AEOLUS-3
A software package for the
determination of atmospheric dispersion and deposition of nuclear power plant effluents
during continuous, intermittent and accident conditions, in open-terrain sites, coastal
sites and deep-river valleys.
Key Features
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Joint frequency wind and
rainfall distributions |
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Concentration X/Qs |
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Finite-cloud gamma X/Qs |
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D/Qs |
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Distant and close-in
receptors (adaptation of the Murphy/Campe model) |
Basic Features at a Glance
Appendix I to 10CFR50 provides numerical guidance
for design objectives and limiting conditions for operation of light-water-cooled reactors
to ensure that radioactivity releases to the environment are "as low as reasonably
achievable." To implement this appendix, the Nuclear Regulatory Commission has
developed a series of guides providing acceptable methods for the calculation of effluent
releases, dispersion of the effluents, and the resulting radiation doses to man. One of
the guides, Regulatory Guide 1.111, describes models and assumptions for estimating
long-term concentrations of radioactive material in the vicinity of nuclear power plants
which would result from routine airborne releases. Another guide, Regulatory Guide 1.109,
describes models and assumptions for calculation of annual doses to man which would result
from such releases.
In addition to the above, and for compliance with
the requirements of 10 CFR Part 100 and 10 CFR Part 50, the Commission has also issued
Regulatory Guide 1.145 which provides guidance on short-term atmospheric dispersion models
for the assessment of consequences of potential accidents at nuclear power stations.
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Implementation of the
following models:
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Long-term dispersion and
deposition models in Regulatory Guide 1.111 for routine releases |
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The models in Regulatory
Guide 1.145 for short-term, accidental releases |
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A model similar to that
in the XOQDOQ code for intermittent releases |
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Adaptation of the
Murphy/Campe dispersion equation for close-in receptors, based on 95% meteorology and
user-specified wind-direction sectors affecting the receptors
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Open terrains, coastal
sites, and deep river valleys, with continuous, intermittent and accidental- release
options, the models/features in each case (or as applicable) including the following:
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Use of multi-year hourly
meteorological data (wind direction, wind speed, vertical temperature difference, and,
optionally, rainfall and solar radiation) |
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Straight-line trajectory
models with Gaussian diffusion (inclusive of plumes which follow the valley in the
deep-river-valley option) |
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Concentration and gamma
(X/Q) models (see Footnote 1) (plume centerline and
sector- average) |
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Depletion and deposition
models [two options: (a) the models in Regulatory Guide 1.111, and (b) models making use
of the deposition-velocity concept] |
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Extrapolation of wind
speed with height |
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Partial plume
entrainment at the release point (split-H model, with part-time elevated and part-time
ground-level releases) |
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Building wake effects |
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The Murphy and Campe
building-wake methodology for close-in receptors |
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Plume meander effects |
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Plume rise effects
(buoyant or momentum) |
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User-specified terrain
features |
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Vertical reflection
correction in all cases, and horizontal reflection correction in valley flows |
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Recirculation correction
factors (built-in values for open terrains, or user-specified values) |
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In-transit decay
correction (two user-specified decay constants, one for noble gases and one for halogens) |
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User-specified halogen
and noble-gas relative isotopic concentrations, or gamma spectra, for the finite-cloud
gamma (X/Q)s |
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Preparation of
joint-frequency distributions (atmospheric stability, wind direction and wind speed;
rainfall; sea breezes; up-valley and down-valley flows and associated rainfall)
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Outputs which include
the following dispersion and deposition parameters:
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For routine, continuous
releases:
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The plume centerline
concentration (X/Q) |
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The sector-average
concentration (X/Q) |
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The plume centerline
finite-cloud gamma (X/Q) |
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The sector-average
finite-cloud gamma (X/Q) |
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The plume centerline
decayed (D/Q) |
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The sector-average
decayed (D/Q)
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For intermittent and
accidental releases:
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The hybrid concentration
(X/Q) |
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The hybrid finite-cloud
gamma (X/Q) |
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The hybrid (D/Q) |
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where:
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(X/Q)s for all types of
releases are calculated for (i) undecayed, undepleted conditions, (ii) decayed conditions
for noble-gas-release applications, and (iii) decayed and depleted conditions for
halogen-release applications
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The hybrid model for
intermittent and accidental releases makes use of log-log plots of the 1-hour plume
centerline values (for the concentration X/Q, the gamma X/Q and the D/Q) and their
corresponding sector-average values averaged over the joint-frequency distribution, to
compute 'hybrid' values at intermediate time intervals of interest
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The results for
accidental releases include tables for each sector independently, and for all sectors
combined (overall-site model)
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Detailed
intermediate-result printout for any receptor of interest, such as decay correction
factors, wet and dry depletion and deposition factors, horizontal reflection correction in
valleys, dispersion zones and virtual source distances in sea breeze analyses, ordered
arrays of values in intermittent and accidental releases, etc.
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FORTRAN 77; 7900 coded
lines; DOS and UNIX applications; ASCII file input; 132-column output
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Documentation Package
P100-R19, "AEOLUS-3 - A Computer Code for the
Determination of Atmospheric Dispersion and Deposition of Nuclear Power Plant Effluents
During Continuous, Intermittent and Accident Conditions in Open-Terrain Sites, Coastal
Sites and Deep-River Valleys"
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P100-R19-A - Technical
description |
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P100-R19-B - Program
Listing |
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P100-R19-C -
Implementation Test Runs |
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P100-R19-D - Code
Verification Test Report |
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P100-R19-E - Addendum |
Footnote 1
Physically speaking, the
gamma X/Q for a given finite plume defines the equivalent concentration in a semi-infinite
cloud at ground level which will yield the same gamma radiation exposure as the finite
plume itself. In short, the standard gamma dose rate equation for a semi-infinite cloud is
converted to the dose rate equation for a finite cloud by simply replacing the
concentration (X/Q) in the former with the gamma (X/Q).
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