![]() Site map |
|||
![]() |
![]() |
![]() |
![]() |
![]() |
![]() |
![]() |
![]() |
By means of the control file for the plaster sample
(plaster.sav
) the necessary elements will be explained here.
First, the instrumental function (calculated with GEOMET and MAKEGEQ, see previous pages) has to be provided:
VERZERR=urdneu11.geqThen the measuring value file is needed:
VAL[1]=kldomei5.val
This file is in the APX-63 format, a simple text format from the SEIFERT-FPM diffractometers. BGMN can process files with the extension 'rd' (Philips APD) and 'raw' (SIEMENS Diffrac-AT) as well. If you want to use other formats, you have to convert it into one of the above.
If a secondary graphite monochromator was used, an appropriate polarisation factor is (26.6 is the 2-theta angle of the graphite crystal; without monochromator use 'POL=1', which is the default):
pi=2*acos(0) POL=sqr(cos(26.6*pi/180))The structure files are given in this way:
STRUC[1]=quartz.str STRUC[2]=calcite.str STRUC[3]=gypsum.strAnd the formulae for the quantitative analysis are:
GOAL[1]=quartz/(quartz+calcite+gypsum) GOAL[2]=calcite/(quartz+calcite+gypsum) GOAL[3]=gypsum/(quartz+calcite+gypsum)In this file (
plaster.lst
) the results are written:
LIST=plaster.lstAn output file for the peak list (
plaster.par
) is necessary if
you want a graphical representation of the results:
OUTPUT=plaster.parFor the easy publication of diagrams a file (
plaster.dia
) with
measuring values, calculated, difference and background data can be written:
DIAGRAMM=plaster.diaLast, the global parameters for the zero point (
EPS1
) and sample
displacement (EPS2
) are included:
PARAM[1]=EPS1=0_-0.0001^0.0001 PARAM[2]=EPS2=0The calculation is started by the command
bgmn plasterand after each iteration step a line with information about the iteration number, the least squares sum and some other values is printed.
RESOUT[1]=quartz.res
PDBOUT[1]=quartz.pdb
STRUCOUT[1]=quartz.sto