Operational Reactor Safety
22.091 /22.903
Professor Andrew C. Kadak Professor of the Practice
Safety Analysis Report and LOCA Lecture 10
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 1
Topics to be Covered
• Safety Analysis Report – C ontents
• Chapter 15
– T ransients and Accidents Analyzed
• Loss of Coolant Accident Example
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 2
The Hazard (some fission-product isotopes)
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Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 3
Decay Heat
10 -1
10 -2
10 -3
10 1
-4
10 -1
10 10 2
10 3
10 4
10 5
10 6
10 7
10 8
T ime After Shutdown(s)
1- hour 1-day 1-week 1-month 1-year
seconds
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Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 4
Source: Todreas & Ka zimi, Vol. 1
.
CRITICAL SAFETY FUNCTIONS
KEEP FISSION PRODUCTS WITHIN THE FUEL
• Control Reactor Power Control reactivity additions Shutdown reliably
• Cool the Reactor and Spent Fuel Maintain coolant inventory Maintain coolant flow Maintain coolant heat sinks
KEEP RADIOACTIVE MATERIAL OUT OF THE BIOSPHERE
• M aintain Containment Integrity Prevent over-pressurization Prevent over-heating Prevent containment bypass
• Capture Material Within Contain ment Scrubbing
Deposition Chemical capture
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SH IEL D PERSONNE L FRO M RADIATIO N
Prof. Andrew C. Kadak, 2008
Department of Nuclea r S c ien ce & Engineering
Page 5
Emergency Safety Functions
Reactor Safety
Department of Nuclea r S c ien ce & Engineering Study, WASH-1400
Page 6
Prof. Andrew C. Kadak, 2008
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PWR SYSTEMS USED TO PERFORM EMERGENCY FUNCTIONS
Emergency Coolant Injection
Prof. Andrew C. Kadak, 2008 Page 7
React o D r e S p a f r e t t m y ent of Nuclea r S c ien ce & Engineering Study, WASH-1400
PWR SYSTEMS USED TO PERFORM EMERGENCY FUNCTIONS
Emergency Coolant Recirculation
Prof. Andrew C. Kadak, 2008
Department of Nuclea r S c ien ce & Engineering
Page 8
Reactor Safety Study, WASH-1400
PWR SYSTEMS USED TO PERFORM EMERGENCY FUNCTIONS
Post Accident Radioactivity Removal
Reactor Safety Study, WASH-1400
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 9
PWR SYSTEMS USED TO PERFORM EMERGENCY FUNCTIONS
Post Accident Heat Removal
Prof. Andrew C. Kada
ment of Nuclea r S c ien ce & Engineering Page 10
Reactor Safety Stud y D , W e p A a r S t H-1400
k, 2008
PWR Engineered Safety Systems
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Prof. Andrew C. Kadak, 2008 Page 11
BWR Early Engineered Safety Systems
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Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 12
Siting Criteria (10 CFR 100)
• Consideration of:
Characteristics of reactor design
Population characteristics, exclusion area, low population zone, population center distance
Assume a bounding fission product release based on a major accident
Define an exclusion area of such size that an individual located at any point on its boundary for two hours immediately following the accident would not receive a total radiation dose to the whole body in excess of 25 rem (250 mSv) or a total radiation dose in excess of 300 rem (3000 mSv) to the thyroid from iodine exposure.
Define a low popula tion zone of such size th at an individual located at any point on its outer boundary who is exposed to the radioactive cloud during the entire period of its passage would not receive a total radiation dose to the whol e body in excess of 25 rem (250 mS v) or a total radiation dose in excess of 300 rem (3000 mSv) to the thyroid from iodine exposure.
A population center distance of at least 1.33 times the distance from the reactor to the outer boundary of the population center distance
Seismology, meteorology, geology, hydrology.
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 13
General Design Criteria (10 CFR 50 Appendix A)
http://www.nrc.gov/reading-rm/doc- collections/cfr/part050/
• The principal design criteria establish the necessary design, fabrication, construction, testing, and performance requirements for structures, systems, and components importan t t o safety ; that is, structures, systems, and components that provide reasonable assurance that the facility can be operated withou t undu e ris k t o the healt h an d safet y o f th e public .
