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- <a name="top"></a><h1 class="suptitle">supplementary materials</h1><br /><div class="buttonlinks"><a href="./index.html" target="_parent"><img src="../../../../../graphics/htmlborder.gif" alt="HTML version" align="top" border="0" /></a><a href="./at2615.pdf" ><img src="../../../../../graphics/pdfborder.gif" alt="pdf version" align="top" border="0" /></a><a href="http://scripts.iucr.org/cgi-bin/sendcif?at2615sup1" ><img src="../../../../../graphics/cifborder.gif" alt="cif file" align="top" border="0" /></a><a href="http://scripts.iucr.org/cgi-bin/sendcif?at2615sup1&Qmime=cif" ><img src="../../../../../graphics/3dviewborder.gif" alt="3d view" align="top" border="0" /></a><a href="./at2615Isup2.hkl" ><img src="../../../../../graphics/structurefactorsborder.gif" alt="structure factors" align="top" border="0" /></a><a href="./at2615sup0.html" ><img src="../../../../../graphics/supplementarymaterialsborder.gif" alt="supplementary materials" align="top" border="0" /></a><a href="./at2615checkcif.html" ><img src="../../../../../graphics/checkcifborder.gif" alt="CIF check report" align="top" border="0" /></a><a href="http://scripts.iucr.org/cgi-bin/citedin?at2615" ><img src="../../../../../graphics/citedinborder.gif" alt="cited in" align="top" border="0" /></a><a href="http://scripts.iucr.org/cgi-bin/similar?wordList=furyl%20or%20propen&from=at2615" ><img src="../../../../../graphics/similarpapersborder.gif" alt="similar papers" align="top" border="0" /></a> <a href="../../../../../../services/openaccess.html"><img src="../../../../../../logos/free.gif" alt="Open access" align="top" border="0" /></a></div><div class="bibline"><p><i>Acta Cryst.</i> (2008). E<b>64</b>, o1951 [ <font size="2"><a title="Open URL link" href="http://dx.doi.org/10.1107/S1600536808029152">doi:10.1107/S1600536808029152</a></font> ]</p></div>
- <h3>3-(5-Methyl-2-furyl)-1-(<span class="it"><i>p</i></span>-tolyl)-2-propen-1-one</h3><h3><a href="http://scripts.iucr.org/cgi-bin/citedin?search_on=name&author_name=Guo,%20H.-M.">H.-M. Guo</a>, <a href="http://scripts.iucr.org/cgi-bin/citedin?search_on=name&author_name=Wang,%20X.-B.">X.-B. Wang</a> and <a href="http://scripts.iucr.org/cgi-bin/citedin?search_on=name&author_name=Jian,%20F.-F.">F.-F. Jian</a></h3>
- <div class="abstract">
- <a name="abstract"></a>
- <div class="heading2">Abstract <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>The title compound, C<span class="inf"><sub>15</sub></span>H<span class="inf"><sub>14</sub></span>O<span class="inf"><sub>2</sub></span>, was prepared from 4-methylhypnone and 5-methylfurfural by Clasion-Schmidt condensation. All of the bond lengths and bond angles are in normal ranges. The dihedral angle formed by the benzene ring and furan ring is 5.31 (2).</p></div>
- <!-- endabstractdiv -->
- <div class="contentslist">
- <ul>
- <li class="comment"><a title="Comment" href="#comment">Comment</a></li>
- <li class="relatedliterature"><a title="Related literature" href="#relatedliterature">Related literature</a></li>
- <li class="experimental"><a title="Experimental" href="#experimental">Experimental</a></li>
- <li class="refinement"><a title="Refinement" href="#refinement">Refinement</a></li>
- <li class="computingdetails"><a title="Computing details" href="#computingdetails">Computing details</a></li>
- <li class="figures"><a title="Figures" href="#figures">Figures</a></li>
- <li><a title="(I)" href="#chemicalname1">3-(5-Methyl-2-furyl)-1-(<i>p</i>-tolyl)-2-propen-1-one </a><ul>
- <li><a title="Crystal data" href="#crystaldata1">Crystal data</a></li>
- <li><a title="Data collection" href="#datacollection1">Data collection</a></li>
- <li><a title="Refinement data" href="#refinementdata1">Refinement data</a></li>
- <li class="specialdetails"><a title="Special details" href="#specialdetails1">Special details</a></li>
- <li class="licoords"><a title="Fractional atomic coordinates" href="#fractionalatomiccoordinates1">Fractional atomic coordinates</a></li>
- <li class="liadps"><a title="Atomic displacement parameters" href="#atomicdisplacement1">Atomic displacement parameters</a></li>
- <li class="ligeomlong"><a title="Geometric parameters" href="#geometricparameters1">Geometric parameters</a></li>
- </ul></li>
- <li class="publreferences"><a title="References" href="#publreferences">References</a></li>
- </ul>
- </div>
- <!-- endcontentslistdiv -->
- <div class="comment">
- <a name="comment"></a>
- <div class="heading2">
- Comment <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>Among flavonoids, chalcones have been identified as interesting compounds having
- multiple biological actions which include antiinflammatory (Hsieh <i>et
- al.</i>,1998) and antioxidant (Anto <i>et al.</i>, 1994). Of
- particular
- interest, the effectiveness of chalcones against cancer has been investigated
- (De Vincenzo <i>et al.</i>, 2000; Dimmock <i>et al.</i>, 1998).
