UPPW-11 - Part 2
February 7, 2004
Problem :Bethanechol chloride C7H17ClN2O2
   
Not any result for two ICDD entries (43-1748 and 46-1964), 
both Grant-in-Aid, this was an interesting case for investing more
efforts.

Two new powder patterns were recorded, one from conventional 
X-ray data and the other from synchrotron radiation. Try to
index with both data for comparison. Peak positions come
from the application of the PowderX and WinPLOTR programs.
The raw data are also available, so that you may try by yourself
(bethanechol.zip, see the readme.txt file inside).
1- Conventional X-ray data
2- Synchrotron radiation data
3- RESULTS

1- Conventional X-ray data Wavelength : CuKalpha Bragg Brentano geometry Diffractometer : Bruker D8 Advance Filter : graphite monochromator in the diffracted beam Soller 2°, variable slits V6/V6, Soller 2°, receiving slit 0.1mm.  Sample pressed on a silicium zero-background holder - there is a huge preferred orientation... Peak positions extracted after Kalpha2 removal by PowderX : Use a wavelength = 1.54056 A     2Theta     d (A)    Height      Area     FWHM     10.765   8.21189     586.4    5048.1    0.0900               13.522   6.54300     267.4    2659.7    0.1000               14.690   6.02503    1220.2   12200.8    0.1000               15.398   5.74973    1011.1    9639.7    0.1000               16.336   5.42166     651.7    5422.6    0.0900               16.453   5.38340     907.6    7253.9    0.0800               17.312   5.11797    1057.6   10563.0    0.1000               18.828   4.70937    4046.6   38944.4    0.1000               19.699   4.50305     604.1    4518.1    0.0800               20.031   4.42900   37355.4  372792.8    0.1000               20.752   4.27682   29949.5  262874.6    0.1000               21.641   4.10301    1410.0   11674.2    0.0900               22.414   3.96332    1727.5   17143.8    0.1000               22.788   3.89913     338.3    3085.2    0.1000               23.152   3.83862     399.0    3572.5    0.0900               23.528   3.77803     717.7    7108.4    0.1100               23.872   3.72444    3541.2   34941.0    0.1100               24.970   3.56314    3271.3   44472.8    0.1400               25.365   3.50843     343.4    3678.3    0.1100               25.549   3.48368     471.1    4696.7    0.1100               26.653   3.34175    1484.9   16158.0    0.1100               27.292   3.26492    6395.6   70220.6    0.1100               27.404   3.25188     378.2    4152.2    0.0900               28.153   3.16705    1547.6   15997.6    0.1100               29.345   3.04109     483.0    5163.2    0.1100               29.634   3.01202    3439.0   37394.7    0.1100               29.859   2.98982     388.4    4271.8    0.1100               30.737   2.90641     368.3    3118.0    0.1000               31.038   2.87896     917.7   14029.6    0.1600               31.346   2.85138    1085.6   10555.1    0.1000               31.694   2.82083     694.5    6890.7    0.1000               31.981   2.79615     304.0    2601.9    0.1100               32.704   2.73596    2645.2   26031.0    0.1000               32.986   2.71319     265.8    3386.3    0.1300               33.259   2.69156     960.7    9169.6    0.1000               33.572   2.66721    2790.6   30643.6    0.1100               33.824   2.64791    1487.4   14439.3    0.1000               34.273   2.61426    2272.4   22636.6    0.1000               34.473   2.59953    1041.1   10374.5    0.1000               35.072   2.55647     780.5    8561.6    0.1100               36.330   2.47079     216.5    2598.4    0.1200               36.761   2.44281    1122.5   12337.7    0.1100               38.632   2.32872     514.3    5257.9    0.1100               38.939   2.31106     270.0    2965.8    0.1100               39.722   2.26728     494.3    5168.9    0.1100               39.920   2.25645     272.3    2502.2    0.1000           Plot of the peak extraction with PowderX : You may also use WinPLOTR for peak position extraction:
      2-theta     Intensity
      10.77139     851.57367
      13.52686     495.88849
      14.69663    1621.39709
      15.40200    1493.84937
      16.34025    1053.72449
      16.45465    1420.88977
      17.31883    1549.34705
      18.83232    5224.92920
      19.71169    1037.66187
      20.03352   42190.27730
      20.75316   35701.29300
      21.64195    1928.24133
      22.41502    2412.89478
      22.78733     675.22955
      23.15637     744.61774
      23.53123    1123.72656
      23.87491    4531.69043
      24.99511    4739.06250
      25.55305     819.55084
      26.66311    1964.76892
      27.29758    8198.01758
      28.16043    2001.15540
      29.36309     857.51581
      29.64191    4131.47461
      30.73515     654.15381
      31.08307    1412.29028
      31.34560    1537.70874
      31.69426    1116.46436
      32.70807    3149.14478
      33.26403    1433.92297
      33.57528    3590.28076
      34.27499    2907.26660
      34.46975    1580.02295
      35.07713    1215.08728
      36.76001    1598.01526
      38.63772     870.49487
      38.93926     613.23083
      39.72001     855.00787
      40.29115    1040.59851
      40.69636    2157.91284

Pmot of the peak position extraction with WinPLOTR:







2- Synchrotron radiation data From Peter Stephens : This was in a capillary, rotating 5 degrees at each point.  The x-ray wavelength was 0.6995(1) Angstrom.  Peak positions determined using TOPAS. 2-theta 4.887 6.139 6.664 6.989 7.403 7.460 7.850 8.531 8.921 9.062 9.251 9.386 9.781 10.136 10.300 10.468 10.634 10.783 11.280 11.450 11.538 12.032 12.309 12.693 Diffractometer dimensions are 9999 and 330 mm, and the slit widths are each 8mm in the Finger model.  For programs such as GSAS and FULLPROF, the axial divergence parameters S/L and D/L should be approximately 0.013. Files are given as : - bethcl.xye - columns are 2theta, normalized intensity, and statistical esd.  This works as an .xye file in topas. - bethclfp.dat - suitable for FULLPROF, to be read in with INST=4. The peaks are a bit lumpy on the leading edges.  We chopped the crystals slightly before putting them in the capillary - perhaps the grains are still a bit large.  It's pretty clear from the raw data that not all the peaks have the same width, which suggests anisotropic strain broadening. ~^~^~^~^~^~^~^~^~^~^~^~^~^~^~^~^~^~^~^~ Peter W. Stephens, Professor Department of Physics & Astronomy State University of New York Stony Brook, NY 11794-3800 Also the peak positions extracted by using WinPLOTR :       2-theta      intensity        4.88347     621.03375        6.13510    3346.94678        6.65972    2584.68872        6.98167   10082.64840        7.39827    5562.50830        7.45556    7862.69287        7.84648    8171.25586        8.52491   22505.94730        8.91795    3039.21948        9.02300    4712.42090        9.05811   18023.87700        9.24659    1723.87256        9.38270   30460.68750        9.77793    1071.30981       10.13092    9286.77148       10.29570     801.25635       10.46380    2147.25049       10.62740    2796.40894       10.77905    6253.17773       11.26817   15937.82030       11.28600   12646.79980       11.44456    1640.77466       11.53195    4507.09375       12.02698    6162.85107       12.29600   21771.59960       12.30746   23952.33790       12.68795    6189.18555       13.22028    1789.09290       13.34459    6060.21582       13.45726    2243.41064       13.95884    5343.84131       13.98149    3791.70044       14.09899    3920.16992       14.25158    2207.43970       14.69006    1923.03406       14.82360    1573.35303       14.94255    5070.35400       15.08046    7077.85986       15.19008    3919.37622 Corresponding WinPLOTR drawing : And this is the conventional powder pattern which was obtained (Bragg-Brentano - reflection)  almost free of preferred orientation (dusting the sample through a sieve - low resolution)  for comparison with the synchrotron pattern above (transmission - capillary) : !!!!!!!!!!!!
3-RESULTS
Most probable cell(s) according to the Participants :
UPPWs end in apotheosis...
Complete consensus on an obvious monoclinic cell giving high figures of
merit (FoM) from both the synchrotron and the new conventional X-ray data.
Most participants were curious to compare with the ICDD PDF 43-1748 and
46-1964 Grant-in-Aid entries, and found that both had a large zeropoint
error (~ -0.10°2-theta) and more or less impurity lines (8 impurity lines
among the first 25 ones for 43-1748 and 3 among the first 32 for 46-1964). 

Moreover, one participant (Jacco van de Streek, CCDC) proposes the crystal 
structure solved by using DASH.

Program              a          b           c        alpha      beta     gamma       V     
                                            M(20)       F 20         Unindexed    Zero   Spacegroup

TREOR (NM)        11.023      16.418      7.148       90.      126.49      90.      1040.0
  (X-conv)                              M(20)= 47    F20 = 116 (0.006, 30)                 P21/a

TREOR (SG)        11.021      16.422      7.147       90.      126.48      90.      1040.0
  (X-conv)                              M(20)= 41    F20 = 96 (0.007, 30)                  P21/a

CRYSFIRE (RS)      8.880      16.408      7.138       90.       93.86      90.      1037.7
  (synch)                               up to 160                                          P21/n

EFLECH/INDEX (JB)  7.139      16.413      8.879       90.       93.83      90.   
  (synch)
X'PERT PLUS (JvM)  8.881      16.417      7.141       90.       93.86      90.      1038.7
(ITO, DICVOL, McMaille) (synch)
DICVOL (JvdS)      8.875      16.408      7.137       90.       93.84      90.      1036.9
(in DASH) (synch)                         M(20)=197     F20 = 1080 (0.0006, 32)            P21/n
AUTOX (VZ)         7.153      16.421      8.880       90.       93.77      90.      1040.8

McMaille (ALB)     8.875      16.407      7.141       90.       93.82      90.      1037.6       
          (X-conv)                        M(20)=52      F20 = 127 (0.005, 31)              P21/n
                   8.876      16.409      7.135       90.       93.83      90.      1036.8
          (synch)                         M(20)=168     F20 = 888 (0.0008, 30)             P21/n


Results from NM and SG (TREOR), Robin Shirley (CRYSFIRE), Joerg Bergmann (EFLECH/INDEX),
JvM (X'PERT PLUS : ITO, DICVOL, McMaille), Jacco van de Streek (DICVOL/DASH), Victor Zlokazov (AUTOX)
 and Armel Le Bail (McMaille).

Plot by using DASH solving the crystal structure from the synchrotron data :
Plot by using ESPOIR solving the crystal structure from the synchrotron data :
This is the end of UPPWs.
Thanks a lot to all participants !