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ENSI Erfahrungs- und Forschungsbericht 2011
nisms determine the particle retention close to
the break where major retention takes place.
2. Even with a very low submergence significant
aerosol retention takes place. With high flow
rate and large spherical particles, aerosol trans-
port efficiency through the flooded bundle is
very low underlining the importance of the jet
– bundle interactions close to the tube break
on the aerosol retention in the flooded bundle.
3. Droplets are entrained from the water surface
with high gas flow rates. They carry aerosol par-
ticles with them and once the droplets evap-
orate, aerosol particles are released to the gas
flow. However, compared to particle retention
in the water due to inertial effects close to the
tube break, the effect of droplet entrainment on
particle transport is small. However, further work
would be recommended to determine this effect
when the aerosol loading in the water is high
at the later stages of the accident progression
when cumulative released aerosol mass is high.
4. Based on these tests as well as earlier data [vii],
the increasing submergence of the break in-
creases the particle retention in the water, and
the effect is much stronger in the flooded bun-
dle than in bare pools. This is presumably due to
the jet – bundle interactions, creating very com-
plex two-phase flows. This indicates that mod-
els developed for bare pools should be adapted
for calculation of aerosol retention in the flood-
ed bundle even in the regions far away from the
tube break.
When the steam generator secondary side was
filled with water up to the dryer section inlet
(Phase VIII, flooded separator), aerosol retention
was even higher than in the flooded bundle. The
effect of different gas flow rates and particle siz-
es was investigated. The decontamination fac-
tor in the flooded separator was found to be very
high in all the tests. No significant difference in DF
was measured with different flow rates or differ-
ent particle sizes. The high aerosol retention in the
flooded separator was mainly due to the large wa-
ter submersion of the break, combined with the
complex flow pattern inside the flooded separator.
Modeling of aerosol retention by pool scrubbing
in a wet SG faces two challenging conditions: gas
injection under the jet regime and the presence of
tube surfaces. The approach adopted to extend
the current capabilities of estimating pool scrub-
bing DFs (Decontamination Factors) has been to
extend a previous developed tool to accommo-
date the specific features of the SGTR scenario:
SPARC90 [viii]. So far the major progress has been
achieved in the adaptation of the particle trap-
ping as a consequence of water droplets entrained
within the gas jet at the inlet point. Decontamina-
tion by droplet entrainment is strongly dependent
on droplet features such as the number of drop-
lets entrained, their diameter and the relative ve-
locity. The equations embedded within SPARC90
have been reviewed and, when necessary, updat-
ed with alternative equations better fitted to the
conditions expected in the SGTR scenario. Present-
ly this work is still in progress and will be continued
in the ARTIST-extension project.
Droplet retention in the steam generator
dryer, DBA accident conditions
Rupture of one or more steam generator tubes re-
sults in leakage of primary coolant to the second-
ary side, and consequently, pressure increase in the
secondary side of the steam generator. The pres-
sure increase may be sufficient to cause a pres-
sure relief valve to open thereby providing a di-
rect pathway for the radioactive primary coolant
to the environment. The radioactivity release re-
sulting from such incidents depends strongly on
the conditions in the primary and secondary side
of the steam generator. For most of the condi-
tions, radioactivity release can be calculated based
on existing data [ix], however, under non-recircu-
lating conditions in the dry secondary side, no ex-
perimental data are available to assess the reten-
tion of radioactivity in the steam generator. Under
these conditions, release takes place mainly in the
form of droplets formed when the primary coolant
is released to the secondary side as a flashing jet.
The retention of droplets in the upper structures
SQRT(Stk)
DF
Flooded bundle, agglomerates
Flooded bundle, spherical
Figure 5:
The decontamination
factor DF in the tests in
the flooded bundle.
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