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Transcript of n *m * u m npfi - International Nuclear Information System (INIS)
JAERI-Research—97-022 JP9704010
JAERI-Research97-022
JP9704010
n *m * u m npfiJapan Atomic Energy Research Institute
VOL 'i 3 k 1
Ar-WlBJftiHi-li. ll««VJj«mW:fttfi# lW:ftM«.S (T319-11 4«JWtftt-fl|5MH) fox, fcf1iLSL</i'^iv, ftfc
This report is issued irregularly.
Inquiries about availability of the reports should be addressed to Research Information
Division, Department of Intellectual Resources, Japan Atomic Energy Research Institute,
Tokai-mura, Naka-gun, Ibaraki-ken, 319-11, Japan.
©Japan Atomic Energy Research Institute, 1997
JAERI-Research 97-022
Proposal of Safety Design Methodologies for an HTGR-hydrogen Production System
(Mainly on Countermeasures against Fire and Explosion)
Tetsuo NISHIHARA, Kazuhiko HADA and Syusaku SHIOZAWA
Department of Advanced Nuclear Heat Technology
Oarai Research Establishment
Japan Atomic Energy Research Institute
Oarai-tnachi, Higashiibaraki-gun, Ibaraki-ken
(Received February 13, 1997)
Among key issues of the safety design for an HTGR-hydrogen production system is to
ensure the safety of the nuclear reactor against fire and explosion accidents in the
hydrogen production plant. The fire and explosion accidents in the hydrogen production
plant are categorized into the following two cases; Accidents inside the reactor
building (R/B) and accidents outside the R/B.
Against accidents inside the R/B, the proposed safety design concept is to prevent the
occurrence of the accidents based on the defence in depth concept. The piping system
and/or heat transfer tubes which have the potential possibility of combustible materials
ingress into the R/B due to the failure are designed at the highest aseismic level to
prevent the failure against severe earthquake. Even if the failure occurs, the piping
trench and related compartments are fulfilled with nitrogen so as to prevent the
occurrence of accidents.
The proposed safety design concept for the accidents outside the R/B is the mitigation
of effects of accidents. Proposed countermeasures is to take the safe distance between
the hydrogen production plant and the items important to safety in the nuclear plant. We
showed that the anticipated accidents to estimate the safe distance are large scale
pool burning, fireball, pressure vessel burst and vapor cloud explosion. Especially,
new estimating concept to establish the safe distance is proposed for the vapor cloud
explosion. To reduce the safe distance, we proposed the underground non-pressurized
storage tank and ventilation system for the storage of large amount of combustible
JAERI-Research 97-022
liquid.
Keywords: HTGR, Hydrogen Production System, Safety Design Concept, Fire, Explosion,
Defence In Depth, Safe Distance, Pool Burning, Fireball, Pressure Vessel
Burst, Vapor Cloud Explosion
NEXT PAQE(S)loft BLANK
JAERI-Research 97-022
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JAERI-Research 97-022
Contents
1. Introduction 1
2. Safety Design Concept of an HTGR-hydrogen Production System 3
2. 1 System Arrangement 3
2. 2 New Anticipated Events for an HTGR-hydrogen Production System 4
2. 3 Safety Design Concept against Fire and Explosion 7
3. Survey of Safety Design Regulations against Fire and Explosion 10
3. 1 Safety Design Regulations for Nuclear Power Plant 10
3. 1. 1 Regulations in Japan 10
3. 1. 2 Regulations in Overseas Countries 12
3. 2 Safety Design Regulations for Non-nuclear Chemical Plant 14
3.2.1 Kouatsugasu Torishimari Hou 14
3.2.2 Syoubou Hou 15
3.2. 3 Sekiyu Konbinato~tou Saigaiboushi Hou 16
3.2.4 Roudouanzen-eisei Hou 17
3. 2. 5 Safe Distance in Japanese Regulations 18
3. 3 Comparison of Safety Design Regulations 19
4. Proposal of Safety Design Criteria against Fire and Explosion