• Six major categories:
Overall requirements
Protection by multiple fission product barriers
Protection and reactivity control systems
Fluid systems
Reactor containment
Fue l an d reactivit y contro l
Prof. Andrew C. Kadak, 2008
Department of Nuclea r S c ien ce & Engineering
Page 14
The Single-Failure Criterion
• “Fluid and electric systems are considered to be designed against an assumed single failure if neither (1) a single failure of any active component (assuming passive components function properly) nor (2) a single failure of a passive component (assuming active components function properly), results in a loss of the capability of the system to perform its safety functions.”
• The intent is to achieve high reliability (probability of success) without quantifying it.
• Looking for the worst possible single failure leads to better syst e m understanding .
Prof. Andrew C. Kadak, 2008
Department of Nuclea r S c ien ce & Engineering
Page 15
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GDC 10 and 11
• Criterion 10--Reactor design . The reactor core and associated coolant, control, and protection systems shall be designed with appropriate margin to assure that specified acceptable fuel design limits are not exceeded during any condition of normal operation, including the effects of anticipated operational occurrences.
• Criterion 11--Reactor inherent protection . The reactor core and associated coolant systems shall be designed so that in the power operating range the net effect of the prompt inherent nuclear feedback characte ristics tends to compensate for a rapid increase in reactivity.
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Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 16
GDC 35
• An ECCS must be designed to withstand the following postulated LOCA: a double-ended break of the largest reactor coolant line, the concurrent loss of offsite power, and a single failure of an active ECCS component in the worst possible place.
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Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 17
Defense in Depth
“Defense-in-Depth is an element of the Nuclear Regulatory Commission’s safety philosophy that employs successive compensatory measures to prevent accidents or mitigate damage if a malfunction, accident, or naturally caused even t occurs at a nuclear facility.”
[Commission’s W h ite Paper, USNRC, 1999]
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 18
DEFENSE-IN-DEPTH MULTILAYER PROTECTION FROM FISSION PRODUCTS
NURE G D / e C p R a r - t 6 m 0 4 e 2 n , t 1 o 9 f 9 N 4 u . clea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 19
DEFENSE-IN-DEPTH, SAFETY STRATEGIES
Prof. Andrew C. Kadak, 2008
NURE G D / C e p R a - r 6 t 0 m 4 e 2 n , t 1 9 o 9 f 4 N . uclea r S c ien ce & Engineering
Page 20
Safety Analysis Report Contents
Chapter 1 I ntroduction and General Description of Plant Ch apt er 2 S ite Ch aract eristics
Chapter 3 D esign of Structures, Com ponents, Equipment, and System s Chapter 4 Reactor
Chapter 5 Reactor Coolant Systems and Connected Systems Ch apter 6 E ngineered Safety Features
Chapter 7 Instrum entation and Controls Ch apter 8 E lectric Power
Chapter 9 A uxiliary System s
Chapter 10 Steam and Power Conversion System Ch apter 11 Radio active Waste M a n a g e ment Chapter 12 Radiation Protection
Chapter 13 Conduct of Operations Ch apter 14 Initial Test Program
Ch apter 15 Accid ent An alysis Ch apter 16 Technical Specifications Ch apter 17 Qu ality Assurance
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. K N a d U a R k , E 2 G 0 0 / C 8 R-6042, 1994.
Page 21
Design Basis Accidents
• A DBA is a postulated accident that a facility is designed and built to withstand without exceeding the offsite exposure guidelines of the NRC’s siting regulation (10 CFR Part 100).
• Each DBA includes at least one signi ficant failure of a component. In general, failures beyond those consistent with the single-failure criterion are not required (unlike in PRAs).
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. K N a d U a R k E , G 2 / 0 C 0 R 8 -6042, USN RC, 1994.
Page 22
POSTULATED ACCIDENTS AND OCCURRENCES
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 23
U.S. Atomic Energ y Commission, 1973.
REPRESENTATIVE INITIATING EVENTS
TO BE ANALYZED IN SECTION 15.X.X OF THE SAR
1. I n c r e a s e i n H e a t R e mova l b y th e S e c o nd a r y System
1 . 1 F eed w a t e r s y s t e m m a l f u n c t io n s t h at r e s u lt s in a d e c r ea s e in f e e d w a te r te m p e r a t u r e .
