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Averaging over Scattering: tex2html_wrap_inline4391, etc.

DDSCAT automatically carries out numerical integration of various scattering properties. In particular, it calculates the mean value tex2html_wrap_inline4391 for the scattered intensity for each incident polarization state. This is accomplished by evaluating the scattered intensity for ICTHM different values of tex2html_wrap_inline4339 (including tex2html_wrap_inline4351 and tex2html_wrap_inline4399), and taking a weighted sum. For each value of tex2html_wrap_inline4339 except 0 and tex2html_wrap_inline4405, the scattering intensity is evaluated for IPHM different values of the scattering angle tex2html_wrap_inline4341. The angular integration over tex2html_wrap_inline4339 is accomplished using Simpson's rule (with uniform intervals in tex2html_wrap_inline4411), so ICTHM should be an odd number. The angular integration over tex2html_wrap_inline4341 is accomplished by sampling uniformly in tex2html_wrap_inline4341 with uniform weighting; IPHM can be either even or odd.

The following quantities are evaluated by this angular integration:

It is important that the user recognize that accurate evaluation of these angular averages requires adequate sampling over scattering angles. For small values of the size parameter tex2html_wrap_inline4421, the angular distribution of scattered radiation has a dipolar character and the sampling in tex2html_wrap_inline4339 and tex2html_wrap_inline4341 does not need to be very fine, so ICTHM and IPHM need not be large. For larger values of the size parameter x, however, higher multipoles in the scattered radiation field become important, and finer sampling in tex2html_wrap_inline4339 and tex2html_wrap_inline4341 is required. We do not have any foolproof prescription to offer, since the scattering pattern will depend upon the target geometry and dielectric constant in addition to overall size parameter. However, as a very rough guide, we suggest that the user specify values of ICTHM and IPHM satisfying
  
The sample ddscat.par file supplied has tex2html_wrap_inline4433 and tex2html_wrap_inline4435; the above criteria would suggest that this would be suitable for x<5.

The cpu time required for evaluation of these angular averages is proportional to tex2html_wrap_inline4439. Since the computational time spent in evaluating these angular integrals can be a significant part of the total, it is important to choose values of ICTHM and IPHM which will provide a suitable balance between accuracy (in this part of the overall calculation) and cpu time.

Within one scattering plane, the scattered intensity tends to have approximately (1+x) peaks for tex2html_wrap_inline4443, so that the above prescription for ICTHM would have at least 5 sampling points per maximum. The angular distribution over tex2html_wrap_inline4341 is usually not as structured as that over tex2html_wrap_inline4339 so we suggest that IPHM need not be as large as ICTHM. We have refrained from ``hard-wiring'' the values of ICTHM and IPHM because we are not confident of the reliability of the recommended criteria (23,24) - it is up to the user to specify appropriate values of ICTHM and IPHM according to the requirements of the problem being addressed.


next up previous contents
Next: Mueller Matrix for Scattering Up: User Guide for Previous: Incident Polarization State

Bruce Draine
Thu Aug 10 09:34:16 EDT 2000