insights from review and analysis of the fukushima daiichi accident
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Insights from review and analysis of the Fukushima
Dai-ichi accidentMasashi Hirano
a, Taisuke Yonomoto
a, Masahiro Ishigaki
a, Norio Watanabe
a, Yu
Maruyamaa
, Yasuteru Sibamotoa
, Tadashi Watanabea
& Kiyofumi Moriyamaa
aNuclear Safety Research Center, Japan Atomic Energy Agency, 2-4 Shirane, Shirakata,
Tokai-mura, Naka-gun, Ibaraki, 319-1195, Japan
Version of record first published: 24 Jan 2012.
To cite this article: Masashi Hirano , Taisuke Yonomoto , Masahiro Ishigaki , Norio Watanabe , Yu Maruyama , YasuteruSibamoto , Tadashi Watanabe & Kiyofumi Moriyama (2012): Insights from review and analysis of the Fukushima Dai-ichi
accident, Journal of Nuclear Science and Technology, 49:1, 1-17
To link to this article: http://dx.doi.org/10.1080/18811248.2011.636538
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INVITED REVIEW Fukushima NPP Accident Related
Insights from review and analysis of the Fukushima Dai-ichi accident
Masashi Hirano*, Taisuke Yonomoto, Masahiro Ishigaki, Norio Watanabe, Yu Maruyama, Yasuteru Sibamoto,
Tadashi Watanabe and Kiyofumi Moriyama
Nuclear Safety Research Center, Japan Atomic Energy Agency, 2-4 Shirane, Shirakata, Tokai-mura,Naka-gun, Ibaraki 319-1195, Japan
(Received 5 September 2011; accepted final version for publication 26 September 2011 )
An unprecedented earthquake and tsunami struck the Fukushima Dai-ichi Nuclear Power Plants on 11
March 2011. Although extensive efforts have been continuing on investigations into the causes andconsequences of the accident, and the Japanese Government has presented a comprehensive report on the
accident in the IAEA Ministerial Conference held in June 2011, there is still much to be clarified on what
happened during the accident and why. This article aims at identifying what should be clarified further
about the progression of the accident at Units 13 through the review and analysis of information released
from Tokyo Electric Power Company and government authorities. It also discusses the safety issues raised
by the accident based on the insights gained, in order to contribute to establishing a new framework that
pursues continuous improvement toward the highest standards of safety that can reasonably be achieved.
Keywords: Fukushima Dai-ichi accident; accident management measures; alternative water injection;
containment integrity; venting; defense in depth; design basis; beyond design basis; external events;
continuous improvement; highest standards of safety
1. Introduction
Approximately three weeks after the accident at the
Fukushima Dai-ichi Nuclear Power Plants (hereinafter,
referred to as F-1NPPs) of Tokyo Electric Power
Company (TEPCO), the Nuclear and Industrial Safety
Agency (NISA) made a presentation at a side event on the
accident during the Fifth Review Meeting of the Conven-
tion of Nuclear Safety, co-sponsored by Japan and the
International Atomic Energy Agency (IAEA), on 4 April
2011 and reported the overall plant behavior during the
accident to that time to the international community [1].
On 25 April 2011, the NISA requested TEPCO to report
the plant records and other relevant information pur-
suant to the Law for the Regulation of Nuclear Source
Material, Nuclear Fuel Material and Reactors (Nuclear
Regulation Law), and Electricity Utilities Industry Law
[2]. On 16 May 2011, TEPCO reported to the NISA [3]
and at the same time released a lot of information
including the plant records on its Webpage at http://
www.tepco.co.jp/en/nu/fukushima-np/index-e.html. On
receiving the report, the NISA further requested
TEPCO to provide additional information which could
supplement the report [4]. On 24 May 2011, TEPCO
submitted the supplemental information to the NISA
[5], which then issued its evaluation report [6].
The Nuclear Emergency Response Headquarters of
the Government presented a comprehensive report on
the accident [7] at the IAEA Ministerial Conference on
Nuclear Safety held atthe IAEA from20 Juneto 24June.
The IAEA fact finding expert mission for the accident
visited Japan from 24 May to 2 June and presented its
report [8] also in this meeting. TEPCO conducted ana-
lyses of plant behaviors at Units 13 with the Modular
Accident Analysis Program (MAAP) codeand the results
were included in the Governments report. On 18 June
2011, TEPCO also released a report that included the
description of operator actions taken to cope with the
accident in its early phase [9].
In the US, the near-term task force of the Nuclear
Regulatory Commission (NRC) issued its report on 12
July 2011 [10]. Although the task force made recom-
mendations especially on the regulatory framework for
the US NRC, the discussion is insightful and part of it
is thought to be commonly applicable to Japan.
In this article, based on the reports mentioned above,
first, the basic information on the damages to the F-
1NPPs by the earthquake and tsunami are summarized.
Then, the plant records during the accident at Units 13
are analyzed to identify key operator actions or physical
phenomena that are not fully understood yet. Finally,
Journal of Nuclear Science and Technology
Volume 49, No. 1, January (2012) pp. 117
http://www.tandfonline.com
*Corresponding author. Email: [email protected]
ISSN 0022-3131 print/ISSN 1881-1248 online
2012 Atomic Energy Society of Japan. All rights reserved.
http://dx.doi.org/10.1080/18811248.2011.636538
http://www.tepco.co.jp/en/nu/fukushima-np/index-e.htmlhttp://www.tepco.co.jp/en/nu/fukushima-np/index-e.htmlhttp://www.tepco.co.jp/en/nu/fukushima-np/index-e.htmlhttp://www.tepco.co.jp/en/nu/fukushima-np/index-e.html -
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based on the insights gained from the analysis, some key
safety issues raised by the accident are discussed.
Since this article focuses on behaviors of reactors at
Units 13 during the early phase of the accident when
radioactive materials were released significantly, other
matters such as behaviors of spent fuel pools and on-site and off-site emergency responses are not discussed.
2. Damages by earthquake and tsunami and plant
behavior
2.1. After the earthquake and before the tsunami
A summary of basic plant information on the F-
1NPPs is shown in Table 1 [1,7]. Each of the Units 15
has a Mark-I primary containment vessel (PCV)
consisting of a dry well (D/W) and a suppression
chamber (S/C), whereas Unit-6 has a Mark-II PCV.
The observed seismic acceleration was mostly
smaller than that of the design basis earthquake Ssof the site. However, at Units 2, 3, and 5, the maximum
acceleration observed for the basemat of the reactor
building in the east-west direction was larger than the
maximum response acceleration to Ss, especially in the
frequency range of 0.20.3 s, by approximately 30% at
the highest. Units 13 scrammed during 14:4647 Japan
Standard Time on high seismic acceleration and almost
simultaneously a loss-of-offsite power (LOOP) took
place. At that time, six out of seven offsite power lines
were connected to the site (one line had been taken out of
service for maintenance) and all of them were lost due to
damages of the breakers at switchyards or other causesincluding the collapse of the steel tower (or pylon) of the
transmissionlines to Units 5 and 6 due to a landslide of a
nearby slope. A total of 12 out of 13 emergency diesel
generators (EDGs) automatically started (one at Unit 4
had been taken out of service for periodic inspection).