1 . 2 F eed w a t e r s y s t e m m a l f unc t ion s t hat r e s u lt in an inc r e a s e i n f e e dw a te r f l o w .
1. 3 S t e a m pre s sure r e g u l a t o r m a lf u n c t i on or fa i l u re t h a t resu l t s i n i n c r ea s i ng st e a m fl o w .
1 . 4 I nadv e r ten t open i n g o f a s t e a m gene r a to r r e li e f o r sa f e ty valv e .
1 . 5 S pec t r um o f s t e a m s y s t e m p i ping f a ilu r e s in s i de and out s ide o f c onta i nmen t in a P W R .
2 . D e c r ea s e i n He a t R e m ova l b y t h e S e c o n d a r y S y s t e m
2. 1 S t e a m pre s sure s r e g u l a t o r m a lfunc t i o n o r fai l u re t h a t re s u l t s i n d e cr e a s i n g s t e a m fl o w.
2 . 2 L o s s o f ext e r nal el e c t r i c l oad.
2. 3 T u r bi n e tr i p ( s t op v a l v e c l o s ure).
2 . 4 I nadv e r ten t c l osu r e o f ma i n s t e a m i s olat i o n v a lve s .
2 . 5 L o s s o f conden s e r vacuu m .
2. 6 C o i n c i d e n t l o ss o f o n s i t e a n d e x t er n a l ( o ffs i t e ) a . c . p o w e r t o t h e st a t i o n .
2 . 7 L os s of n o r m al f e ed wat er fl ow.
2 . 8 F eed w a t e r p i ping b r eak .
3. De cr e a s e i n Re a c t o r Co o l a n t Sy st e m Fl o w Rat e
3 . 1 S ingl e and mu l tip l e r e ac t o r coo l ant pump t r ip s .
3. 2 B W R r e cir c u l a t i o n l o o p c o n t rol l er m a lf u n c t i o n s t h a t re s u l t i n de cre asi n g f l o w ra t e .
3 . 3 Re a cto r coo l ant pump sh a f t s e i z u r e .
3 . 4 Re a cto r cool a n t p u m p s h a f t b r e a k .
Prof. Andrew C. Kadak, 2008
Department of Nuclea r S c ien ce & Engineering
Page 24
NUREG/CR-6042, USN RC, 1994.
REPRESENTATIVE INITIATING EVENTS
TO BE ANALYZED IN SECTION 15.X.X OF THE SAR (cont.)
4 . Re a c ti v i t y a n d P o we r Di str i b uti o n A n oma li e s
4.1 U ncont r o l l ed cont r o l r o d a s se m bly w i thd r a w s f r o m a s ubc r i t i c a l o r lo w po w e r st a r tup cond i tion ( a s s u m ing the m o s t u n f avo r abl e r e act i v ity cond i t ion s o f th e co r e and r e a c to r cool a n t s ys t em ) , i nclud i n g c on t r ol r od o r te m po r a r y c o nt r ol devi c e r e m o va l e r r o r d u r i ng r e f u e l ing.
4.2 U n cont r o l l ed cont r o l r o d a s se m b ly w i thd r a w s a t t h e pa r t i c ula r p o w e r l e ve l ( a s s um ing th e m o s t u n f a vo r a ble r e a c tiv i t y c ondit i o ns o f t he c o r e and r e ac t o r coo l ant sy s t e m ) tha t yi e l d s t he m os t se v e re re su l t s (l ow p o wer t o f u l l p o w er) .
4.3 Cont r o l r o d m a lope r a tion ( sy s t e m m a l f u n c tion o r op e r ato r e r r o r ) , in c l uding m a lope r a tion o f pa r t l e ngth cont r o l r o d s .
4.4 A m a l f unc t ion o r f a i l u r e o f t h e f l ow cont r o l le r in BWR loop tha t r e s u l t s in an inco r r e c t te m p e r a t u r e.
4.5 A m a l f unc t ion o r f a i l u r e o f t he f l ow cont r o l le r in BWR loop tha t r e s ul t s in an inc r e a se d rea c t o r c o o l a n t fl o w rat e .