- As part of our
- search for new biologically active compounds we synthesized the title compound
- (I), and describe its structure here.</p><p>In the structure of (I) (Fig. 1), all of the bond lengths and bond angles fall
- in the normal range (Zhou, 2007; Ali <i>et al.</i>, 2005). The
- dihedral
- angles formed by the benzene ring and furan ring is 5.31 (2)°. There are some
- weak C—H···O hydrogen bonds in the crystal structure (Table 1).</p>
- </div>
- <!-- endcommentdiv -->
- <div class="relatedliterature">
- <a name="relatedliterature"></a>
- <div class="heading2">
- Related literature <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>For the biological activity of chalcones, see: Hsieh <i>et al.</i>
- (1998);</p><p>Anto <i>et al.</i> (1994). For the effectiveness of chalcones against
- cancer,
- see: De Vincenzo <i>et al.</i> (2000); Dimmock <i>et al.</i>
- (1998).</p><p>For bond-length and angle data, see: Ali <i>et al.</i> (2005); Zhou
- (2007).</p>
- </div>
- <!-- endrelatedliteraturediv -->
- <div class="experimental">
- <a name="experimental"></a>
- <div class="heading2">
- Experimental <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>A mixture of the 5-methylfurfural (0.02 mol), and 4-methylhypnone (0.02 mol)
- and 10% NaOH (10 ml) was stirred in ethanol (30 mL) for 3 h to afford the
- title compound (yield 85%). Single crystals suitable for X-ray measurements
- were obtained by recrystallization from ethanol at room temperature.</p>
- </div>
- <!-- endexperimentaldiv -->
- <div class="refinement">
- <a name="refinement"></a>
- <div class="heading2">
- Refinement <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>H atoms were fixed geometrically and allowed to ride on their attached atoms,
- with C—H distances = 0.93-0.96 Å, and with
- <i>U</i><sub>iso</sub>=1.2–1.5<i>U</i><sub>eq</sub>.</p>
- </div>
- <!-- endrefinementdiv -->
- <div class="computingdetails">
- <a name="computingdetails"></a>
- <div class="heading2">
- Computing details <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).</p>
- </div>
- <!-- endcomputingdetailsdiv -->
- <div class="schemes">
- <a href="./at2615scheme1.gif"></a>
- </div>
- <!-- endschemesdiv -->
- <div class="figures">
- <div class="tablewrap">
- <a name="figures"></a>
- <div class="heading2">
- Figures <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><table style="table-layout:fixed" width="100%" class="nodecs">
- <colgroup span="2">
- <col width="110"></col>
- <col></col>
- </colgroup>
- <tr><td class="nodecs" align="center" width="110">
- <a href="./at2615fig1.html"><img width="100" src="./at2615fig1thm.gif" alt="[Figure 1]" align="middle"/></a>
- <br /><a href="./at2615fig2.html"><img width="100" src="./at2615fig2thm.gif" alt="[Figure 2]" align="middle"/></a>
- <br /></td><td class="nodecs" valign="middle" >The structure of the title compound showing 30% probability displacement
- ellipsoids and the atom-numbering scheme.</td></tr></table>
- </div>
- </div>
- <!-- endfiguresdiv -->
- <div class="datablock1">
- <div class="heading2">
- <a name="chemicalname1"></a>3-(5-Methyl-2-furyl)-1-(<i>p</i>-tolyl)-2-propen-1-one <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div -->
- <div class="tablewrapcrystaldatalong">
- <a name="crystaldata1"></a><span class="heading3">Crystal data</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >C<sub>15</sub>H<sub>14</sub>O<sub>2</sub></td><td width="50%" class="tabledata" ><i>F</i>(000) = 480</td></tr><tr><td width="50%" class="tabledata" ><i>M</i><i><sub>r</sub></i> = 226.26</td><td width="50%" class="tabledata" ><i>D</i><sub>x</sub> = 1.206 Mg m<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >Monoclinic, <i>P</i>2<sub>1</sub>/<i>c</i></td><td width="50%" class="tabledata" >Mo <i>K</i><span style="font-family:Times">α</span> radiation, <span style="font-family:Times">λ</span> = 0.71073 Å</td></tr><tr><td width="50%" class="tabledata" >Hall symbol: -P 2ybc</td><td width="50%" class="tabledata" >Cell parameters from 1770 reflections</td></tr><tr><td width="50%" class="tabledata" ><i>a</i> = 8.0394 (8) Å</td><td width="50%" class="tabledata" ><span style="font-family:Times">θ</span> = 0.4–27.5°</td></tr><tr><td width="50%" class="tabledata" ><i>b</i> = 17.0278 (17) Å</td><td width="50%" class="tabledata" >µ = 0.08 mm<span style="font-family:Times"><sup>−</sup></span><sup>1</sup></td></tr><tr><td width="50%" class="tabledata" ><i>c</i> = 10.6550 (8) Å</td><td width="50%" class="tabledata" ><i>T</i> = 293 K</td></tr><tr><td width="50%" class="tabledata" ><span style="font-family:Times">β</span> = 121.347 (6)°</td><td width="50%" class="tabledata" >Bar, colourless</td></tr><tr><td width="50%" class="tabledata" ><i>V</i> = 1245.7 (2) Å<sup>3</sup></td><td width="50%" class="tabledata" >0.2 × 0.2 × 0.2 mm</td></tr><tr><td width="50%" class="tabledata" ><i>Z</i> = 4</td><td width="50%" class="tabledata" ></td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewrapcrystaldatalongdiv -->
- <div class="tablewrapdatacollectionlong">
