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Health Physics

The gummed film data were occasionally not consistent with other types of measurements Someof the
difficulties m interpreting the gummed film data were
the lack of mformation on the exact date of counting
and any counting efficiency corrections that might
have been madeto the origmal data Because much of
the fallout at the sites of the gummed film stations was
associated with very heavy precipitation, the abihty of
gummed film to retam fallout particles was likely to
have been very low at times These various factors
resulted m high uncertamty im our interpretations of
the gummed film data, particularly for the purpose of

making quantitative mterpretations

Despite various limitations, the gummed film data
were good indicators of the specific calendar days on
whichfallout occurred at the samplingsites and unequivocally demonstrated the contmuation of fallout for several days after a mayor test The gummed film data and
the HASL automatic gamma-ray momtors were both
imdicatve that the HASL air surveys were often conducted prior to the end offallout deposition and, occasionally, even conducted prior to the arrival of fallout
Thus, some earher reported deposition estimates based
only on the air survey data were too low,particularly in
the southem Marshall Islands where muchofthe fallout
occurred several days after the detonations

Use of an atmospheric transport model
Becausethere are no knownfallout momtormg data
for the Marshall Islands prior to the 1952 Ivy series
(except at the test site atolls), it was necessary to use a
meteorological model and archival meteorological data
to estimate fallout deposition at the atolls for tests

August 2010, Volume 99, Number 2
Modeling the transport and deposition of particles
released from a nuclear weapons test 1s a complex and
highly uncertam exercise, even if perfect mformation on
the spatial variations im wind speeds and directions over
the entire region 1s available The actual activity-particle
size distribution im a nuclear debris cloud varies with the
particular type and yield of the tests, the height of the
burst and the local topography Nodataof these types are

available for the Pacific tests Thus, the amountof °7Cs

attached to particles of a particular size released from a
particular altitude could only crudely be estrmated for the
tests of mterest based on limited data from Nevadatests
In order to relate the geographic pattern of deposition and number of deposited particles estimated by

HYSPLIT to the ’Cs deposition as a function of yield,

debris cloud size, and altitude, we developed a crude

model to describe the relative numbers of particles
released from the cap of the stabihzed mushroom cloud
at various altitudes as well as from the stem (Morozet al

2010) An actvity-particle size distribution was also
estimated based on data of beta activity as a function of
particle size from measurements followmg NTS tests,

modified slightly to reflect the fact that '*’Cs tends to be
depleted on the larger particles due to a predisposition for
the larger particles to be deposited prior to the formation

of ‘Cs from its gaseous precursor, °’Xe The total
amount of ‘Cs released was estimated from the esti-

mated fission yield of each test (UNSCEAR 2000, Hicks
1981, 1982) Note, however, that even the fission yields

for US TN tests are only an estimate (UNSCEAR
2000), since those data are still classified

Trajectory

Comparisons were made of the geographic deposition patterns predicted by HYSPLIT with historical
groundoraircraft radiological momtorimg data Based on
comparisons for tests where momitoring data were available, 1t appears that when HYSPLITpredicted fallout in

2007), was developed and 1s maintamed by the National

mated deposition generally agrees with measured '*’Cs to

under certam conditions, can be apphed to estrmating
dispersion of fallout from nuclear testmg Our application of the HYSPLIT model for estrmatmg Marshall
Islands fallout 1s discussed m a compamion paper m this

meteorological model could be used to only provide
crude estates of fallout where no measurements were
made A more rehable use for HYSPLIT was to support
our mterpolations of deposition at atolls from real measurements of deposition at nearby atolls
Although the HYSPLIT model estimates are very
uncertam, m somecases they were the only source of any
imformation on fallout deposition and, m general, supported numerous anecdotal reports of substantial fallout
prior to 1952 at someatolls, m particular at Ujelang from
two 1951 tests, Dog and Item The HYSPLITpredictions
werealso used to complete the fallout deposition pattern
for 1956 and 1958 tests for which only a limited number
ofatolls were monitored for radioactive debris The 1956

conducted m 1946, 1948, and 1951

here,

Hybrid

Smgle-Particle

The model used

Integrated

(HYSPLIT) (Draxler and Hess 1997, Draxler et al

Oceanic and Atmosphenc Admmustration (NOAA) and

issue (Moroz et al 2010) The HYSPLIT code models

the fallout deposition downwind from available meteorological data at the timeofthe test, usmg reanalysis data
sets of historical meteorological measurements extrapolated to a sparse grid The model simulates the transport
and deposition ofparticles of different sizes onigmating
at different altitudes at the location of the test The
HYSPLIT model does not simulate the weapons debris
cloud itself or the radioactivity associated with particles
of a given size

the areas where fallout was actually observed, the estwithm a factor of 10 (Moroz et al

2010) Thus, the

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