4.6 C h e m i c a l a n d vol u m e c o n t rol sy ste m m a l f u n c t i o n t h a t re su l t s i n a de cre ase i n t h e boron con c ent r a t ion in the r eac t o r c oolan t o f a P WR .
4 . 7 I nadv e r ten t lo a d ing a n d o p e r a t i o n o f a f u e l a s s e m b ly in a n im p r ope r pos i tion .
4 . 8 S pe c t r u m o f r od e j e c tion ac c i den t s in a P W R .
4 . 9 S pe c t r u m o f r od d r o p ac c i den t s in a BWR .
5. In c r e a s e i n Re a c t o r Co o l a n t I nv e nto r y
5 . 1 I nadv e r ten t ope r a tion o f ECC S d u r i ng po w e r ope r a t i on s .
5.2 C h e m i c a l a nd vol u m e c o n t rol s y s t e m m a l f u n c t i o n (or o p e rat or e r ror) t h a t i n c r ea s e s re a c t o r coo l ant inven t o r y
5.3 A n u m b e r o f B W R tra n s ie n t s , i n c l u d i n g i t e m s 2. 1 t h rough 2 . 6 a n d i te m 1. 2 .
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 25
NUREG/CR-6042, USN RC, 1994.
REPRESENTATIVE INITIATING EVENTS
TO BE ANALYZED IN SECTION 15.X.X OF THE SAR (cont.)
6. De cr e a s e i n Re a c to r C o o l a n t In ve n t or y
6. 1 I n a d v er t e n t o p e n i ng of a pre ss uri zer safet y or r e li ef v a l v e i n a PW R or a s af e t y or re l i ef v a lv e in a B W R .
6 . 2 B r e a k in in s t r u m ent lin e o r othe r lin e s f r om r ea c to r c oolan t p r e s s u r e bounda r y t h at pen e t r a t e c onta i nmen t .
6 . 3 S te a m g e ne r a t o r tub e f a ilu r e .
6 . 4 S pec t r um o f BWR st eam s y s t em piping f a i lu r e s ou t s i d e of con t ain m ent .
6 . 5 L o s s - o f - cool a n t a c c i dent s r e su l t ing f r om the sp e c t r u m o f pos t u la t e d p i ping b r eak s w i t h in th e r e a cto r cool a n t p r e s su r e bounda r y , i n clud i n g s t e a m line b r e a ks in s i de o f c o nta i nmen t in a B W R .
6 . 6 A nu m b e r o f BWR t r an s i e n t s , inc l uding it e m s 2 . 7, 2.8 , and 1.3 .
7. Ra di o a c ti v e Re le a s e fr o m a Sub s y ste m o r Compon e n t
7.1 R a d i o a c t i v e g a s wa st e s y ste m l e ak or fa ilure .
7 . 2 R a d io a c ti v e l i q u id wa st e sy ste m l e ak o r fa ilu r e .
7 . 3 P os t u la t ed r a dioa c tiv e r e l ea s e s due t o l i quid tank f ai l u r e s .
7 . 4 D e s ign b a si s f u e l hand l i ng acc i d ent s in t h e conta i nmen t a n d s p ent f u e l s t o r ag e bui l d ing s .
7 . 5 S pent f u el c a sk d r op a c cid e nt s .
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 26
NUREG/CR-6042, USN RC, 1994.
Emergency Core Cooling System (ECCS) (January 1974, 10 CFR 50.46)
• Postulate several LOCAs of different sizes and locations to provide assurance that the most severe LOCAs are considered.
• Postulate concurrent loss of offsite or onsite power and the most damaging single failure of ECCS equipment (GDC 35).
• Acceptance Criteria
Peak cladding temperature cannot exceed 2200 ºF (1204 ºC)
Oxidation cannot exceed 17% of cladding thickness
Hydrogen generation from hot cladding-steam interaction cannot exceed 1% of its potential
Core geometry must be coolable
Long-term cooling must be provided
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Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 27
Double Ended Guillotine Break
Department of Nuclea r S c ien ce & Engineering
Page 28
Prof. Andrew C. Kadak, 2008
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Figures © Hemisphere. All rights reserved.