- <a name="datacollection1"></a><span class="heading3">Data collection</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >Bruker SMART CCD area-detector <br />diffractometer</td><td width="50%" class="tabledata" >1706 reflections with <i>I</i> > 2<span style="font-family:Times">σ</span>(<i>I</i>)</td></tr><tr><td width="50%" class="tabledata" >Radiation source: fine-focus sealed tube</td><td width="50%" class="tabledata" ><i>R</i><sub>int</sub> = 0.026</td></tr><tr><td width="50%" class="tabledata" >graphite</td><td width="50%" class="tabledata" ><span style="font-family:Times">θ</span><sub>max</sub> = 28.2°, <span style="font-family:Times">θ</span><sub>min</sub> = 2.4°</td></tr><tr><td width="50%" class="tabledata" >phi and <span style="font-family:Times">ω</span> scans</td><td width="50%" class="tabledata" ><i>h</i> = <span style="font-family:Times">−</span>8<span style="font-family:Times">→</span>10</td></tr><tr><td width="50%" class="tabledata" >7980 measured reflections</td><td width="50%" class="tabledata" ><i>k</i> = <span style="font-family:Times">−</span>17<span style="font-family:Times">→</span>22</td></tr><tr><td width="50%" class="tabledata" >2985 independent reflections</td><td width="50%" class="tabledata" ><i>l</i> = <span style="font-family:Times">−</span>13<span style="font-family:Times">→</span>13</td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewrapdatacollectionlongdiv -->
- <div class="tablewraprefinementdatalong">
- <a name="refinementdata1"></a><span class="heading3">Refinement</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >Refinement on <i>F</i><sup>2</sup></td><td width="50%" class="tabledata" >Secondary atom site location: difference Fourier map</td></tr><tr><td width="50%" class="tabledata" >Least-squares matrix: full</td><td width="50%" class="tabledata" >Hydrogen site location: inferred from neighbouring sites</td></tr><tr><td width="50%" class="tabledata" ><i>R</i>[<i>F</i><sup>2</sup> > 2<span style="font-family:Times">σ</span>(<i>F</i><sup>2</sup>)] = 0.043</td><td width="50%" class="tabledata" >H-atom parameters constrained</td></tr><tr><td width="50%" class="tabledata" ><i>wR</i>(<i>F</i><sup>2</sup>) = 0.136</td><td width="50%" class="tabledata" > <i>w</i> = 1/[<span style="font-family:Times">σ</span><sup>2</sup>(<i>F</i><sub>o</sub><sup>2</sup>) + (0.0613<i>P</i>)<sup>2</sup> + 0.0738<i>P</i>] <br />where <i>P</i> = (<i>F</i><sub>o</sub><sup>2</sup> + 2<i>F</i><sub>c</sub><sup>2</sup>)/3</td></tr><tr><td width="50%" class="tabledata" ><i>S</i> = 1.02</td><td width="50%" class="tabledata" >(Δ/<span style="font-family:Times">σ</span>)<sub>max</sub> < 0.001</td></tr><tr><td width="50%" class="tabledata" >2985 reflections</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>max</sub> = 0.17 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >155 parameters</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>min</sub> = <span style="font-family:Times">−</span>0.11 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >0 restraints</td><td width="50%" class="tabledata" >Extinction correction: SHELXL, Fc<sup>*</sup>=kFc[1+0.001xFc<sup>2</sup><span style="font-family:Times">λ</span><sup>3</sup>/sin(2<span style="font-family:Times">θ</span>)]<sup>-1/4</sup></td></tr><tr><td width="50%" class="tabledata" >Primary atom site location: structure-invariant direct methods</td><td width="50%" class="tabledata" >Extinction coefficient: 0.011 (3)</td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewraprefinementdatalongdiv -->
- <div class="tablewrapcrystaldatashort">
- <a name="crystaldata1"></a><span class="heading3">Crystal data</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >C<sub>15</sub>H<sub>14</sub>O<sub>2</sub></td><td width="50%" class="tabledata" ><i>V</i> = 1245.7 (2) Å<sup>3</sup></td></tr><tr><td width="50%" class="tabledata" ><i>M</i><i><sub>r</sub></i> = 226.26</td><td width="50%" class="tabledata" ><i>Z</i> = 4</td></tr><tr><td width="50%" class="tabledata" >Monoclinic, <i>P</i>2<sub>1</sub>/<i>c</i></td><td width="50%" class="tabledata" >Mo <i>K</i><span style="font-family:Times">α</span> radiation</td></tr><tr><td width="50%" class="tabledata" ><i>a</i> = 8.0394 (8) Å</td><td width="50%" class="tabledata" >µ = 0.08 mm<span style="font-family:Times"><sup>−</sup></span><sup>1</sup></td></tr><tr><td width="50%" class="tabledata" ><i>b</i> = 17.0278 (17) Å</td><td width="50%" class="tabledata" ><i>T</i> = 293 K</td></tr><tr><td width="50%" class="tabledata" ><i>c</i> = 10.6550 (8) Å</td><td width="50%" class="tabledata" >0.2 × 0.2 × 0.2 mm</td></tr><tr><td width="50%" class="tabledata" ><span style="font-family:Times">β</span> = 121.347 (6)°</td><td width="50%" class="tabledata" ></td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewrapcrystaldatashortdiv -->
- <div class="tablewrapdatacollectionshort">
- <a name="datacollection1"></a><span class="heading3">Data collection</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >Bruker SMART CCD area-detector <br />diffractometer</td><td width="50%" class="tabledata" >1706 reflections with <i>I</i> > 2<span style="font-family:Times">σ</span>(<i>I</i>)</td></tr><tr><td width="50%" class="tabledata" >7980 measured reflections</td><td width="50%" class="tabledata" ><i>R</i><sub>int</sub> = 0.026</td></tr><tr><td width="50%" class="tabledata" >2985 independent reflections</td><td width="50%" class="tabledata" ><span style="font-family:Times">θ</span><sub>max</sub> = 28.2°</td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewrapdatacollectionshortdiv -->
- <div class="tablewraprefinementdatashort">