inside the Reactor Building (R/B) 38
4. 1 Occurrence Prevention 39
4. 2 Countermeasures for the Beyond Design Basis Accident 40
4. 3 Proposed Safety Design Criteria for the Accident inside the R/B 41
5. Proposal of Safety Design Criteria against Fire and Explosion
outside the R/B 45
5. 1 Fire and Explosion in the Hydrogen Production Plant 45
5. 1. 1 Explosion Caused in the Vessel 45
5. 1. 2 Fire and Explosion in the Plant Area 48
5.2 Safe Distance 50
5.2. 1 Distance against Large Scale Pool Burning 51
5.2.2 Distance against Fireball 53
5.2. 3 Distance against Pressure Vessel Burst 55
5.2.4 Distance against Vapor Cloud Explosion 58
5. 2. 5 Proposal for Reducing Safe Distance 64
VII
JAERI-Research 97-022
5. 3 Proposed Safety Design Criteria for the Accident outside the R/B 66
6. Conclusions 102
Acknowledgements 106
References 107
Appendix Development of Vapor Cloud Explosion Analysis Code 109
Vlll
JAERI-Research 97-022
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C/V R/B
R/B : Reactor buiIding
C/V : Containment vessel
I/V : Isolation valve
ECR : Endothermic chemical reactor
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JAERI-Research 97-022
Table 3.1 Safety design guideline for fire and explosion in nuclear power plant
±
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JAERI-Researeh 97-022
Table 3.2 Safety design guideline for fire and explosionin kouatsugasu-torishimarihou (13) (1/3)
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JAERI-Researdi 97-022
Table 3.2 Safety design guideline for fire and explosionin kouatsugasu-torishimari-hou (l3> (2/3)
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JAERI-Research 97-022
Table 3.2 Safety design guideline for fire and explosionin kouatsugasu-torishimari hou (13> (3/3)
a
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24 -
JAERI-Research 97-022
Table 3.3 Safety design guideline for fire and explosion in S y o u b o u h o u < M ) (1/3)
Ci
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JAERI-Rcsearch 97-022
Table 3.3 Safety design guideline for fire and explosion in S y o u b o u - h o u < l 4 ) (2/3)
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JAERI-Research 97-022
Table 3.3 Safety design guideline for fire and explosion in Syoubou-hou (14> (3/3)
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JAERI-Researdi 97-022
Table 3.4 Safety design guideline for fire and explosionin Roudouanzeneisei-hou (lfi) (1/2)
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JAERI-Research 97-022
Table 3.4 Safety design guideline for fire and explosionin Roudouanzen-eisei-hou < 1 G ) (2/2)
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JABRI-Research 97-022
Table 3.5 Safe distance in Kouatsugasu-torishimari-hou ( 1 7 ) ( I B ) (1/2)
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JAERI-Research 97-022
Table 3.5 Safe distance in Kouatsugasu-torishimari-hou (1 7) (I 8) (2/2)
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JAERl-Research 47-022
Table 3.6 Safe distance in Syoubou-hou (M> (1/2)
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JAERI-Research 97-022
T a b l e 3 . 6 Safe d i s t a n c e in Syoubou-hou (14> ( 2 / 2 )
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JAERI-Research 97-022
Table 3.7 Explosion contribution ratio (1 9)
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- 64 -
JAERI-Rescarch 47-022
5. 3
9
(1)
(5.3)
(2)
5.1
i f S > ^ U - h
(3).10)~(5. 12), Fig. S- 5.5
(4) ^5
i f So^ ^(5.17)
5.L, ^(5.28)> (5.f J 4 fFig. 5.
- 66 -
JAKRI-Research 97-022
Table 5.1 Emissive power of fire per unit surface area (22)
t> 7 vWcfo
* ] " / *
tltt
Jtnfe
n — +"V"
y ^y-;u
x^y-,u
LNG (y
Xf-ly >
7°O^>
7° D t° U >
n-7^>
^ 7 + /
>
D
4
5
5
4
2
6
8
1
7
1 3
7
7
8
j&fc
<
0.
8.
0.
1.
3.
1.
4.
9.
1.
5.
3.
4.
3.
2.