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Prof. Andrew C. Kadak, 2008
S c ien ce & Engineering Page 30
Department of Nuclea r
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2500
2400 "
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Safety Valv e s Open
High Pressure Trip - Both Poxer
Operded Relief Vatves Open
2350
Both
Spr a g y r i V g alVe S Full Open
Above
2350 psia
High
Pres sure
Both SpraY Valves Full
Closed
2300 ,
2275 ;'
Belo \ ’/ 2300 psia
Proportional Hea \ er Grou p " 0Fr
2250 ”
2225
22@ -”
tontrnl Set P0lflf
All Batkug Heaters ” 0fF" ét<ve 2223
Proportional
y l l Backup Heaters "Ok’" 8elow 22@
Low Pressure Alarn
psia
Thermal Marain/Loa Pressure Trip
fi-°! .^1int \ Y'• h Varv BP‹hveen
1730 and ZSOS psia’
1750
Thermal h \ arain/Low MininuwV»fue
P ress u T r r e ip
LP.':-LR Pressure Alarm and Satet
Injection Actuation Si¿nal
Pressure Control PrO§fan
7- 13
NEP 1 & 2
TABI• E 15 . 4- 1 c
LAR GE BREAK
TIM E SEQUENC E O G EVENTS
Amendment Nl0 March 1978
DECL |
0.6 DELL |
0. 4 DECL |
0.8 DECL |
|
START |
( Sec ) 0. |
( Sec ) 0. |
( Sec ) 0. |
( Sec} o. |
Rx Trip Signal |
1.04 |
1.10 |
1, 16 |
1.06 |
0.94 * |
1. 10 |
1. 16 |
1.02 * |
|
Acc. IAjectioA |
12.5 |
14.6 |
T9 › 4 |
13.0 |
End of BlowdOWD |
26.5 |
23. 3 |
36.9 |
20.7 |
Bottom of Core Recovery |
38 8 |
37.6 |
48.8 |
34.4 |
Acc. Eapcy |
53.0 |
57. 4 |
63. 9 |
55.4 |
Pump Injection |
25.94 |
26. EO |
26› 16 |
26.02 |
23. 4 |
23.2 |
32.9 |
20.5 |
* From Containment Pressure Signal.
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NEP 1 & 2
TABL E l5.4-1d
Amendment N10
March 1978
Net Free Volume
Initial Conditions Pressure Temperature RWST temperature
CONTAINNEN Z DAT A — hE P CONTAINMEN T
2.987 x 10’ f 3
14. 7 psla 90°F
4O°F
Raw water temperature Outside temperature Relative humidity
Spray System
Number of pumps operating Runout flow rate ( totaL ) Actuation time
NA
0°F
99$
2
6600 u
35 sec
Structural Eeat Sinks
Item
Thicknes s ( ft )
Area ft 2
Containment Cylinder Containment Dome Containment Floor Containment Sump Miscellaneous Concrete Hiscellaneous Steel
.0313 steel, 4.5 concrete 70151
.0417 steel, 3 5 concrete 33867
4.0 concrete, .0208 steel, 9.0 concrete 13820
9.0 coocrete 972
1.0 concrete 160,000
0.2 steel 5,000
0.05 steel 65,000
0.03125 steel 90,000
0.030 steel 100,000
0.020 steel 70,000
0.0057 steel 45,000
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NEP 1 6 2
TABL E 1 3 . 4— 1 a
LARG E BREAK
Amendment N10 March 1978
DECL
0. 6 DCCL
0. 4 DECL
0.8 DECI.
Peak Clad Temp. °F Peak Clad Locaclon Ft- .
Local Z • ' 2 0 Rxn ( »a= ) z
Local Z •° 2° Location Ft.