After the scram, at Unit 1, the isolation condensers
(ICs) shown in Figure 1 [7] were automatically actuated
on high reactor pressure at 14:52 but were shutdown
manually by closing the motor operated valves
(MOVs), MO-3A and MO-3B, at about 15:03. This
was done according to the operating manual to preventthe cooling rate of the reactor pressure vessel (RPV)
from exceeding 55 K/h [7]. After that, the operators
decided to use only Train A and similar automatic
actuation and manual shutdown were supposedly
repeated three times during 15:17 to 15:34. Then, the
tsunami struck and both alternating current (AC) and
direct current (DC) power supplies were lost at 15:37,
resulting in the valves being inoperable. When the
power supplies were lost, the valves on the ICs
remained as is, that means the MO-3A and MO-
3B remained closed and the others remained open.
The high pressure coolant injection (HPCI) system
with a steam turbine driven pump was not actuated atany of the units because the reactor water level did not
decrease to the set point for its actuation (L-2).
At Units 2 and 3, the reactor core isolation cooling
system (RCIC) was started up automatically at 14:50
and 15:05, respectively, on low reactor water level (L-2).
2.2. Just after the tsunami
Approximately 40 min following the earthquake, at
15:27, the first major tsunami arrived and at 15:35 the
second one; this was followed by multiple additional
waves. The ground level of the site is 10 m above sea
level and the tsunami reportedly reached 45 m aboveground level indicating the inundation height was 14
15 m. It should be noted that the ground level of Units
5 and 6 is about 13 m.
Due to the tsunami, a total of 12 out of 13 EDGs
on-site became inoperable resulting in station blackout
Table 1. Specifications summary of units in F-1NPPs [1,7].
Unit Unit 1 Unit 2 Unit 3 Unit 4 Unit 5 Unit 6
Reactor type BWR-3 BWR-4 BWR-4 BWR-4 BWR-4 BWR-5PCV type Mark-I Mark-I Mark-I Mark-I Mark-I Mark-IIPower output
(MWe gross/net)
460/439 784/760 784/760 784/760 784/760 1100/1067
Contractor GE GE, Toshiba Toshiba Hitachi Toshiba GE, ToshibaFirst commercial
operation(year, month)
1971.3 1974.7 1976.3 1978.10 1978.4 1979.10
Max. pressure ofRPV (MPa)
8.24 8.24 8.24 8.24 8.62 8.62
Max. temperatureof RPV (8C)
300 300 300 300 302 302
Max. pressure ofPCV (MPa)
0.43 0.38 0.38 0.38 0.38 0.28
Max. temperatureof PCV (8C)
140 140 140 140 138 171(D/W) 105(S/C)
No. of EDGs (watercooled/air cooled)
2/0 1/1 2/0 1/1 2/0 2*/1**
Plant status priorto accident In operation In operation In operation Refueling outage Refuelingoutage Refueling outage
Note: *One of them is dedicated to the HPCS; **one was functional after the tsunami.
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(SBO) at Units 14. The air cooled one at Unit 6 that
survived the tsunami supplied power to maintain the
cooling capabilities of the cores and the spent fuel
pools at both Units 5 and 6, since the interconnection
of emergency busbars between two units (namely,
Units 5 and 6, as well as Units 1 and 2, and Units 3 and
4) had been implemented as an accident management
(AM) measure to allow the electric power from the
EDG at one unit being used at the other unit.
There were a total of three air-cooled EDGs two
were inoperable while the one at Unit 6 was operable;
these had been additionally installed in 1994 as part of
AM measures [11]. For Units 5 and 6, there were
originally four water-cooled ones among which one at
Unit 6 was dedicated to the high pressure core spray
system (HPCS) and another one had been shared by
both units. These EDGs were located in the basement
of the respective turbine buildings. The air-cooled one
which functioned after the tsunami had been installedfor Unit 6 on the first floor of the EDG building. For
Units 1 and 2, there were originally only three water-
cooled ones and one was shared by both units. This
situation was the same for Units 3 and 4. Then, an air-
cooled one was installed for each of Units 2 and 4 on the
first floor of the building called the Common Pool for
storing spent fuel. They survived the tsunami but could
not supply power because the metal-clad switchgears,
located in the basement level of their respective turbine
buildings, were damaged by the tsunami. It should be
noted that all the metal-clad switchgears were not
functioning except those at Unit 6.
A total of 12 seawater pumps for residual heat
removal (RHR) for six units, installed outside without
walls, were submerged under seawater, resulting in loss
of the ultimate heat sink (UHS) in all the units.
At Unit 1, the ICs were inoperable after the
tsunami because the MO-3A and MO-3B had been
closed as already mentioned. The HPCI also became
inoperable due to loss of DC power [7].
At Units 2 and 3, the RCICs were operatedfor many hours after the tsunami as is discussed in
Section 4.
Figure 1. Schematic of ICs.
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3. Accident management measures applied
On 28 May 1992, the Nuclear Safety Commission
(NSC) recommended the licensees voluntarily imple-
menting the AM measures [12,13]. Responding to this
recommendation, the licensees had proposed andimplemented the measures, and submitted their report
to the NISA in May 2002, with the results from a
probabilistic safety assessment (PSA) for internal
events for verifying their effectiveness. The NISA
evaluated the submittals from the individual licensees
and compiled the evaluation report in October 2002,
which was reported to the NSC [14].
An example of the measures taken to prevent severe
accidents (SAs) and actually applied in the F-1NPPs
accident is the alternate water injection into the core
shown in Figure 2 [7], where additional pipe lines and
valves were installed to allow the fire protection system
(FPS) and make-up water condensate (MUWC) systemto inject water into the core and PCV through the
emergency core cooling system (ECCS) injection lines.
In addition, a procedure was implemented to reduce
the RPV pressure by opening the safety relief valves
(SRVs), shown in Figure 3 [7], to allow the low pressure
pumps to inject water into the core. Although the use
of fire engines was not part of the measures, they were
actually used in the accident. As is discussed in Section
4, it was difficult to open the SRVs [9], which are air-
operated valves (AOVs), because the operators need
both DC power and compressed air from the instru-
ment air (IA) system.