3
7
1
0
8
2
6
8
7
6
5
7
4
2
5
mm0
0
4
0
6
6
3
8
7
3
8
2
2
6
G
(k
D
1
1
1
1
1
2
1
7
4
2
2
2
W/m2 )
2=3 0
2. 7 9
7. 4 4
5. 1 2
2. 7 9
6.9 8
8. 6 0
5. 5 8
9. 7 7
1. 6 3
5. 5 8
0.7 0
2.0 9
2. 0 9
4. 4 2
D : (m)
- 68 -
Table 5.2 Effects of thermal radiation (2 7)
to
I
Radiation Intensity(kW/m2)
37.5
25.0
12.5
9.5
4.0
1.6
Observed Effect
Sufficient to cause damage to process equipment
Minimum energy required to ignite wood at indefinitely long exposures
Minimum energy required for piloted ignition of wood,melting of plastic tubing
Pain threshold reached after 8 secSecond degree burns after 20 sec
Sufficient to cause pain to personnel, if unable to reach coverwithin 20 secHowever, blistering of the skinCsecond degree burns) is likely0% lethality
Will cause no discomfort for long exposure
>m73
Table 5.3 Survey of experimental researches on fireball generation
Scale
Small
Large
Researchers
Fay and Lewis (30)
Hardee et al. (31)
Hasegawa and Sato l32)
Lihou and Maund l33)
High (34)
Hardee and Lee ( 3 5 )
Maurer et al. <36)
Johnson et al. (371
Containment
Soap bubble
Polyethylene bags
Glass spherepressurized
Soap bubbles
Pressurized tank
Pressurized tank
Fuels
CH4C2H6
CH4
C5H12
C4H10CH4
LocketFuel
C 3118
C3H6
C4H1 0Cans
Fuel Massmf(kg)
20-190(cnf)
0.1-1
0. 3-30
1. 5-6(g)
1-5000
1, 29, 454
0.1-452
1000-2000
Durationt (s)
0.4-0.8
1. 8-2. 4
0. 8-1. 7
0. 5-1. 00. 4-0. 7
1.5
4. 5-9. 2
DiameterD (m)
0. 2-0. 7
1. 5-2. 2
2.7-15
0. 4-0. 80. 3-0. 6
40
56-88
Emiss. Power(kW/irf)
3220
123
110-413
320-375
73
Table 5.4 Empirical relationship of duration and diameter of fireball
Scale
Small
large
Litera-ture
Researchers
Fay and Lewis (30)
Hasegawa and Sato (32)
Moorhouse and Pritchard <38)
Lihou and Maund (33)
Lihou and Maund <33)
Williamson and Mann (39)
Roberts u0)
Pietersen (41), Pitblado(42)
Fuel
C3H8
C5H12
C5H12
CH4
C3H6
C3H8
Data Source
Experiments
Experiments
Hasegawa and Sato
Hardee et al.
Maurer et al.
Hardee and Lee
Literature and model
Literature
Diameter(m)
6.28m,1/3
5.28m,° 277
5.33m,° 327
6.36m,° 325
3.51m,'/3
5.88m(1/3
5.8m,1/3
6. 48m, °- 325
Duration(s)
2.53m,I/6
1.10m,0 181
1.09m,0- 327
2.57m,° l67
0.32m,1/3
1.09m,'/6
0.45m,1/3
0. 825m, ° 2o
m2E50
m, : Constant initial fuel mass(kg)
JAERI-Research 97-022
Table 5.5a Adjustment factors for cylindrical vesse (4 1)
0.
3.
3S
5<
R
RRR
<0.
S3.
3
5
Mult
411
iplier
. 0
. 6
.4
Table 5.5b Adjustment factors for slightly elevated above ground (44)
R
R S1.0
1. 0< R
M u l t i p l i e r
2.0
1. 1
- 72 -
T a b l e 5.6 V a p o r cloud p r o d u c t i o n m e c h a n i s m for d i f f e r e n t c o n d i t i o n of c o m b u s t i b l e m a t e r i a l s
w
Am
/nn
Am
/mt
-ar .;E
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E
m
m E
n E
B.
m it :A
m70
JAERI-Research 97-022
•R
LO >—I •—I .—It— CO OO OOCT3 CT> CX> CT3
H 04 XW X
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CT5 - I - ]
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Gs
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G G GK K K
-Hfr
- 74 -
Table 5.8 Atmospheric stability (5 3)
I
mm (u)
m / s
U< 2
2 SU< 3
3 ^ U < 4
4 ^U< 6
6 ^U
01*« ( T ) kW/rrf
T^O. 60
A
A - B
B
C
C
0. 60 >T^0.30
A - B
B
B - C
C-D
D
0. 30 >T20.15
B
C
C
D
D
0.15>T
D
D
D
D
D
mm$L%m (Q) kW/nf
-0.020
D
D
D
D
D
- 0 . 020 >Q^-0 .040
G
E
D
D
D
-0.040
>Q
G
F
E
D
D
jo
A-B. B-C, C-D(i^n€'tlB> C>
Table 5.9 Diffusion parameter in the method of Sakagami (5 4)
Ien
£ 5E(F )
(D)
(C)
(B)
h (m)
0.5
10
20
30
0.5
10
20
30
0.5
10
20
30
0.5
10
20
30
0A
4.78X10-'
4.78X10-'
4.78x10"'
4.78X10"2
1. 48x10"'
1. 09X10-'
1. 01X10-'
0.97X10"'
4. 50X10"3
2.12X10-3
1.80X10"3
1.61X10"3
1.12X10"3
2. 52X10"4
1.78X10-4
1.44X10"4
/~qA
4.26
4.26
4.26
4.26
1.56X10'
2.18x10'
2.37x10'
2.48x10'
7.59x10'
1.59X10'
1.88X10'
2.09x10'
2.77x10'
1.24X103
1.73X103
2. HxlO3
0B
4.20X10"'
4.60X10-2
4.71x10- '
4. 77X10"2
1. 10x10-'
2.46X10"'
3.00x10"'
3.29x10"'
4.25X10"3
1.48X10-'
1.98X10-2
2. 34X10"2
1. 30X10-3
7.20X10"3
1.10x10"'
1.40x10"'
Q B
3. 50X10-'
2.93X10"'
2. 86X10-'
2. 83X10-'
5.30
1.02
7. 00X10-'
5.65X10"'
3.48x10'
2.87
1.61
1.14
3.73X102
1.18X10'
5.19
3.21
m
50
JAERI-Rcsearch 97-022
T a b l e 5 . 1 0 L o w e r l i m i t o f e x p l o s i v e f u e l - a i r d e n s i t y (B 5)
TW|,y
j-9 J -Jl
x-9 y
if- u >
* *
1
1
%
2. 5
5. 0
2. 5
3. 3
3. 0
2. 7
4. 0
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m K «
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>-tf" y
9 y
9 /-H
1.