2148
7.5
6.7
7.5
2137
7.5
6. 7
7.5
1790
9.0
2. 1
8.0
2144
7.3
6.8
6.0
Total Z 2 0 Rxn Z
*0.3 *0.3
<O.3
<0.3
Hot Rod Burst Time sec
21.0
23.2
84.8
20.2
Hot Rod Burst Location Ft. 5.75
NSSS Pou’e:c J ct 102Z oC
Peak I.1neac Power kw/it 102Z o€
Peaking Factor ( At License Rating )
3. 75
3425
12.6
2.32
7.O
Accuaulatoz Vatez Vo1uzae ( Cub1c J eeL ) 950
Puel region t cycle soslysed
WIT 1
Cycle
1
Rnglon
All
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3Nl1
.O
0
0
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( 0d/d ) ¥3k0d
AMENDMENT NIJ MARCH 197i
( s
ox
033S )
50
20
30
lO
N EW ENGLAND POWEft COMPANY N E P & 2
Preliminary Safety Analysis Fleport
CORE POWER TRANSIENT - DECLG ( C - 1.0 )
A
FIG. 15.4.1-14A •• = = ° ^
( 0’l ’O 59O3O - 3lVb AO98 >V@b8
Z 6 \ d 3 N
AN'o’dNOO tJ3/ \ / \ Od ON \ r1ON3 M3N
8Z6£ HOtJYN
0tN 1N1WONZWV
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BREAK FLOW ( LB/SEC )
01
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( ‹ I Sd ) 3¥flSS3 \ Id
AMENDMENT N1o MAICH 1978
OOO Z
50
20
NEW ENGLAND POWER COMPANY N E P & 2
PreliIT \ inSry Safety Analysis Report
CORE PRESSURE — DECLG ( C D 1.0 )
( sa
x
FIG. 15.4.1-4A
1 1 1 1 1 l I
20.0
I2 . 5
l O . O
5 . O
2.5
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( 1‹ ) 1353i k31Y/4
AMENDMENT N1f
MARCH 197t
0 0 \ f 8 C 0 4 t £ R
300
200
I00
T | ME ( SECONDS )
NEW ENGLAND POWER COMPANY
N E P 1 & 2
Prel imii›ary Sule‹y An a vi is Fleport
REFLOOD TRANSIENT - DECLG ( C D - 1.0} DOWNCOMER AND CORE WATER LEVELS
n
FIG. 15.4.1-UA • • •
( 0"t ’3 ) DOOZO — 3dFlJ-Yu3dN3A O'b’13 1YZd
taodag stsAjeug Atajeg ‹ •^ u ! ^ !I ^* d
g 9 I d 3 N
ANVdINO3 UZMOd ON'V’0DN1 MZN
500
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CLAD A VERA G T E EMPERATURE HOT g0O ( “F )
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›
2500
2000
@l500
TY/0 PHASE VOLUME
42 in. DOUBLE-ENDED HOT LEG BREAK ¥/ITH
MINIMUM SAFETY INJECTION
4000
3000
<<* I000
PRESSURE
Ll§UlD-
VOLUME
TIME, SECONBS
T0P0FC0R2 2000
BOHOM OF CORE
30
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TEMPERATURES -
°F
2500
TEMPERATURE TRANSIENT MATCHES FLOW TRANSIENT
2000
1500
AT CONTAINMENT PRESSURE
HOT SPOT FLU 10
0 20 40 60 80 100 120 140 160 180 2oo TlHE AFTER BREAS - SEC08DS
Figure 15. 4- 6, Double Snded Cold Leg Break ( Guillotine )
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15 . 4
NEP 1 6 2
CONDITIO N t Y - LIMITIN G FAULTS
Amendment NlO
Harch 1978
Refer to RESAR-3 ( 4-loop, without loop stop valves ) Section 15.4, with
the following modifications:
15 . k • 1 Ha jor Reac tor Coo l ane S s tern PI e Ru tures
Los s o I Co o lan d Acc ident )
The analysis specified by 10 CIR Part 50.46 ( 1 ) Acceptance Criteria for Emergency Core Cooling Systems for Light Water Cooled Nuclear Power Reactors is presented in this section. The results of the LOPA analyses
are shown in Table 15.4-1a and show compliance with the Acceptance Criteria.
The analytical techniques used are in compliance with Appendix K of 10 CFR Part 50, and are described in Reference ( 2 ) The results for the small break LOCA are presented in subsection 15.3.1 of the PSAR and are in conformance with 10 CFR Part 50.46 and Appendix K of 10 CFR Part 50.
The boundary considered for the IDCA as related to connecting piping is
defined in RESAR-3, Section 3.6.
