM, with crystallographic equivalent R(c)=0.41 and 0.39 and sixth-root residual R(x)=0.11 and 0.10 for UM and CTSYM, respectively. Both UM and CTSYM are B-form with straight helical axes and show sequence-dependent variations in conformation. The internal dynamics of UM and CTSYM were previously determined by analysis of (13)C relaxation parameters in the context of the Lipari &amp; Szabo model-free formalism. Helical parameters for the two DNA oligomers were examined for linear correlations with the order parameters (S(2)) of groups of (13)C spins in base-pairs and dinucleotide units of UM and CTSYM. Correlations were found for six interstrand base-pair parameters tip, y-displacement, inclination, buckle and stretch with various combinations of S(2) for atoms in Watson-Crick base-pairs and for two inter-base-pair parameters, rise and roll with various combinations of S(2) for atoms in dinucleotides. The correlations for the interstrand base-pair helical parameters indicate that the conformations of the deoxyribose residues of each strand are dynamically coupled. Also, the inter-base-pair separation has a profound effect on the local internal motions available to the DNA, supporting the idea that rise is a principal degree of freedom for DNA conformational variability. The correlations indicate collective atomic motions of spins that may represent specific motional modes in DNA, and that base sequence has a predictable effect on the relative order of groups of spins both in the bases and in the deoxyribose ring of the DNA backbone. These observations suggest that an important functional outcome of DNA base sequence is the modulation of both the conformation and dynamic behavior of the DNA backbone.
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==About this Structure==
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Relationship of DNA structure to internal dynamics: correlation of helical parameters from NOE-based NMR solution structures of d(GCGTACGC)(2) and d(CGCTAGCG)(2) with (13)C order parameters implies conformational coupling in dinucleotide units.,Isaacs RJ, Spielmann HP J Mol Biol. 2001 Mar 23;307(2):525-40. PMID:11254380<ref>PMID:11254380</ref>
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Full crystallographic information is available from [http://oca.weizmann.ac.il/oca-bin/ocashort?id=1G80 OCA].
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==Reference==
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From MEDLINE&reg;/PubMed&reg;, a database of the U.S. National Library of Medicine.<br>
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Relationship of DNA structure to internal dynamics: correlation of helical parameters from NOE-based NMR solution structures of d(GCGTACGC)(2) and d(CGCTAGCG)(2) with (13)C order parameters implies conformational coupling in dinucleotide units., Isaacs RJ, Spielmann HP, J Mol Biol. 2001 Mar 23;307(2):525-40. PMID:[http://www.ncbi.nlm.nih.gov/pubmed/11254380 11254380]
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</div>
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[[Category: Isaacs, R J.]]
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<div class="pdbe-citations 1g80" style="background-color:#fffaf0;"></div>
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[[Category: Spielmann, H P.]]
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== References ==
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[[Category: C13 dynamic]]
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<references/>
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[[Category: Conformational exchange]]
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__TOC__
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[[Category: Deoxyribose conformation]]
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</StructureSection>
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[[Category: Dna]]
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[[Category: Large Structures]]
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[[Category: Helical parameter]]
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[[Category: Isaacs RJ]]
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[[Category: Hmt]]
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[[Category: Spielmann HP]]
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[[Category: Nmr]]
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[[Category: Order parameter]]
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[[Category: Phosphate conformation]]
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[[Category: Psoralen]]
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''Page seeded by [http://oca.weizmann.ac.il/oca OCA ] on Fri May 2 17:15:29 2008''
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NMR SOLUTION STRUCTURE OF D(GCGTACGC)2

PDB ID 1g80

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