A second example is what is called wet venting
or hardened venting shown in Figure 4 [15], toprevent the PCV failure from overpressurization in
the case of RHR loss, where a pressure-resistant pipe
line was installed to connect the venting line starting
from the top of the S/C to the exhaust line of the
standby gas treatment system (SGTS) inside the
stack. On this line, there are two AOVs (large and
small) in parallel, though only one is shown in
Figure 4, a MOV and a rupture disc to prevent
inadvertent releases of radioactive materials. In the
accident, the MOV was opened by using its
handwheel and the AOVs were opened by connecting
mobile batteries for opening the solenoid valves, and
air cylinders or mobile compressors for compensatingfor the loss of compressed air. Moreover, the
operators had to repeatedly apply the air cylinder
or mobile compressor since the AOV self-returned to
its closed position due to spring force when the
compressed air was lost [9].
It should be noted that electricity is assumed to be
available for opening the SRVs and valves for wet
venting in TEPCOs AM measures; this is certainly
Figure 2. Schematic of alternate water injection implemented as AM measures and actually applied.
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Figure 3. SRVs and SVs for Units 2 and 3.
Figure 4. Schematic of hardened venting implemented as one AM measure for BWR 4.
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one of the main causes for difficulties to open them in a
timely manner during the accident as discussed later.
4. Accident progression at units 13 after the tsunami
4.1. Unit 1
Figure 5 shows the RPV pressures, D/W pressure,
and volumetric flow rate of either freshwater or
seawater injection into the core. The data such as
pressures and reactor water level taken using the
differential pressure transducer should be carefully
interpreted because the water in the pressure sensing
line might have boiled away as the PCV temperature
rose. The first data point of D/W pressure was 0.6 MPa
at 1:05 on 12 March which had already exceeded its
maximum design pressure (Pd). Although the steam
generated in the core was released to the S/C through
the SRVs as shown in Figure 3, steam alone could not
bring about such a large pressure increase in the D/Wsince the water in the S/C still remained subcooled at
this time. On the other hand, if it is assumed that the
ICs were unavailable after the tsunami, the fuel heat-up
and subsequent zirconium-water reaction would have
started to occur within about 2 h. Then, the mixture of
steam and hydrogen would have been transported to
the PCV through SRVs. Therefore, it is reasonable to
presume that the accumulation of hydrogen in the PCV
contributed to this pressure increase. This presumption
is consistent with the fact that a scribble message
remained on the whiteboard in the main control room,
indicating the radiation monitor indication increasedwhen opening the outside door of the air lock at 17:50
[6]. As well, the radiation level in the reactor building
increased at around 22:00 and also in the turbine
building at around 23:00 [9]. These indicate a leakage
from PCV might have taken place already in the early
phase of the accident, although the reason is not
known yet. The D/W pressure at 2:30 on 12 March was
found to be 0.84 MPa; this was almost double of the
Pd, and sufficiently high for causing a leakage as
discussed later.
Figure 6 shows the D/W pressure calculated with
Containment Vessel Balance (CVBAL) [16] along withthe plant records. As briefly described in Appendix A,
CVBAL is a simple computer program developed by
Japan Atomic Energy Agency (JAEA) taking into
account only mass and energy balances within a single
volume. In this calculation, the amounts of hydrogen
and oxidization heat generated by zirconium-water
reaction were given as inputs by assuming that the total
amount of zirconium in the core reacted with steam.
Although structural heat loss was not taken into
account in this calculation, the initial pressure build-
up in the PCV was underestimated. This indicates that
the hydrogen accumulation was not sufficient to lead to
such a large pressure increase, and therefore, addi-tional causes, for example, direct steam release to D/W
through safety valves (SVs) or rupture of SRV line,
may have occurred. A continuous discharge of gaseous
fluid from the containment was assumed to start twice;
one when the D/W pressure reached the peak and the
other when venting was done, in order to obtain good
agreement with plant records. The former simulated
the leakage from the containment and the latter
simulated the venting.
Returning to Figure 5, the RPV pressure was 0.8
MPa at 2:45 on 12 March, while the pressure recorded
before this data point was 6.9 MPa at 20:07 on 11March. This indicates that the depressurization
occurred between these two times. It should be noted
that there is no written indication that the operators
attempted to open the SRVs during this time period [7].
If that was the case, the RPV depressurization was
caused by the damage of the RPV pressure boundary.
Figure 5. RPV pressures, D/W pressure, and injection water flow rate into core at Unit 1.
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In TEPCOs analysis [7], the molten fuels relocated to
the lower plenum and damage to the RPV occurred
15 h after the earthquake, and this caused the RPV
depressurization. The freshwater injection was started
at 5:46 on 12 March using fire engines. This means that
no water had been supplied to the core for 14 h and9 min after the tsunami. Furthermore, if the pump
heads of the fire engines, for which specifications are
not available, were lower than 0.75 MPa, the core
injection would not have started until the containment
was vented at about 14:00. In that case, no water would
have been supplied to the core for about 22 h.
Figure 7 shows the RPV pressure, D/W pressure,
and dose rate measured with the Main Gate Monitor-ing Post. Soon after the D/W pressure reached the peak
at 2:30 on 12 March 2011, the dose rate started to
Figure 7. RPV pressures and D/W pressure for Unit 1 along with site air dose rate.
Figure 6. D/W pressure calculated with CVBAL and plant records for Unit 1.
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increase. This indicates that the containment leakage
might have started due to overpressure at around this
time. The CVBAL analysis in Figure 6 also indicated
that the assumed occurrence of the containment
leakage reproduced the formation of the pressure
plateau at approximately 750 kPa before the actuationof the S/C venting. The hydrogen that had leaked to
the reactor building during this period might have
caused the explosion, namely deflagration or detona-
tion, at 15:36 on 12 March 2011.
Intension is not understandable for some of the
operator actions such as the RPV depressurization and
use of the ICs as discussed in the following.
The operators had started preparation for alter-
native injection within 1 h after the tsunami, and
recognized the necessity of the depressurization of
RPV for the alternate injection [9]. There is, however,
no description indicating they attempted to open the
SRVs in TEPCOs report [9].The ICs could have been used to remove the decay
heat, delay the core damage, and even depressurize the
RPV, if the operators had used them during the
operation after the earthquake and before the tsunami.
According to TEPCO [9], however, they only checked
the condition of one of the ICs at 18:10, almost 3 h
after the tsunami. Furthermore, after they opened the
MO-2A and MO-3A at 18:18 and confirmed the
actuation by checking steam generation in the second-
ary side, they closed the MO-3A at 18:25 and left it
closed for the next 3 h. Then, they opened it again at
21:30. If the core damage started before 21:30 andwater was not sufficiently supplied to the IC secondary
side, opening of the MO-3A at 21:30 might have
caused the containment bypass due to the overheat of
piping.
Regarding the basic design and use of ICs, there
are several things that should be explained further.