Should a major break occur, depressurization of the reactor coolant system results in a pressure decrease in the pressurizer. Reactor trip signal occurs when the pressurizer low-pressure trip set point is reached. A safety injection system signal is actuated wLen the appropriate set point is reached. These countermeasures will limit the consequences of the accident in two ways:
a. Reactor trip and borated water injection complement void formation in causing rapid reduction of power to a residual level corresponding to fission product decay heat.
b. Injection of borated water provides heat transfer from the core
and prevents excessive clad temperatures.
At the beginning of the blowdown phase, the entire reactor coolant system contains subcooled liquid which transfers heat from the core by forced convection with some fully developed nucleate boiling. After the break develops, the time to departure from nucleate boilin g is calculated, consistent with Appendix K of 10 CFR Part 50. Thereafter, the core heat transfer is based on local conditions with transition boiling and forced convection to steam as the major heat transfer mechanisms. During the refill period rod-to-rod radiation is the only heat transfer mechanism.
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13.4-1
NEP 1 & 2 Amendment N10
March 1978
When the reactor coolant System pressure falls below 600 psia, the accumulators begin to inject borated water. The conservative assumption is made that atcumulatoz water injected bypasses the.core and goes out through'the break until the termination of bypass. The conservatism is again consistent with Appendix K of 10 CFR Part 50.
15. 4. 1 . 1 Therma l An a ly s i s
a. Westinghouse Performance Criteria for Emergency Core Cooling
Sys eem
The reactor is designed to withstand thermal effects oaused by a LOCA, including the double-ended severance of the largest reactor coolant system pipe. The reactor core and internals, together with the emergency core cooling system, âre desigoed so that the reactor can be safely shut down and the essential heat transfer geometry of the core preserved following the accident.
The emergency core cooling system, even wheo operating during the injection mode with the most severe single active failure, is designed to meet the Acceptance Criteria.
b. Hethod of Thermal Analysis
The description of the various aspects of the LO€A analysis is given in Reference ( 2 ) . This document describes the major phenomena modeled, the interfaces among the computer codes, and features of the codes which maintain compliance with the Acceptance Criteria. The individual todes are described in detail in References ( 3 ) through ( 6 ) . The containment parameters used in the containment analysis code, Reference ( 6 ) , to determine the emergency core cooling system backpressure are presented in Table l5. $-1b .
The analysis presented here was performed using tLe October, 1975 version of the Westinghouse Evaluation Model. This version includes the modifications to the models, referenced above, as specified by the NRC in Reference ( 7 ) and complies with Appendix K of 10 CIR Part 50. The October, 1975 Westinghouse Evaluation M0del is documented in References
( 8 ) through ( 10 ) .
The analysis was performed using the conservative assumption that the fluid temperature in the upper head of the reactor vessel is equal to the reactor vessel outlet temperature. The effect of upper head temperature on ECOS perfomance is discussed iz References ( 13 ) anB ( 14 ) .
The time sequence of events for all breaks analyzed is shown in Table
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13. 4-1a
NEP 1 & 2 Amendment. N10
March 1978
The analysis was performed using a reference containment which has internal steel and concrete structural heat sinks which conform to the guidelines
of Branch Technica1 Position USB 6-1.
The containment initial conditions of 90 F and 14.7 psia are representatively low values anticipated during normal full-power operation. The initial relative humidity was conservatively assumed to be 98.8 percent.
The condensing heat transfer coefficient used for heat transfer to the steel contaioment structures for tbe limiting break is giVen in Figure 15.4.1-16.
The containment temperature respoose is presented in Figure 15.4.1-17 for
t:he l Smt ting break .
The containment sump temperatGre does not affect the analysis because the maximum peak cladding temperature occurs prior to initiation of the recirculation mode for containment spray system.
The mass and energy releases used iu the containment backpressure calculation for the limiting break are presented in Table 15.4-ie.
