[ Identification | Description | Input parameters | Output parameters | Links ]
Convert_FlatE_2_Maxwell componentThe routine modifies/converts the incident flat (in energy) neutron spectra, as it comes out from a source like the standard adaptive source Source_adapt, to obtain a Maxwellian neutron distribution, as it is approximatively the case for thermal neutrons in a reactor's moderator (e.g. the HFR of the ILL in Grenoble). So, this component is only a virtual one, not corresponding to a real element in a neutron beam.
| Name | Unit | Description | Default |
|---|---|---|---|
| T | K | The temperature of the source, 293 K for thermal neutrons (beam tube H11 at ILL) | |
| E0 | meV | Mean energy of neutrons (as for Source_adapt) | |
| dE | meV | Energy spread as for Source_adapt (energy range is from E0-dE to E0+dE) |
| Name | Unit | Description | Default |
|---|---|---|---|
| Lmin | AA | Minimum wavelength in energy range | |
| Lmax | AA | Maxium wavelength in energy range | |
| l0 | AA | Mean wavelength of neutron spectra, about 1.8 AA for thermal neutrons | |
| L2P | AA**4 | Normalisation constant for Maxwell distribution |
Convert_FlatE_2_Maxwell.comp.
[ Identification | Description | Input parameters | Output parameters | Links ]
Generated automatically by McDoc, Kristian Nielsen <kristian.nielsen@risoe.dk> / Jan 22 2001