Changeset 82e5fb for doc/userguide


Ignore:
Timestamp:
May 25, 2021, 11:04:50 PM (4 years ago)
Author:
Frederik Heber <frederik.heber@…>
Branches:
Candidate_v1.7.0, stable
Children:
91793c
Parents:
889067e
git-author:
Frederik Heber <frederik.heber@…> (05/25/21 21:55:59)
git-committer:
Frederik Heber <frederik.heber@…> (05/25/21 23:04:50)
Message:

Added option error-file to fit potential actions.

File:
1 edited

Legend:

Unmodified
Added
Removed
  • doc/userguide/userguide.xml

    r889067e r82e5fb  
    24302430      --set-threshold 1e-3 \
    24312431      --training-file test.dat
     2432      --error-file error.dat
    24322433   </programlisting>
    24332434          <para>Now, all empirical potential functions are summed up into a
     
    24372438          potential between oxygen and hydrogen and another angular potential
    24382439          for the angle between hydrogen, oxygen, and hydrogen atom. Then, we would
    2439           fit a function consisting of the sum of the two potentials functions in order to approximate the energy of a single
    2440           water molecule (actually, it&apos;s the sum of three potentials. As mentioned before, a constant potential is always added to compensate non-bonding energies, i.e. not depending on interatomic distances). Here, the threshold criterion takes the place of the
    2441 <emphasis role="bold"> take-best-of</emphasis> option. Here, the minimization is reiterated so often on random (but to some extent chosen from a sensible range) starting parameters until the final L2 error is below 1e-3. Also, all data used
    2442           for training, i.e. the tuples consisting of the fragments nuclei
    2443           coordinates and the associated energy value are written to the file
    2444           <filename>test.dat</filename>. This allows for graphical representation or other
    2445 way of analysis, e.g. for a Morse potential between oxygen and hydrogen the bonding energy can be plotted as a one-dimensional function and compared to the &quot;point cloud&quot; of sample points from the fragment term of Born-Oppenheimer surface. It is this point cloud, i.e. the training data, that is written to the file
    2446           <filename>test.dat</filename>.</para>
     2440          fit a function consisting of the sum of the two potentials functions in
     2441          order to approximate the energy of a single water molecule (actually,
     2442          it&apos;s the sum of three potentials. As mentioned before, a constant
     2443          potential is always added to compensate non-bonding energies, i.e. not
     2444          depending on interatomic distances). Here, the threshold criterion takes
     2445          the place of the<emphasis role="bold"> take-best-of</emphasis> option.
     2446          Here, the minimization is reiterated so often on random (but to some
     2447          extent chosen from a sensible range) starting parameters until the final
     2448          L2 error is below 1e-3. Also, all data used for training, i.e. the tuples
     2449          consisting of the fragments nuclei coordinates and the associated energy
     2450          value are written to the file <filename>test.dat</filename>. This allows
     2451          for graphical representation or other way of analysis, e.g. for a Morse
     2452          potential between oxygen and hydrogen the bonding energy can be plotted
     2453          as a one-dimensional function and compared to the &quot;point cloud&quot;
     2454          of sample points from the fragment term of Born-Oppenheimer surface.
     2455          It is this point cloud, i.e. the training data, that is written to the file
     2456          <filename>test.dat</filename>. Moreover, the error per fragment is written
     2457          to the file <filename>error.dat</filename></para>
    24472458          <para>Note that you can combine the two ways, i.e. start with a
    24482459          fit-potential call but give an empty potential file. The resulting
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