As discussed in Section 2, the operators shut them
down according to the procedures to prevent the
RPV from being overcooled at the rate exceeding 55
K/h. Then, the tsunami rendered them inoperable. It
is stated in the Installment License Application
Document of Unit 1 [17] that the design pressure
of an IC is about 7 MPa and its outlet temperature
is 2868
C. If so, it is hard to understand why such ahigh cooling rate exceeding 55 K/h took place. It is
reasonable to presume that the outlet temperatures
of the ICs were much lower than the design value in
the accident. If this is the case, the basic design
philosophy of the ICs, namely what the originally
intended use of the ICs and how they had actually
been used until this accident occurred, should be
explained.
4.2. Unit 2
Figure 8 shows the RPV pressure, D/W pressure and
S/C pressure, and reactor water level at Unit 2. TheRCIC had been continuously operated during approxi-
mately 3 days and the water level had been maintained
at around the normal value, i.e. approximately
4000 mm above the top of active fuel (TAF). Since
the DC power supply was unavailable, it is understood
that the governor valve to control the steam flow to the
RCIC turbine could not have fulfilled its intended
function (the valve seemed to have been in the open
position due to fail as is per design). Its operation
mode was switched from injection to recirculation from
4:20 to 5:00 on 12 March 2011 and, therefore, both S/C
and D/W pressures increased due to accumulation ofdecay heat.
The RCIC stopped at 13:25 on 14 March 2011, it is
not known why, and then, the water level started to
decrease and the RPV pressure started to increase.
The seawater injection started at 19:54 after the RPV
was depressurized at about 18:00 by opening the
SRVs. The water level recovery could be confirmed
after about 22:00 on 14 March 2011. This means that
Figure 8. RPV pressure, D/W pressure, S/C pressure, and reactor water level for Unit 2.
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it took approximately 4.5 h after termination of the
RCIC to depressurize the RPV, and no water had
been supplied to the core for approximately 6 h and
29 min.
Figure 9 shows the comparison of the recorded
PCV pressures with the calculations by CVBAL. Thebase case without any leakage from the PCV results in
significant overestimation of the D/W and S/C
pressures. In the sensitivity calculation, therefore, a
leakage from the gaseous volume of D/W was assumed
to take place from the beginning of the accident. The
calculation agreed better with the plant record when a
leak diameter of 78 mm-equivalent was applied. The
underestimation of pressure during the early phase in
the sensitivity calculation indicates that further better
agreement could be obtained with assuming delayed
occurrence of leakage. It should be noted that a similar
leakage was also assumed to occur in TEPCOs
analysis [7].
Figure 10 shows the same parameters as those in
Figure 8 in a different time range along with the on-siteair dose rate. From this figure, it can be seen that the
RPV depressurization occurred four times at about
18:30, 21:30, 23:30 on 14 March 2011 and 1:30 on 15
March 2011. The depressurization at the first three
times was probably caused by opening the SRV. The
pressure increase after each depressurization was
caused due to the SRV being closed unintentionally.
When it was opened the second time at about 21:30,
the RPV pressure decreased to about 0.5 MPa and the
Figure 9. D/W pressures calculated with CVBAL along with plant records for Unit 2.
Figure 10. RPV pressure, D/W pressure, S/C pressures, and reactor water level for Unit 2 along with on-site air dose rate.
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water level increased immediately after that, which
indicates that sea water injection was increased by the
depressurization. Concurrently with the second depres-
surization, the dose rate started to increase. This
indicates that a leakage from D/W might have taken
place at this time and also that core damage hadalready started by this time. No pressure increase
after the fourth depressurization indicates either the
SRV was stuck open or the RPV pressure boundary
failed.
It should be noted here that large differences
between the D/W and S/C pressures existed after
about 22:00 on 14 March 2011, which increased to
about 0.4 MPa after about 0:00 on 15 March 2011.
This difference cannot be physically explained con-
sidering the large flow path between the S/C and D/W,
which suggests a measurement error. Since the RPV
pressure after the depressurization was almost the same
as the D/W pressure, the D/W pressure measurement isconsidered to be more reliable. The operators, how-
ever, regarded this pressure difference as the actual
pressure distribution, and decided to use the venting
line from the D/W after they had completed the
preparation of that line from the S/C at 21:00 on 14
March 2011 [9]. Then, they completed the preparation
of that line from the D/W at 0:02 on 15 March 2011.
Several minutes after that, however, they confirmed the
closure of a valve on this line. Consequently, the
venting did not appear to be done due to unintentional
closure of the valves on these lines. No further operator
action has been recorded on venting.An explosive sound was heard at around 6:00 on 15
March 2011. Consistent with this, the dose rate
increased significantly and both D/W and S/C were
depressurized before around 11:00. Since a large
amount of highly contaminated water was identified
in the basement of the turbine building and trench
later, a significant failure might have taken place at the
S/C around this time. These suggest that significant
core damage continued and resulted in depressuriza-
tion of the PCV at around 6:00 to 11:00, although the
amount of injected seawater seems to have been
sufficiently large enough to have cooled the core. This
implies that the actual water injection was not sufficient
because the RPV pressure remained high, approxi-
mately 0.8 MPa. This was because venting could not be
done and the D/W pressure remained high until
around 6:00 to 11:00.
Figure 11 shows the RPV pressure calculated with
the TRAC-BF1 code [18] along with the plant record.
The major models and assumptions applied are
summarized in Appendix B. Figure 12 shows the
sensitivity calculations, where the timing of RPV
depressurization and seawater injection is varied after
termination of the RCIC. The calculation showed that
if the RPV depressurization and seawater injection hadbeen done more than approximately 4 h earlier, core
damage could have been avoided.
4.3. Unit 3
Figure 13 shows the RPV pressure, D/W pressure, S/
C pressure, and reactor water level at Unit 3. At Unit
3, the DC supply was available. The RCIC had been
operated for about 20 h since the tsunami and tripped
at 11:36 on 12 March 2011. Then, the operators started
the HPCI at 12:35 and soon, the RPV pressure started
to decrease to about 10 MPa. TEPCO stated that the
minimum flow line was used to distribute part of the
pump discharge flow to the S/C to ensure the
continuous operation of the HPCI pump without
being tripped-off by the high reactor water level (L8)
according to the operating procedures [19]. Although
the conditions needed for such an operation of the
HPCI are not explained in [19], the reason why the
operating procedures required such an operation
should be clarified because continuous operation of
the HPCI accelerates the consumption of water in thecondensate storage tank (CST) and also causes rather
large depressurization of the RPV due to steam flow to
Figure 11. Numerical results by TRAC-BF1 code (RPVpressure and reactor water level for Unit 2).