- <a name="refinementdata1"></a><span class="heading3">Refinement</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" ><i>R</i>[<i>F</i><sup>2</sup> > 2<span style="font-family:Times">σ</span>(<i>F</i><sup>2</sup>)] = 0.043</td><td width="50%" class="tabledata" >H-atom parameters constrained</td></tr><tr><td width="50%" class="tabledata" ><i>wR</i>(<i>F</i><sup>2</sup>) = 0.136</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>max</sub> = 0.17 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" ><i>S</i> = 1.02</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>min</sub> = <span style="font-family:Times">−</span>0.11 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >2985 reflections</td><td width="50%" class="tabledata" >Absolute structure: ?</td></tr><tr><td width="50%" class="tabledata" >155 parameters</td><td width="50%" class="tabledata" >Flack parameter: ?</td></tr><tr><td width="50%" class="tabledata" >0 restraints</td><td width="50%" class="tabledata" >Rogers parameter: ?</td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewraprefinementdatashortdiv -->
- <div class="specialdetails">
- <div class="tablewrap">
- <a name="specialdetails1"></a><span class="heading3">Special details</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- <table style="table-layout:fixed" width="100%" class="tabledata">
- <tr><td class="tabledata"><p><b>Geometry</b>. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes)
- are estimated using the full covariance matrix. The cell e.s.d.'s are taken
- into account individually in the estimation of e.s.d.'s in distances, angles
- and torsion angles; correlations between e.s.d.'s in cell parameters are only
- used when they are defined by crystal symmetry. An approximate (isotropic)
- treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s.
- planes.</p></td></tr>
- <tr><td class="tabledata"><p><b>Refinement</b>. Refinement of <i>F</i><sup>2</sup> against ALL reflections. The weighted <i>R</i>-factor
- <i>wR</i> and goodness of fit <i>S</i> are based on <i>F</i><sup>2</sup>, conventional
- <i>R</i>-factors <i>R</i> are based on <i>F</i>, with <i>F</i> set to zero for
- negative <i>F</i><sup>2</sup>. The threshold expression of <i>F</i><sup>2</sup> >
- <span style="font-family:Times">σ</span>(<i>F</i><sup>2</sup>) is used only for calculating <i>R</i>-factors(gt) <i>etc</i>.
- and is not relevant to the choice of reflections for refinement.
- <i>R</i>-factors based on <i>F</i><sup>2</sup> are statistically about twice as large
- as those based on <i>F</i>, and <i>R</i>- factors based on ALL data will be
- even larger.</p></td></tr></table>
- </div>
- </div>
- <!-- endspecialdetailsdiv -->
- <div class="tablewrapcoords">
- <a name="fractionalatomiccoordinates1"></a> <span class="heading3">Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å<sup>2</sup>)</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="100%" summary="" class="tabledata"><tr><td class="tabledata" > </td><td class="tabledata" ><i>x</i></td><td class="tabledata" ><i>y</i></td><td class="tabledata" ><i>z</i></td><td class="tabledata" ><i>U</i><sub>iso</sub>*/<i>U</i><sub>eq</sub></td><td class="tabledata" ></td></tr><tr><td class="tabledata" >O1</td><td class="tabledata" ><span style="font-family:Times">−</span>0.32694 (14)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.22464 (6)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.56944 (10)</td><td class="tabledata" >0.0574 (3)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >O2</td><td class="tabledata" >0.14482 (19)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.01503 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.24561 (13)</td><td class="tabledata" >0.0810 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C1</td><td class="tabledata" ><span style="font-family:Times">−</span>0.5507 (3)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.33021 (11)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.7020 (2)</td><td class="tabledata" >0.0892 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1A</td><td class="tabledata" ><span style="font-family:Times">−</span>0.6226</td><td class="tabledata" ><span style="font-family:Times">−</span>0.3521</td><td class="tabledata" ><span style="font-family:Times">−</span>0.7991</td><td class="tabledata" >0.134*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1B</td><td class="tabledata" ><span style="font-family:Times">−</span>0.6395</td><td class="tabledata" ><span style="font-family:Times">−</span>0.3140</td><td class="tabledata" ><span style="font-family:Times">−</span>0.6722</td><td class="tabledata" >0.134*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1C</td><td class="tabledata" ><span style="font-family:Times">−</span>0.4632</td><td class="tabledata" ><span style="font-family:Times">−</span>0.3691</td><td class="tabledata" ><span style="font-family:Times">−</span>0.6347</td><td class="tabledata" >0.134*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C2</td><td class="tabledata" ><span style="font-family:Times">−</span>0.4379 (2)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.26168 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.70182 (17)</td><td class="tabledata" >0.0582 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C3</td><td class="tabledata" ><span style="font-family:Times">−</span>0.4181 (2)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.22529 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.80412 (18)</td><td class="tabledata" >0.0656 