A Review of Criticality Accidents A Review of Criticality Accidents
A Review of Criticality Accidents A Review of Criticality Accidents
A Review of Criticality Accidents A Review of Criticality Accidents
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B. PHYSICAL AND NEUTRONIC CHARACTERISTICS FOR THE PROCESS FACILITY CRITICALITY<br />
ACCIDENTS<br />
In this section, we examine the physical and<br />
neutronic characteristics <strong>of</strong> criticality accidents that<br />
have occurred in nuclear processing facilities <strong>of</strong> the<br />
Russian Federation, the United States, the United<br />
Kingdom, and Japan. To assess the validity <strong>of</strong> the<br />
accident descriptions, we have compared the physical<br />
parameters reported for each accident to the experimentally<br />
known conditions for criticality.<br />
Accident Reconstruction<br />
The geometry and material specifications provided<br />
in accident documentation fall far short <strong>of</strong> qualifying<br />
as criticality benchmarks as accepted by the international<br />
criticality safety community. 33 The ability to<br />
accurately reconstruct accident configurations is<br />
seriously limited by the lack <strong>of</strong> reported technical<br />
detail. For example, in the case <strong>of</strong> accident 21, these<br />
limitations are so severe that a re-construction was not<br />
even attempted. Re-constructions for accidents 1<br />
through 20 and 22 are provided using interpretations <strong>of</strong><br />
conditions reported for the accident. The re–constructions<br />
are intended to estimate the accident configuration<br />
corresponding to the critical state. The estimates<br />
<strong>of</strong> the parameters necessary for these re-constructions<br />
should not be interpreted as new “facts” to be added<br />
into the documentation <strong>of</strong> the accidents.<br />
Only primary parameters affecting criticality are<br />
considered in our estimates–fissile species ( 235U or<br />
239Pu), fissile density, shape <strong>of</strong> fissile material, and<br />
degree <strong>of</strong> moderation. Uranium enrichment is also<br />
considered in the case <strong>of</strong> accidents 9, 15, and 22.<br />
Examples <strong>of</strong> parameters missing in the accident reconstructions<br />
or ignored as being <strong>of</strong> secondary<br />
importance include the vessel material, the vessel wall<br />
thickness, the presence <strong>of</strong> fissile nuclides other than<br />
235U and 239Pu, and the presence <strong>of</strong> external reflectors<br />
near or in contact with the fissile material. The material<br />
mixtures were modeled as homogeneous metal–water<br />
mixtures, from which the degree <strong>of</strong> moderation is<br />
implied. This was a known over–simplification for a<br />
few <strong>of</strong> the accidents (2, 9, 15, and 21) are known to<br />
have had a heterogeneous distribution.<br />
Table 9 presents estimated parameter values for 22<br />
process facility accidents. To the best <strong>of</strong> our knowledge,<br />
these 22 accidents represent a complete listing <strong>of</strong><br />
events that unambiguously qualify as process facilities<br />
accidents in the R. F., the U.S., the U.K., and Japan.<br />
Some explanation <strong>of</strong> the column headings presented<br />
in Table 9 is necessary.<br />
Accident number: The 22 accidents are numbered<br />
in chronological order. Chronological order was<br />
selected in recognition <strong>of</strong> the parallel historical time<br />
line <strong>of</strong> technological developments occurring in the<br />
four countries.<br />
Site and Date: Short abbreviations for the country<br />
in which the accident took place are used: R.F., U.S.,<br />
and U.K. for those that occurred in the Russian<br />
Federation, the United States and the United Kingdom,<br />
respectively. The accident date is provided in the<br />
day-month-year format.<br />
Geometry<br />
Vessel Shape: The vessel shape, e.g., cylindrical,<br />
vertical axis. Although this designation is accurate for<br />
most accidents, some accidents are known to have<br />
occurred when the axis <strong>of</strong> cylindrical symmetry was<br />
neither vertical nor horizontal, but rather tilted at some<br />
angle from the vertical.<br />
Vessel Volume: Vessel volume denotes the total<br />
volume <strong>of</strong> the vessel.<br />
Fissile Volume: This heading could be more<br />
properly described as fissile material volume. It is an<br />
estimate <strong>of</strong> the volume occupied by the fissile material<br />
that dominated the neutronic reactivity <strong>of</strong> the system.<br />
In some cases (accidents 5 and 18), fissile material was<br />
present in low concentration exterior to this volume.<br />
This additional material had a secondary impact on the<br />
system reactivity and was therefore ignored. For those<br />
accidents that occurred or were modeled with a vertical<br />
axis <strong>of</strong> cylindrical symmetry and the fissile material<br />
was in solution or slurry form, an additional parameter,<br />
h/D, is provided. In those cases the fissile material was<br />
modeled as a right-circular cylinder (lower case h<br />
designates the height <strong>of</strong> the cylinder and capital D<br />
designates the diameter <strong>of</strong> the vessel).<br />
Shape Factor: The shape factor was used to convert<br />
actual shape to equivalent spherical shape as a method<br />
to compare these 21 accidents in terms <strong>of</strong> geometrically<br />
equivalent spherical systems.<br />
For the 18 accidents where h/D is specified, the<br />
unreflected curve in Figure 3634 was used to determine<br />
the shape factor. The curve in Figure 36 is based<br />
directly on experimental results minimizing dependence<br />
on calculations. For the remaining 3 accidents<br />
(numbers 2, 6, and 20), buckling or other mathematically<br />
simple approximations were used to estimate the<br />
shape factor.<br />
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