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the HPCI turbine. The HPCI suddenly stopped at 2:42
on 13 March 2011. Although this might be caused by
depletion of the batteries according to TEPCOs
report [9], the HPCI turbine would not trip since its
steam stop valve could remain open in case of
battery depletion. As well, a shortage of water in the
CST could be a cause, considering the design flow
rate and the capacity of the tank, but switchover of
the water source from CST to S/C would be
available in case the battery was available. Hence,
the reason why the HPCI tripped should be clarified.
Then, the RPV depressurization and the venting were
carried out at 9:08 and 9:20, respectively, andfreshwater injection was commenced at 9:25, which
was changed to seawater injection at 13:12. This
means that it took approximately 6.5 h after the
HPCI trip to depressurize the RPV and no water
injection into the core had been done for approxi-
mately 6 h and 43 min.
Figure 14 shows the same parameters as those in
Figure 13 in a different time range, compared with the
on-site dose rates measured at the main gate as well as
at the Monitoring Post No. 4 (MP 4) located near Unit
6. Before venting was done at 9:20, the on-site dose
rates started to increase, when the D/W pressure was
more than Pd. This indicates that core damage had
already started and also a leakage from D/W had
started to occur by that time. The first peak in D/Wpressure was caused by rapid steam and hydrogen
ingress through the SRVs.
Figure 12. Sensitivity calculations for Unit 2: Maximum clad temperature as a function of recovery action (depressurization andinjection) timing. Water injection starts after RPV pressure falls to 0.6 MPa.
Figure 13. RPV pressures, D/W pressure, S/C pressures, and reactor water level for Unit 3.
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The vent valve (large) closed before 11:17 due to
loss of compressed air and then the D/W pressure
increased rapidly again. Then, it started to decrease at
about 12:30 when the valve was opened by replacing
the air cylinder with a new one. The second peak ofdose rate at around 14:00 on 13 March 2011 might
have been caused by this venting. At about 20:10, the
vent valve (small) was confirmed open, and consistent
with this, the D/W pressure started to decrease from
around that time. The third peak of the on-site dose
rate at about 2:00 on 14 March 2011 might have been
caused by this venting.
After about 0:00 on 14 March 2011, the D/W
pressure started to increase again, which implies the
vent valves again closed unintentionally (due to lack of
compressed air). Then, it reached more than 0.5 MPa
exceeding Pd, and leakage might have taken place due
to overpressure as indicated by the dose rate measured
at MP 4. Hydrogen leaked during this time period
should have largely contributed to the explosion at the
reactor building of Unit 3 at about 11:00. All the
pressures decreased suddenly immediately after the
hydrogen explosion. The reason should be clarified.
5. Major safety issues raised by the F-1NPPs accident
5.1. Basic understanding
In the Governments report [7], a total of 28 lessons
learned have been identified based on the information
available before June 2011. Most of the issues relevantto these lessons learned, however, are not new and
some of them, for instance, the design basis tsunami,
have been discussed since long before the accident,
although they were not sufficiently addressed to the
extent expected from the state-of-the-art technical
knowledge and findings, and international practices.
For some of the issues such as the beyond design basisevents, discussion had been started rather recently
before the accident. Those insufficiently addressed
issues clearly indicate that appropriate framework
needs to be established to pursue continuous improve-
ment toward the highest standards of safety discussed
as the safety objective in the IAEA Safety Funda-
mentals No. SF-1 [20]. Hereafter, the major safety
issues raised by the accident are discussed from the
international perspective.
5.2. Design basis tsunami
In 2002, TEPCO evaluated the design basis tsunami
height based on the method developed by the Japan
Society of Civil Engineers (JSCE) [21], which is also
reflected in IAEA Tsunami Hazard Guide DS417 [22],
and voluntarily revised it from 3.1 m to a range of 5.4
5.7 m [7]. The IAEA mission pointed out that the
increased design basis tsunami height and additional
measures taken in 2002 were insufficient; moreover,
they were not reviewed and approved by the regulatory
authority.
One of the focal issues here may be that the tsunami
recurrence period is not identified in the method of
JSCE [7]. As mentioned in the IAEA mission report,the design basis usually excludes very remote events or
combination of events those typically with a lesser
Figure 14. RPV pressures, D/W pressure, S/C pressures, and reactor water level for Unit 3 along with site air dose rates.
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probability of occurrence than 1 in 10,000 to 100,000
per year. As stated in the Governments report, some
experts pointed out in 2009 the existence of tsunami
that accompanied the Jyogan Earthquake in 869. This
implies that even if that tsunami would have been
taken into consideration, the occurrence probabilitywould be an order of 1 in 1000 per year.
It should be noted here that the NSC revised the
Seismic Design Review Guide in 2006 [23] and it was
newly required to take into account tsunami as one of
the events caused by earthquake. However, neither the
specific requirements nor guides to deal with these
events have been developed yet.
Considering the uncertainties in predicting earth-
quake magnitudes and subsequent tsunami, it is
insufficient to rely just on the breakwater that protects
the facility against the design basis tsunami. Safety
measures based on the defense-in-depth concept should
have been provided in order to reduce the risksassociated with earthquakes and subsequent tsunami
beyond their respective design bases.
5.3. AM measures
The AM measures implemented in the F-1NPPs
were insufficient as discussed in the previous section.
Although their effectiveness had been assessed by
using PSA, it was only for internal events and did not
include external events such as earthquakes and
flooding. For this reason, the resultant core damage
frequency (CDF), for example, for SBO becamesufficiently low by taking the interconnection of
emergency busbars between units and recovery of
off-site and on-site power supplies into account and,
therefore, it was concluded that any additional mobile
EDGs and batteries were not effective to further
reduce the CDF. This was detrimental because if these
external events had been taken into consideration,
such additional measures would have been effective to
reduce the total CDF since the seismic risk is
apparently dominant in Japan. If PSA methods for
external events were judged to be immatured at that
time, a simplified method or even engineering judg-
ments could have been applied to develop the AM
measures for common cause failures (CCFs) caused
by such events.
From the accident, a lack of consideration was
revealed on concurrent SAs in multiple units in a site,
loss of spent fuel cooling, and hydrogen explosion
outside containment. It is also important to emphasize
the fact that the deteriorated on-site environment caused
by the hydrogen explosion hindered the operator actions
to cope with the accident. The deteriorated off-site
environment and infrastructure by the earthquake and
tsunami hindered transportation of heavy items for
support to the site and communication.One of the weaknesses in the current AM measures
might be the use of plant specific systems. The IC is one
of them for Unit 1. Considering the capability of the IC
which operates without being heavily dependent on the
power supply, AM measures by using ICs could have
been prepared.
The Governments report states: In addition,
accident management measures are basically regardedas voluntary efforts by operators, not legal require-
ments, and so the development of these measures
lacked strictness. Moreover, the guideline for accident
management has not been reviewed since its develop-
ment in 1992, and has not been strengthened or
improved. Since the prime responsibility for safety
rests with the licensees, however, they should have
borne in mind the recognition that best efforts should
be made to ensure the safety of their facilities even on a
voluntary basis.