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H3A</td><td class="tabledata" ><span style="font-family:Times">−</span>0.4779</td><td class="tabledata" ><span style="font-family:Times">−</span>0.2393</td><td class="tabledata" ><span style="font-family:Times">−</span>0.9026</td><td class="tabledata" >0.079*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C4</td><td class="tabledata" ><span style="font-family:Times">−</span>0.2899 (3)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.16169 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.73553 (18)</td><td class="tabledata" >0.0665 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H4A</td><td class="tabledata" ><span style="font-family:Times">−</span>0.2497</td><td class="tabledata" ><span style="font-family:Times">−</span>0.1259</td><td class="tabledata" ><span style="font-family:Times">−</span>0.7804</td><td class="tabledata" >0.080*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C5</td><td class="tabledata" ><span style="font-family:Times">−</span>0.2364 (2)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.16241 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.59293 (16)</td><td class="tabledata" >0.0545 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C6</td><td class="tabledata" ><span style="font-family:Times">−</span>0.1121 (2)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.11417 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.47132 (18)</td><td class="tabledata" >0.0590 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H6A</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0541</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0723</td><td class="tabledata" ><span style="font-family:Times">−</span>0.4903</td><td class="tabledata" >0.071*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C7</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0686 (2)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.12165 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.33318 (17)</td><td class="tabledata" >0.0577 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H7A</td><td class="tabledata" ><span style="font-family:Times">−</span>0.1275</td><td class="tabledata" ><span style="font-family:Times">−</span>0.1613</td><td class="tabledata" ><span style="font-family:Times">−</span>0.3099</td><td class="tabledata" >0.069*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C8</td><td class="tabledata" >0.0699 (2)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.06898 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.21687 (17)</td><td class="tabledata" >0.0591 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C9</td><td class="tabledata" >0.1224 (2)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.08231 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.06208 (16)</td><td class="tabledata" >0.0558 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C10</td><td class="tabledata" >0.0379 (2)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.13889 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.02027 (18)</td><td class="tabledata" >0.0683 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H10A</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0550</td><td class="tabledata" ><span style="font-family:Times">−</span>0.1724</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0908</td><td class="tabledata" >0.082*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C11</td><td class="tabledata" >0.0888 (3)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.14648 (11)</td><td class="tabledata" >0.1236 (2)</td><td class="tabledata" >0.0761 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H11A</td><td class="tabledata" >0.0287</td><td class="tabledata" ><span style="font-family:Times">−</span>0.1850</td><td class="tabledata" >0.1483</td><td class="tabledata" >0.091*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C12</td><td class="tabledata" >0.2260 (3)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.09881 (10)</td><td class="tabledata" >0.23223 (19)</td><td class="tabledata" >0.0701 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C13</td><td class="tabledata" >0.3126 (3)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.04334 (11)</td><td class="tabledata" >0.1911 (2)</td><td class="tabledata" >0.0802 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H13A</td><td class="tabledata" >0.4077</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0108</td><td class="tabledata" >0.2624</td><td class="tabledata" >0.096*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C14</td><td class="tabledata" >0.2624 (3)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.03474 (10)</td><td class="tabledata" >0.04727 (19)</td><td class="tabledata" >0.0734 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H14A</td><td class="tabledata" >0.3235</td><td class="tabledata" >0.0036</td><td class="tabledata" >0.0231</td><td class="tabledata" >0.088*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C15</td><td class="tabledata" >0.2803 (3)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.10657 (13)</td><td class="tabledata" >0.3896 (2)</td><td class="tabledata" >0.0940 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H15A</td><td class="tabledata" >0.2064</td><td class="tabledata" ><span style="font-family:Times">−</span>0.1483</td><td class="tabledata" >0.3979</td><td class="tabledata" >0.141*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H15B</td><td class="tabledata" >0.2525</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0582</td><td class="tabledata" >0.4215</td><td class="tabledata" >0.141*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H15C</td><td class="tabledata" >0.4168</td><td class="tabledata" ><span style="font-family:Times">−</span>0.1181</td><td class="tabledata" >0.4500</td><td class="tabledata" >0.141*</td><td class="tabledata" ></td></tr></table>