2.
2.1
1 .
6.
>
8
1
4
2
3
0
7
Table 5.11 Constants in Eq (5.23) (5fi)
B
D
F
a
0.844154
1.55211
2.31381
b
0. 0438042
0.0399075
0.0492857
c
-0. 0181337
-0. 00725134
0.0128593
d
0. 0035282
0.00325316
0.00277179
- 77 -
JAERI-Research 97-022
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- 78 -
Table 5.13 Safe distance against four anticipated accidents at HTGR-hydrogen production system (1/2)
I
E=R (
E :
R f .•( E q . ( 5 . 3 ) )
2. 3 k W / m1 7 5 °C ( 3 > ? U - h:
17 5m
= 3 7 5 ( D / 2 r ) 2
Eq . (5. 5) ~ ( 5. 7))D :r :
t : mE q. (5. 8 ) , ( 5. 9 )
t x E 4 / 3 =5 0 0
B L E V E
8 5 0m
E q.(5.10) ~ (5 .12 ) . Fig. 5. 6r Kfctf £«H£A P s
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JAERI-Rescarch 97-022
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- 80 -
JAERI-Research 97-022
1000
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>
ca)
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CD'-TD
CO
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start of 2°
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age c
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k
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100
Fig. 5.2 Tolerance time to burn-injury levels
for various incident heat fluxes (Hymes)'(28)
- 82 -
JAERI-Research 97-022
100
100 1,000 10,000 100,000 1,000,000
Initial fuel mass (kg)
Fig. 5.3 Comparison of fireball duration among severalproposals
- 83 -
JAERI-Research 97-022
1000
>inc
co
•+J
to
3 burns, to bare skin (2mm)
50% lethality (average clothing)
1% lethality (average clothing)
start of 2 burns
range for blisteringof bare skin
t x E4/3=500
Fig. 5.4 Comparison of tolerance time to 1% lethality
between Eisenberg and Hymes(28X43)
- 84 -
JAERI-Research 97-022
1000
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100
10
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Fig. 5.5 TNT charge blast 11 (r : real distance from chargeWTNT : charge weight of TNT)
- 85 -
JAERI-Research 97-022
10
Q.
tn
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Scaled distance : R
100
Fig. 5.6 Over pressure of blast from vessel burst estimated by gasexpansion method (44)
- 86 -
JAERI-Research 97-022
1000
coCL
COCO
>o
100
10
\\
N \
^ \V
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s
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Comi i — (U - ;
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V.