5.4. Regulatory treatment of beyond design basisevents
In 1992, the NSC recommended the licensees
implement the AM measures on a voluntary basis.
The reason is understood as follows [12]: One of the
legal requirements as criteria for the license stipulated
in Article 24 of the Regulation law is no hindrance to
the prevention of the hazard and compliance with this
requirement is strictly reviewed by, for example,
assuming occurrence of design basis events (DBEs).
For this reason, the risk is considered to be suppressed
to a sufficiently low value and the AM measures to
address SAs, namely beyond DBEs, are to reduce therisk further: therefore, no additional regulatory action
is required.
It is stated in the US NRCs task force report
frequently, the concept of DBEs has been equated to
adequate protection, and it has been equated to beyond
adequate protection (i.e. safety enhancements). This
situation seems to be similar to that mentioned above.
However, the US NRC has made regulatory rules that
address beyond DBEs (BDBEs) such as those regard-
ing SBO and anticipated transient without scram
(ATWS). The SBO rule [24], for example, was issued
in 1988.
Contrary to this, in Japan, such rules have never
been made. Regarding SBO, for example, Criterion 27
in the regulatory guide for reviewing the safety design
of light water nuclear power reactor facilities requires
design measures to cope with a short time SBO to
ensure safe shutdown and decay heat removal [25]. In
other words, the extended loss of off-site power did not
need to be considered since it was generally recognized,
at that time, that the reliabilities of both off-site power
and EDGs in Japan were higher than those in the US.
As well, Criterion 27 was intended to assure that the
turbine-driven pump systems, such as RCIC and HPCI
of BWRs and auxiliary feedwater system (AFW) ofPWRs, could cope with the short-term SBO situations.
The SBO rule in the US, on the other hand, requires
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them to cope with a long-term SBO considering
external hazards such as heavy snow fall, tornados,
and hurricane winds.
The IAEA draft Safety Requirements DS414 [26]
for revision of Safety Standards Series No. NS-R-1
requires the design extension conditions (DECs) forbeyond design basis accidents. Similarly, the US NRC
task force concluded that the application of defense-in-
depth should be strengthened by formally establishing,
in the regulations, an appropriate level of defense-in-
depth to address requirements for extended design-
basis events; many of the elements of such regulations
already exist in the form of the SBO rule, ATWS rule,
and others.
There may be several reasons why such rules have
never been established in Japan. One of them seems to
be that the operating experience feedback has been
insufficient. As mentioned above, in the US, the SBO
rule was developed in the 1980s and in someEuropean countries such as Sweden, additional power
generators such as mobile gas turbine generators are
installed on-site in order to cope with the SBO.
However, there has been no discussion on the SBO
since 1994 in Japan.
Another reason might be related to so-called
backfitting. In the US, the backfitting rule [27] provides
bases for determining whether or not backfitting is
required at individual facilities and the NRC requires
the backfitting of a facility only when it determines,
based on the analysis, that there is a substantial
increase in the overall protection of the public healthand safety or the common defense and security to be
derived from the backfit and that the direct and
indirect costs of implementation for that facility are
justified in view of this increased protection.
In European countries, the backfitting is being dealt
with in a 10-yearly safety reassessment referred to as a
periodic safety review (PSR) [28] which includes an
assessment of plant design and operation against
current safety standards and practices, with the
objective of ensuring a high level of safety throughout
the plant operating lifetime.
The Governments report stated: the Government
will clarify technical requirements based on new laws
and regulations or on new findings and knowledge for
facilities that have already been approved and licensed,
in other words, it will clarify the status of retrofitting in
the context of the legal and regulatory framework.
Here, it seems that retrofitting corresponds to
backfitting.
The introduction of AM measures on a voluntary
basis in 1992 may be warranted in the beginning,
considering immaturity of the understanding of SAs
and PSA results showing very low occurrence frequen-
cies of SAs without any AM measure at that time. The
fact that the regulatory position on the AM measureshas never been improved since then, however, clearly
shows that a framework is needed to pursue
continuous improvement toward the highest standards
of safety on both regulatory and industry sides.
5.5. Framework that pursues the highest standards of
safety
In order to establish a framework that pursues the
highest standards of safety that can reasonably be
achieved, it is obvious that the commitments of the
licensees are necessary because the prime responsibility
of safety rests with them.
The regulatory bodies, however, also play important
roles, as well. One of them is to implement clear
regulatory requirements including review guides, stan-
dards, and other relevant documents based on the state-
of-the-art technical knowledge and findings. Such
requirements should, in principle, have legal bases.
Although it may take time to develop such requirements
to resolve a certain issue, the regulatory bodies shouldrecommend or require the licensees to take measures
regardless of a legal or a voluntary basis, if the measures
have an impact on safety. Even on a voluntary basis, as
well, the regulatory bodies may examine the licensees
commitment to implement some of them for enhancing
safety through the review process.
It is of prime importance, furthermore, to continue
to reflect national and international operating experi-
ence, results from safety research worldwide, and
evolution of international safety standards to such
requirements and recommendations.
6. Concluding remarks
Japan needs to establish a framework toward
continuous improvement to pursue the highest stan-
dards of safety that can reasonably be achieved as
described in the IAEA Safety Fundamentals No. SF-1
[20]. Since the prime responsibility for safety rests with
the operating organizations, the licensees need to make
their best effort for continuously improving safety on a
voluntary basis. The major role of the regulatory body
is to have oversight on the licensees efforts and to
revise and backfit the regulatory requirements based on
the state-of-the-art technical knowledge and findings in
accordance with an appropriate rule, if a substantial
increase is clearly expected in the overall protection of
the public health and safety, and the environment.
In order to achieve continuous improvements, all
the entities relevant to nuclear safety such as industries,
regulatory bodies, research organizations, and univer-
sities have to discuss ways to seek the effective frame-
work for this purpose, thoroughly taking the publics
involvement into account.
Furthermore, external stimulation plays a vital role
as a driving force to make the framework actually
functional toward the highest level of safety. Thisexternal stimulation might include pursuing compli-
ance with IAEA Safety Standards and also
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contributing to development of such Standards. Peer
reviews within the frameworks of the Convention on
Nuclear Safety (CNS) [29] and IAEA services such as
the IAEA Integrated Regulatory Review Service
(IRRS) [30] may be effective as an external stimulation.
The contracting parties of the CNS have alreadyproposed to hold a dedicated meeting in 2012 on the F-
1NPPs accident aiming at sharing the lessons learned
and at reviewing the effectiveness and, if necessary, the
continued suitability of the provisions of the CNS [31].