- </div>
- <!-- endtablewrapcoordsdiv -->
- <div class="tablewrapadps">
- <a name="atomicdisplacement1"></a> <span class="heading3">Atomic displacement parameters (Å<sup>2</sup>)</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="100%" summary="" class="tabledata"><tr><td class="tabledata" > </td><td class="tabledata" ><i>U</i><sup>11</sup></td><td class="tabledata" ><i>U</i><sup>22</sup></td><td class="tabledata" ><i>U</i><sup>33</sup></td><td class="tabledata" ><i>U</i><sup>12</sup></td><td class="tabledata" ><i>U</i><sup>13</sup></td><td class="tabledata" ><i>U</i><sup>23</sup></td></tr><tr><td class="tabledata" >O1</td><td class="tabledata" >0.0672 (6)</td><td class="tabledata" >0.0599 (6)</td><td class="tabledata" >0.0517 (6)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0065 (5)</td><td class="tabledata" >0.0355 (5)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0031 (5)</td></tr><tr><td class="tabledata" >O2</td><td class="tabledata" >0.1026 (9)</td><td class="tabledata" >0.0684 (7)</td><td class="tabledata" >0.0750 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0265 (7)</td><td class="tabledata" >0.0484 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0067 (6)</td></tr><tr><td class="tabledata" >C1</td><td class="tabledata" >0.1063 (15)</td><td class="tabledata" >0.0854 (13)</td><td class="tabledata" >0.0788 (13)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0308 (11)</td><td class="tabledata" >0.0503 (11)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0160 (10)</td></tr><tr><td class="tabledata" >C2</td><td class="tabledata" >0.0607 (9)</td><td class="tabledata" >0.0627 (9)</td><td class="tabledata" >0.0534 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0021 (7)</td><td class="tabledata" >0.0313 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0068 (7)</td></tr><tr><td class="tabledata" >C3</td><td class="tabledata" >0.0744 (10)</td><td class="tabledata" >0.0738 (10)</td><td class="tabledata" >0.0502 (9)</td><td class="tabledata" >0.0001 (9)</td><td class="tabledata" >0.0335 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0025 (8)</td></tr><tr><td class="tabledata" >C4</td><td class="tabledata" >0.0812 (11)</td><td class="tabledata" >0.0691 (10)</td><td class="tabledata" >0.0588 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0043 (9)</td><td class="tabledata" >0.0430 (9)</td><td class="tabledata" >0.0049 (8)</td></tr><tr><td class="tabledata" >C5</td><td class="tabledata" >0.0587 (9)</td><td class="tabledata" >0.0546 (9)</td><td class="tabledata" >0.0566 (9)</td><td class="tabledata" >0.0013 (7)</td><td class="tabledata" >0.0345 (7)</td><td class="tabledata" >0.0025 (7)</td></tr><tr><td class="tabledata" >C6</td><td class="tabledata" >0.0630 (9)</td><td class="tabledata" >0.0544 (9)</td><td class="tabledata" >0.0658 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0025 (7)</td><td class="tabledata" >0.0379 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0015 (7)</td></tr><tr><td class="tabledata" >C7</td><td class="tabledata" >0.0614 (9)</td><td class="tabledata" >0.0544 (9)</td><td class="tabledata" >0.0602 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0044 (7)</td><td class="tabledata" >0.0337 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0019 (7)</td></tr><tr><td class="tabledata" >C8</td><td class="tabledata" >0.0624 (9)</td><td class="tabledata" >0.0513 (9)</td><td class="tabledata" >0.0649 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0011 (7)</td><td class="tabledata" >0.0341 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0021 (7)</td></tr><tr><td class="tabledata" >C9</td><td class="tabledata" >0.0567 (9)</td><td class="tabledata" >0.0517 (8)</td><td class="tabledata" >0.0568 (9)</td><td class="tabledata" >0.0029 (7)</td><td class="tabledata" >0.0280 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0030 (7)</td></tr><tr><td class="tabledata" >C10</td><td class="tabledata" >0.0672 (10)</td><td class="tabledata" >0.0725 (11)</td><td class="tabledata" >0.0608 (11)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0082 (8)</td><td class="tabledata" >0.0302 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0020 (8)</td></tr><tr><td class="tabledata" >C11</td><td class="tabledata" >0.0758 (12)</td><td class="tabledata" >0.0849 (12)</td><td class="tabledata" >0.0676 (12)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0017 (10)</td><td class="tabledata" >0.0374 (10)</td><td class="tabledata" >0.0088 (9)</td></tr><tr><td class="tabledata" >C12</td><td class="tabledata" >0.0721 (11)</td><td class="tabledata" >0.0747 (11)</td><td class="tabledata" >0.0597 (11)</td><td class="tabledata" >0.0223 (9)</td><td class="tabledata" >0.0315 (9)</td><td class="tabledata" >0.0060 (8)</td></tr><tr><td class="tabledata" >C13</td><td class="tabledata" >0.0872 (13)</td><td class="tabledata" >0.0762 (12)</td><td class="tabledata" >0.0610 (11)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0049 (10)</td><td class="tabledata" >0.0273 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0138 (9)</td></tr><tr><td class="tabledata" >C14</td><td class="tabledata" >0.0856 (12)</td><td class="tabledata" >0.0631 (10)</td><td class="tabledata" >0.0683 (12)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0131 (9)</td><td class="tabledata" >0.0378 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0096 (8)</td></tr><tr><td class="tabledata" >C15</td><td class="tabledata" >0.1016 (14)</td><td class="tabledata" >0.1128 (16)</td><td class="tabledata" >0.0632 (12)</td><td class="tabledata" >0.0270 (12)</td><td class="tabledata" >0.0398 (11)</td><td class="tabledata" >0.0108 (10)</td></tr></table>