methc
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as e nergy
s expansion methoccylindrical vessel
z_)d
> \
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j
i
10 100
Distance (m)
Fig. 5.7 Comparison of blast for vessel burstbetween TNT method and gas expansion method
- 87 -
JAERI-Research 97-022
Maximum bending stress a b
<Tb=0.5(a/hrPa = short span of wallh = thickness of wall
0 10 20 30 40
Applied pressure : P (kPa)
Fig. 5.8 Maximum bending stress crb on four edges fixed wall
- 88 -
00ID
CD
b
CO
CD
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c_Q
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40 -
30
20
10
00 10 20 30
Applied pressure : P (kPa)
40
16Pdh2
u b
7T{d 4 - (d -2 t ) 4 }
h = 80m
d=1 m>
i
^ ^ d = 1m,
d = 2m,
• —
t=O. 05m^/^
t=O. 1m
50
m
jo
Fig. 5.9 Maximum bending stress on single fixed bar
JAERI-Rcsearch 97-022
1.0E+4
1.0E+3
1 .OE+2
1.0E+1
1.0E+0
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AA
z/' //)
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A
A
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z / /A A
A A A/ /
/
/—//
A s 1^ • /
c / //D ' A/E /
F :::
0.1 1 10 100
Distance of downwind from the release point ( k m )
Fig. 5.10 Diffusion parameter a for equation of Pasquill(54)
- 90 -
JAERI-Research 97-022
1 .OE+3
1 .OE+2
1.0E+1
1.0E+0
V)/' /A/ /
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y
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y
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1 //
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Distance of downwind from the release point (km)
Fig. 5.11 Diffusion parameter cr2 for the equation of PasquillMI (54)
- 91 ~
1to
1
T
jnsity
(
MS
Q
0.04
0.035
0.03
0.025
0.02
0.015
0.01
0.005
0
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Sakagam/
i
•—i
Wind velocity : u=1m/sHeight of release point: h=0.5Atmospheric stability : FDistance of acrosswind : Y-0Height from release point: Z-Relea
—
se rate
i .
= 1 mVs
m
0
70
n
0 200 400 600 800 1000 1200 1400 1600 1800 2000
Distance of downwind from the release point (m)
Fig. 5.12 Comparison of estimation methods for ensity of combustible material in vapor cloud
0.3
0.25
0.2
.£ 0.15wcoQ
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ase poine+nkili+\/
t : h=O.5r
Distance of acrosswind : y=0Height from release point : z=0
n n
— '' •
— «, _ _
n
0 200 400 600 800 1000 1200 1400 1600 1800 2000
Distance of downwind from the release point (m)
m70
Fig. 5.13 Density of combustibe gas in vapor cloud released gas instantaneously
JAERI-Research 97-022
Q_
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Fig. 5.14 Over pressure of blast from a hemispherical fuel-air estimatedby Piston-Blast model(58)
- 94 -
JAERI-Research 97-022
100
0)(/)
o.(D
oww
0)Eb
10
§ 0.1
0.01
0.001
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lev
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100
Fig. 5.15 Over pressure of blast from a hemispherical fuel-air estimatedby Multi-Energy model<59>
- 95 -
I
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250
D_ 200
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— —,
Detonation blastMethane 100ton
• — — - — i
m
73
200 400 600 800 1000 1200 1400 1600 1800 2000
Distance from the center of vapor cloud (m)
Fig. 5.16 Comparison of several estimation methods for over pressure of blast of vapor cloud explosion
Geometry factorEmissive power
* (estimated by Eq. (5. 3))Rf (see Table 5. 1)
I
Operator2. 3kW/m2
Thermal radiationE = Rf <t>
( Tank )
V-—A
Hm70
S a f e d i s t a n c e : r
F i g . 5. 1 7 S c h e m a t i c i l l u s t r a t i o n o f e s t i m a t i o n m e t h o d o f s a f e d i s t a n c e a g a i n s t p o o l f i r e
Diameter : D (estimated by Eq.Duration : t (estimated by Eq.
(5. 5)-(5.7))(5. 8)or (5. 9))
Firebal
I00
Thermal radiationE = 375 (D/2r)2
Stack
ReactorbuiIding
OperatorK
S a f e d i s t a n c e : r
7*
©
F i g . 5. 1 8 S c h e m a t i c i l l u s t r a t i o n o f e s t i m a t i o n m e t h o d o f s a f e d i s t a n c e a g a i n s t f i r e b a l l
8i
Overpressure S(estimated by gas expansion method,see Fig. 5. 6)
Burst
Stack
ReactorbuiIdingIQkPa
Operator10kPa Blast
>mso73n
Safe d i s t a n c e : r
Fig. 5. 19 S c h e m a t i c iI lustration of e s t i m a t i o n method of safe d i s t a n c e a g a i n s t p r e s s u r e vessel burst
Explosion of vapor cloud Formation of vapor cloud
o©
Stack
Overpressure A?%(estimated by multi energy method,see Fig. 5. 15)
ReactorbuiIdingTOkPa
OperatorlOkPa
Equivalentexplosivevapor cloud
Di ffusion(estimated by Eq. (5. 17)or(5. 20))
Explosive vapor cloud
Blast i Wind
Distance against explosion Distance againstdi ffusion
Safe distance : r
Release ofexplosive gas
Undergroundnon pressurizedstorage tank
m73
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JAERI-Research 97-022
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JAERI-Research 97-022
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- 105 -
JAERI-Research 97-022
(1)
(2)
(3)
(4)
(5)
(6)
(7)
(8)
(9)
(10)
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19 (1983)
39 • 159 (1993)
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