References
[1] NISA, JNES, The 2011 off the Pacific Coast of TohokuPacific Earthquake and the Seismic Damage to the NPPs,NISA and JNES (2011). Available at http://www.nisa.meti.go.jp/english/files/en20110406-1.html.
[2] NISA, NISA News Release, 26 April, NISA (2011).Available at http://www.nisa.meti.go.jp/english/press/
index.html.[3] TEPCO, TEPCO Press Release, May 16, TEPCO
(2011). Available at http://www.tepco.co.jp/en/press/corp-com/release/.
[4] NISA, NISA Press Release, May 17, NISA (2011) [inJapanese]. Available at http://www.nisa.meti.go.jp/earthquake_index.html.
[5] TEPCO, TEPCO Press Release, May 24, TEPCO,Tokyo, Japan, 2011.
[6] NISA, NISA News Releases, May 24 and June 6, NISA,2011.
[7] Nuclear Emergency Response Headquarters Govern-ment of Japan, Report of the Japanese Government to theIAEA ministerial conference on nuclear safety, Govern-ment of Japan, 2011.
[8] IAEA, IAEA International Fact Finding Expert Mission ofthe Fukushima Dai-ichi NPP Accident Following the GreatEast Japan Earthquake and Tsunami, IAEA, Vienna,Austria, 2011.
[9] TEPCO, TEPCO Press Release, June 18, TEPCO,Tokyo, Japan, 2011.
[10] C. Miller, A. Cubbage, D. Dorman, J. Grobe, G.Holahan, and N. Sanfilippo, Recommendations forEnhancing Reactor Safety in the 21st Century, USNRC, Maryland, United States, 2011.
[11] Subcommittee on Safety Design Review Guide [inJapanese], Doc.No. 2-1, August 3, NSC (2011). Avail-able at http://www.nsc.go.jp/senmon/shidai/anzen_sekkei/anzen_sekkei2/siryo2-1.pdf.
[12] NSC, On Accident Management as Measures against
Sever Accidents in Light Water Reactor Facilities [inJapanese], approved by NSC on May 28 (1992).Available at http://www.nsc.go.jp/shinsashishin/pdf/1/ho016.pdf.
[13] NSC, Resolution by NSC [in Japanese], May 28, NSC,1992.
[14] Government of Japan, Convention on Nuclear SafetyNational Report of Japan for the Fifth Review Meeting,Tokyo, Japan, Government of Japan, 2010.
[15] TEPCO, TEPCO Press Release [in Japanese], March 26,TEPCO, Tokyo, Japan, 2004.
[16] Y. Sibamoto, K. Moriyama, and H. Nakamura,Examination of the containment vessel conditions duringthe Fukushima Daiichi NPP accident by simple heat andmass balance model [in Japanese], Transactions of 2011
Fall Meeting of the Atomic Energy Society of Japan,1922 September 2011, Kita-Kyushu, Japan. AESJ:Tokyo, Japan, p. 42, (2011).
[17] TEPCO, The Installment License Application Documentof Unit 1 of Fukushima Dai-ichi Nuclear Power Plant[in Japanese], TEPCO, Tokyo, Japan, 1966.
[18] M.M. Giles, G.A. Jayne, S.Z. Rouhani, et al., TRAC-BF1/MOD1: An Advanced Best-Estimate ComputerProgram for BWR Accident Analysis, NUREG/CR-4356, US NRC, Maryland, United States, 1992.
[19] TEPCO, TEPCO Handouts at Press Conference, July 28,TEPCO (2011). Available at http://www.tepco.co.jp/en/nu/fukushima-np/handouts/index-e.html.
[20] IAEA, Fundamental Safety Principles, Safety Funda-mentals No. SF-1, IAEA, Vienna, Austria, 2006.
[21] Tsunami Evaluation Subcommittee, Nuclear CivilEngineering Committee, Tsunami Assessment Method
for Nuclear Power Plants in Japan, JSCE, Tokyo, Japan,2002.
[22] IAEA, Meteorological and Hydrological Hazards in SiteEvaluation for Nuclear Installations, Draft Safety GuideDS417, IAEA, Vienna, Austria, 2009.
[23] NSC, Regulatory Guide for Reviewing Seismic Design ofNuclear Power Reactor Facilities, NSC, Tokyo, Japan,2006.
[24] US NRC Regulations, Title 10 Code of FederalRegulations, Section 50.63 Loss of All AlternatingCurrent Power, 53 FR 23215, US NRC, Maryland,United States, 1988.
[25] NSC, Regulatory Guide for Reviewing Safety Design ofLight Water Nuclear Power Reactor Facilities, NSCRG:L-DS-1.0, NSC, Tokyo, Japan, 1990.
[26] IAEA, Safety of Nuclear Power Plants: Design, DraftSafety Requirements DS414, Revision of Safety Stan-dards Series No. NS-R-1, IAEA, Vienna, Austria, 2010.
[27] US NRC Regulations, Title 10, Code of FederalRegulations, Section 50.109 Backfitting, 53 FR 20610,US NRC, Maryland, United States, 1988.
[28] IAEA, Periodic Safety Review of Nuclear Power Plants,
Safety Guide No. NS-G-2.10, IAEA, Vienna, Austria,2003.[29] IAEA, Convention on Nuclear Safety, INFCIRC/449,
IAEA, Vienna, Austria, 1994.[30] IAEA, Integrated Regulatory Review Service, IAEA.
Available at http://www-ns.iaea.org/reviews/rs-reviews.asp.
[31] L. Ganjie, SummaryReport of the 5thReviewMeeting of theContracting Parties to the Convention on the Safety onNuclear Safety, CNS/RM/2011/6/Final, IAEA, Vienna,Austria, 2011.
[32] K. Moriyama, Y. Maruyama, and H. Nakamura, SteamExplosion Simulation Code JASMINE v.3 Users Guide,JAEA-Data/Code 2008-014, Japan Atomic EnergyAgency, Ibaraki, Japan, 2008.
[33] T. Watanabe, M. Ishigaki, A. Sato, and H. Nakamura,Analysis of BWR station blackout accident[in Japanese], J. At. Energy Soc. Jpn. 10(4) (2011), pp.240244.