- </div>
- <!-- endtablewrapadpsdiv -->
- <div class="tablewrapgeomlong">
- <a name="geometricparameters1"></a> <span class="heading3">Geometric parameters (Å, °)</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><!-- startgeom --><table style="table-layout:fixed" width="100%" summary="" class="tabledata">
- <colgroup span="4">
- <col width="30%"></col>
- <col width="20%"></col>
- <col width="30%"></col>
- <col width="20%"></col>
- </colgroup>
- <tr><td width="30%" class="tabledata" >O1—C2</td><td width="20%" class="tabledata" >1.3689 (17)</td><td width="30%" class="tabledata" >C7—H7A</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >O1—C5</td><td width="20%" class="tabledata" >1.3800 (16)</td><td width="30%" class="tabledata" >C8—C9</td><td width="20%" class="tabledata" >1.492 (2)</td></tr><tr><td width="30%" class="tabledata" >O2—C8</td><td width="20%" class="tabledata" >1.2218 (17)</td><td width="30%" class="tabledata" >C9—C10</td><td width="20%" class="tabledata" >1.379 (2)</td></tr><tr><td width="30%" class="tabledata" >C1—C2</td><td width="20%" class="tabledata" >1.477 (2)</td><td width="30%" class="tabledata" >C9—C14</td><td width="20%" class="tabledata" >1.384 (2)</td></tr><tr><td width="30%" class="tabledata" >C1—H1A</td><td width="20%" class="tabledata" >0.9600</td><td width="30%" class="tabledata" >C10—C11</td><td width="20%" class="tabledata" >1.372 (2)</td></tr><tr><td width="30%" class="tabledata" >C1—H1B</td><td width="20%" class="tabledata" >0.9600</td><td width="30%" class="tabledata" >C10—H10A</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >C1—H1C</td><td width="20%" class="tabledata" >0.9600</td><td width="30%" class="tabledata" >C11—C12</td><td width="20%" class="tabledata" >1.374 (2)</td></tr><tr><td width="30%" class="tabledata" >C2—C3</td><td width="20%" class="tabledata" >1.333 (2)</td><td width="30%" class="tabledata" >C11—H11A</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >C3—C4</td><td width="20%" class="tabledata" >1.409 (2)</td><td width="30%" class="tabledata" >C12—C13</td><td width="20%" class="tabledata" >1.374 (2)</td></tr><tr><td width="30%" class="tabledata" >C3—H3A</td><td width="20%" class="tabledata" >0.9300</td><td width="30%" class="tabledata" >C12—C15</td><td width="20%" class="tabledata" >1.503 (2)</td></tr><tr><td width="30%" class="tabledata" >C4—C5</td><td width="20%" class="tabledata" >1.347 (2)</td><td width="30%" class="tabledata" >C13—C14</td><td width="20%" class="tabledata" >1.374 (2)</td></tr><tr><td width="30%" class="tabledata" >C4—H4A</td><td width="20%" class="tabledata" >0.9300</td><td width="30%" class="tabledata" >C13—H13A</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >C5—C6</td><td width="20%" class="tabledata" >1.416 (2)</td><td width="30%" class="tabledata" >C14—H14A</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >C6—C7</td><td width="20%" class="tabledata" >1.330 (2)</td><td width="30%" class="tabledata" >C15—H15A</td><td width="20%" class="tabledata" >0.9600</td></tr><tr><td width="30%" class="tabledata" >C6—H6A</td><td width="20%" class="tabledata" >0.9300</td><td width="30%" class="tabledata" >C15—H15B</td><td width="20%" class="tabledata" >0.9600</td></tr><tr><td width="30%" class="tabledata" >C7—C8</td><td width="20%" class="tabledata" >1.464 (2)</td><td width="30%" class="tabledata" >C15—H15C</td><td width="20%" class="tabledata" >0.9600</td></tr><tr><td width="25%" class="tabledata" ></td><td width="25%" class="tabledata" ></td><td width="25%" class="tabledata" ></td><td width="25%" class="tabledata" ></td></tr><tr><td width="30%" class="tabledata" >C2—O1—C5</td><td width="20%" class="tabledata" >106.82 (11)</td><td width="30%" class="tabledata" >O2—C8—C9</td><td width="20%" class="tabledata" >119.91 (14)</td></tr><tr><td width="30%" class="tabledata" >C2—C1—H1A</td><td width="20%" class="tabledata" >109.5</td><td width="30%" class="tabledata" >C7—C8—C9</td><td width="20%" class="tabledata" >119.74 (14)</td></tr><tr><td width="30%" class="tabledata" >C2—C1—H1B</td><td width="20%" class="tabledata" >109.5</td><td width="30%" class="tabledata" >C10—C9—C14</td><td width="20%" class="tabledata" >117.28 (15)</td></tr><tr><td width="30%" class="tabledata" >H1A—C1—H1B</td><td width="20%" class="tabledata" >109.5</td><td width="30%" class="tabledata" >C10—C9—C8</td><td width="20%" class="tabledata" >124.02 (14)</td></tr><tr><td width="30%" class="tabledata" >C2—C1—H1C</td><td width="20%" class="tabledata" >109.5</td><td width="30%" class="tabledata" >C14—C9—C8</td><td width="20%" class="tabledata" >118.69 (15)</td></tr><tr><td width="30%" class="tabledata" >H1A—C1—H1C</td><td width="20%" class="tabledata" >109.5</td><td width="30%" class="tabledata" >C11—C10—C9</td><td width="20%" class="tabledata" >121.08 (16)</td></tr><tr><td width="30%" class="tabledata" >H1B—C1—H1C</td><td width="20%" class="tabledata" >109.5</td><td width="30%" class="tabledata" >C11—C10—H10A</td><td width="20%" class="tabledata" >119.5</td></tr><tr><td width="30%" class="tabledata" >C3—C2—O1</td><td width="20%" class="tabledata" >109.70 (14)</td><td width="30%" class="tabledata" >C9—C10—H10A</td><td width="20%" class="tabledata" >119.5</td></tr><tr><td width="30%" class="tabledata" >C3—C2—C1</td><td width="20%" class="tabledata" >134.46 (16)</td><td width="30%" class="tabledata" >C10—C11—C12</td><td width="20%" class="tabledata" >121.87 (17)</td></tr><tr><td width="30%" class="tabledata" >O1—C2—C1</td><td width="20%" class="tabledata" >115.83 (13)</td><td width="30%" class="tabledata" >C10—C11—H11A</td><td width="20%" class="tabledata" >119.1</td></tr><tr><td width="30%" class="tabledata" >C2—C3—C4</td><td width="20%" class="tabledata" >107.42 (15)</td><td width="30%" class="tabledata" >C12—C11—H11A</td><td width="20%" class="tabledata" >119.1</td></tr><tr><td width="30%" class="tabledata" >C2—C3—H3A</td><td width="20%" class="tabledata" >126.3</td><td width="30%" class="tabledata" >C11—C12—C13</td><td width="20%" class="tabledata" >117.08 (17)</td></tr><tr><td width="30%" class="tabledata" >C4—C3—H3A</td><td width="20%" class="tabledata" >126.3</td><td width="30%" class="tabledata" >C11—C12—C15</td><td width="20%" class="tabledata" >121.90 (18)</td></tr><tr><td width="30%" class="tabledata" >C5—C4—C3</td><td width="20%" class="tabledata" >107.23 (14)</td><td width="30%" class="tabledata" >C13—C12—C15</td><td width="20%" class="tabledata" >121.02 (18)</td></tr><tr><td width="30%" class="tabledata" >C5—C4—H4A</td><td width="20%" class="tabledata" >126.4</td><td width="30%" class="tabledata" >C12—C13—C14</td><td width="20%" class="tabledata" >121.72 (17)</td></tr><tr><td width="30%" class="tabledata" >C3—C4—H4A</td><td width="20%" class="tabledata" >126.4</td><td width="30%" class="tabledata" >C12—C13—H13A</td><td width="20%" class="tabledata" >119.1</td></tr><tr><td width="30%" class="tabledata" >C4—C5—O1</td><td width="20%" class="tabledata" >108.82 (13)</td><td width="30%" class="tabledata" >C14—C13—H13A</td><td width="20%" class="tabledata" >119.1</td></tr><tr><td width="30%" class="tabledata" >C4—C5—C6</td><td width="20%" class="tabledata" >133.33 (14)</td><td width="30%" class="tabledata" >C13—C14—C9</td><td width="20%" class="tabledata" >120.96 (17)</td></tr><tr><td width="30%" class="tabledata" >O1—C5—C6</td><td width="20%" class="tabledata" >117.85 (13)</td><td width="30%" class="tabledata" >C13—C14—H14A</td><td width="20%" class="tabledata" >119.5</td></tr><tr><td width="30%" class="tabledata" >C7—C6—C5</td><td width="20%" class="tabledata" >127.68 (15)</td><td width="30%" class="tabledata" >C9—C14—H14A</td><td width="20%" class="tabledata" >119.5</td></tr><tr><td width="30%" class="tabledata" >C7—C6—H6A</td><td width="20%" class="tabledata" >116.2</td><td width="30%" class="tabledata" >C12—C15—H15A</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >C5—C6—H6A</td><td width="20%" class="tabledata" >116.2</td><td width="30%" class="tabledata" >C12—C15—H15B</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >C6—C7—C8</td><td width="20%" class="tabledata" >121.64 (14)</td><td width="30%" class="tabledata" >H15A—C15—H15B</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >C6—C7—H7A</td><td width="20%" class="tabledata" >119.2</td><td width="30%" class="tabledata" >C12—C15—H15C</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >C8—C7—H7A</td><td width="20%" class="tabledata" >119.2</td><td width="30%" class="tabledata" >H15A—C15—H15C</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >O2—C8—C7</td><td width="20%" class="tabledata" >120.35 (15)</td><td width="30%" class="tabledata" >H15B—C15—H15C</td><td width="20%" class="tabledata" >109.5</td></tr></table>
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- <!-- endheading2div --><p>Ali, H. M., Puvaneswary, S., Basirun, W. J. & Ng, S. W. (2005). <i>Acta Cryst.</i> E<b>61</b>, o1079–o1080.<br /><br />Anto, R. J., Kuttan, G., Kuttan, R., Sathyanarayana, K. & Rao, M. N. A. (1994). <i>J. Clin. Biochem. Nutr</i>. <b>17</b>, 73–80.<br /><br />Bruker (1997). <i>SMART </i>and <i>SAINT</i>. Bruker AXS Inc., Madison, Wisconsin, USA.<br /><br />De Vincenzo, R., Ferlini, C., Distefano, M., Gaggini, C., Riva, A., Bombardelli, E., Morazzoni, P., Valenti, P., Belluti, F., Ranelletti, F. O., Mancuso, S. & Scambia, G. (2000). <i>Cancer Chemother. Pharmacol.</i> <b>46</b>, 305–312.<br /><br />Dimmock, J. R., Kandepu, N. M., Hetherington, M., Quail, J. W., Pugazhenthi, U., Sudom, A. M., Chamankhah, M., Rose, P., Pass, E., Allen, T. M., Halleran, S., Szydlowski, J., Mutus, B., Tannous, M., Manavathu, E. K., Myers, T. G., De Clercq, E. & Balzarini, J. (1998). <i>J. Med. Chem.</i> <b>41</b>, 1014–1026.<br /><br />Hsieh, H. K., Lee, T. H., Wang, J. P., Wang, J. J. & Lin, C. N. (1998). <i>Pharm. Res.</i> <b>15</b>, 39–46.<br /><br />Sheldrick, G. M. (2008). <i>Acta Cryst.</i> A<b>64</b>, 112–122.<br /><br />Zhou, L.-Y. (2007). <i>Acta Cryst.</i> E<b>63</b>, o3113.<br /><br /></p>
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