Appendix A
A model, CVBAL, illustrated in Figure A1 was developedfor estimation of accident conditions inside the PCV fromobserved pressure and temperature trends based on roughassumptions. It often happens that an application of moresophisticated codes needs much more time and labor for thepreparation of input data and running the calculation. Also,they are not necessarily suitable for handling low pressuresubcooled conditions. Thus, such a simple program with a
simple method may be highly useful.A set of conservation equations, exit conditions, and
numerical solution method are summarized below. The
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http://www.nisa.meti.go.jp/english/files/en20110406-1http://www.nisa.meti.go.jp/english/files/en20110406-1http://www.nisa.meti.go.jp/english/press/indexhttp://www.nisa.meti.go.jp/english/press/indexhttp://www.tepco.co.jp/en/press/corp-com/release/http://www.tepco.co.jp/en/press/corp-com/release/http://www.nisa.meti.go.jp/earthquake_indexhttp://www.nisa.meti.go.jp/earthquake_indexhttp://www.tepco.co.jp/en/nu/fukushima-np/handouts/index-ehttp://www.tepco.co.jp/en/nu/fukushima-np/handouts/index-ehttp://www-ns.iaea.org/reviews/rs-reviews.asphttp://www-ns.iaea.org/reviews/rs-reviews.asphttp://www-ns.iaea.org/reviews/rs-reviews.asphttp://www-ns.iaea.org/reviews/rs-reviews.asphttp://www.tepco.co.jp/en/nu/fukushima-np/handouts/index-ehttp://www.tepco.co.jp/en/nu/fukushima-np/handouts/index-ehttp://www.nisa.meti.go.jp/earthquake_indexhttp://www.nisa.meti.go.jp/earthquake_indexhttp://www.tepco.co.jp/en/press/corp-com/release/http://www.tepco.co.jp/en/press/corp-com/release/http://www.nisa.meti.go.jp/english/press/indexhttp://www.nisa.meti.go.jp/english/press/indexhttp://www.nisa.meti.go.jp/english/files/en20110406-1http://www.nisa.meti.go.jp/english/files/en20110406-1 -
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water-vapor state is calculated by a fast running wide rangesteam table program developed for JASMINE code [32].The ideal gas equation was used for non-condensable gases(e.g. N2, H2) with the zero point of the energy placed at273 K.
Mass conservation equations
Mass conservation for component k (k v,l,n,ni,lc) isexpressed by the following equations,
dmv
dt _miv _mov _mev; A1
dml
dt _m0il _m
0ol _m
0ev _m
0lex; A2
dmlc
dt _milc _molc _mlex; A3
dmn
dt _min _mon; A4
dmni
dt _mini _moni; A5
mv rvVg;ml rlVl; mlc plcVlc; mn rnVg; mni rniVg;A6
Vt Vg Vl Vlc const:; A7
where,
mk: mass of component k,_mik, _mok: mass flow rates of flow-in (ik) and flow-out (ok)
of component k,_mev: evaporation rate of water,_mlex: mixing rate of the subcooled water into the
saturated water,Vt, Vg, Vl, Vlc: total, gas and water volumes,rk: density of component k.
Subscripts v, l, lc, n, and ni for component k indicate,
v: vapor,l: water (saturated),lc: water (subcooled),n: non-condensable gas injected from outside (e.g. N2),ni: non-condensable gas produced inside the volume (e.g.
H2).
Energy conservation equations
Energy conservation equations are expressed as,
E mvev mlel mlcelc mnen mnieni; A8
dE
dt Wgi Wgo pt
_mil
ril
_milc
rilc
pt
_mol
rl
_molc
rlc
_miveiv _mileil _minein _minieini _milceilc
_movev _molel _monen _monieni _molcelc
X
k
QK
A9
where,E: total internal energy in the system,ek: internal energy of component k,rik: densities of flow-in fluids (at the total pressure and
the temperature of each flow-in fluid),pt: total pressure of the gas phase (pvpnpni).
For the terms in the right-hand side of Equation (A9),the first line means the work at the inlet and outlet, thesecond and third lines mean flow-in and flow-out of theinternal energy, respectively, and the last one means the heatinput.
Exit conditions
The flow rate is expressed by the following, with the holearea (A), density, and the velocity (u),
_mok Aru: A10
The velocities of gas components are assumed common(uniform mixture).
The Bernoullis law for incompressible fluids is used forthe liquid phase,
u ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
2p p0=rkp
; A11
where, p0: outside pressure.The generalized Bernoullis law with compressibility
is used for the gas phase with consideration on the criticalflow,
u
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi2gg1
ptrt
p2=gr p
g1=gr pr > pc
qffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
ptrtg
2g1
g1g1
rpr pc
8>: A12
pr p0=pt;pc 2
g 1
gg1
; A13
where,rt: total density of the gas phase (rv rn rni),g: specific heat ratio of the gas mixture,
pc: critical pressure.
Figure A1. Mass and energy balance model for theevaluation of pressure and temperature based onassumptions of PCV situation during the accident.
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Numerical solution method
(1) Integrate the mass conservation equations fromEquations (A1)(A5) and energy conservation equa-tion of Equation (A9) with an explicit integrationscheme in terms of time, obtain the mass of eachcomponent and the total internal energy at the new
time step, except that the phase change term,_mevDt Dmev, in Equations (A1) and (A2) is left
unsolved with implicit scheme as follows,
mvn1 Dmn1ev m
v m
nv Dt _miv _mov;
A14
mn1l Dm
n1ev m
l m
nl Dt _mil _mol _mlex:
A15
Superscripts (n), (n+1) denote old and new timestep variables, * denotes the intermediate values of
mass changes except the phase change.(2) Total internal energy at the new time step is expressedas the sum of specific internal energies of componentsthat are unknown.
En1 mv Dmn1ev
en1v m
l Dm
n1ev e
n1l
mn1lc e
n1lc m
n1n e
n1n m
n1ni e
n1ni :
A16
The known masses except Dmev are substituted inthis equation.
(3) Solve the conservation and state equations at the newtime step by the Newton method and obtain thephase change mass, pressures, and volumes.
Appendix B
The analysis of a long-term station blackout accident of aBWR has been performed using the TRAC-BF1 code, andthe results were compared with the observed data at the F-1NPP Unit 2 [33]. As shown in the noding diagram in FigureB1, the RPV thermal hydraulics from the feed water line tothe steam line were modeled. Although Unit 2 was a BWR-4
with 780 MW output, the analysis was based on a BWR-5with 1100 MW by scaling the feed water flow rate with thepower ratio. Since the power-to-volume-ratio and the relativevolume distribution in the RPV are almost the same betweenthe two reactors, thermal hydraulic responses are expected tobe conserved. The reactor scram due to the earthquakeacceleration and the station blackout sequence were assumedto occur. The RCIC was actuated under the assumption thatthe steam flow rate to the RCIC turbine and the injectionflow rate from the RCIC pump were both balanced with thereactor power. The steam line and the feed water line shownin Figure B1 were used for the RCIC. The RCIC wasterminated at 250,000 s, and depressurization using the SRVwas performed at 270,000 s, according to the event sequenceat Unit 2. Although the reactor type and the power weredifferent, the reactor pressure and the core liquid level were ingood agreement with the observed data [33]. This mayindicate the appropriateness of the above-mentioned scalingconsideration.
Figure B1. TRAC-BF1 noding diagram.
Journal of Nuclear Science and Technology, Volume 49, No. 1, January 2012 17