These results can be demonstrated to be conservative for NKP as follows:
Table 15.4-1b lists the reference containment parameters used in the calculation that yielded a peak clad temperature of 2148 P. Table 15 . 4—Id lists the NEP containment parameters. Pigure 15.4.1-18 shows containment pressure versus time for the limiting break for each set of containment
parameters. The figure demonstrates that the NEP back pressure is at all times higher than that of the contaioment used in the ECCS performance calculation. As a result, the core flooding rates for NEP l & 2 exceed the calculated flooding rates; the higher flooding rates will yield a peak clad temperature lower than 2148’S.
c. Results
Table 15.4-1a presents the peak clad temperatures, hot spot metal reaction, and other key results for a range of break sizes. The range of break sizes was determined to include the limiting case for peak clad temperature from sensitivity studies reported in References ( II ) and ( 12 ) .
The SATAN YI analysis of the LOCA is performed at 102 percent of Engineered Safeguards Design Rating. The peak linear power and core power used in the analyses are given in table 15.4-1a. The equivalent core parameter
at the license application power level are also shown in Table 15.4-1a. Since there is margin between the value of the peak linear power density used in this analysis and the value expected in operation, a lower peak clad temperature would be obtained by using the peak linear power density expec ted during op e rat 1 on .
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IS . 4-1 b
NEP 1 & 2 Amendment N10
Narch 1978
For the results discussed below, the hot spot is defined to be the location of maximum peak clad temperature. This location is given in Table 15.4-1a for each break size analyzed.
Figures 15.4.l-lA through 15.4.1-16 present the transients for the principal parameters for the break sizes analyzed. The following items are noted:
Figures 15 . 4 1-lA through 15. S. 1-3D
Figures lâ.4.l-4A
through 15.4.1-6D
figures 15.4.l-7A through 15.4.1-9D
Figures 15. 4. I -l0A
through 15 . k. I -10H
Figures 15.4.1-UA
through l5.4.l-I2D
Figures 15. 4 . 1 -l3A through l5 . 4 . l-13D
The following quantities are presented at the clad burst location and at the hot spot ( location of maximum clad temperature ) , both on the hottest fuel rod ( hot rod ) :
a. Fluid quality
b. Mass ve1ocity
c. Heat transfer coefficient
The heat transfer coefficient shown is calculated
by the LOGTA IV Code.
The system pressure shown is the calculated pressure in the core. The flow tate out the break is plotted as the sum of both ends for the guillotine break cases. The core pressure drop shown is from the lower plenum, near the core, to the upper plenum
at the core outlet.
These figures show the hot spot clad temperature transient and the clad temperature transient at the burst location. The fluid temperature shown is also for the hot spot and burst location, The core flow ( top and bottom ) is also shown.
These figures present the core reflood transient.
These figures show the emergency core cooling system flow for all cases analyzed. As described earlier, the accumulator delivery during blowdowo is discarded until the end of bypass is calculated. Accumulator flow, however, is established in refill-reflood cal- culations. The accumulator flow assumed is the sum of that injected in the intact cold legs.
These figures show the containment pressure transient.
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15.4- 1c
AP 1 G 2
Amendment Nl0
March 1978
Figures l5 .4. 1-UA These figures show the core power Irans ient. through 15.4. 1 -UD
Figure 15.4.1-15 This figure shows the break energy released to the
containment during blowdown.
Figure 15.4.1-16 This figure provides the containment wall condensing heat transfer coefficient.
In addition to the above, Tables 15.4-ie and l5.4-lf present the reflood mass and energy releases to the containment and the broken loop accumulator mass and energy flowrate to the containment, respectively.
The clad temperature analysis is based on a tota1 peaking factor of 2.32. The hot spot metal water reaction reached is 6.7 percent, which is well Lelow the embrittlement limit of 17 percent, as required by 10 CFR Part
50.46. In addition, the total core metal water reaction is less than 0.3 percent for all breaks as compared with the 1 percent criterion of 10 CFR Part 50.46.
The results of several sensitivity studies are reported in Reference ( 12 ) . These results are for conditions which are not limiting in nature and hence are reported on a generic basis.
Conclusion s - Therma l Analysis
Eor bzeatus up to and including the double-ended severance of a reactor coolant pipe, the emergency core cooling system will meet the Acceptance Criteria as presented in 10 CFR PART 50.46. That is:
a. The calculated peak €uel element clad temperature provides margin to the requirement of 2200 F even with containment parameters as conservative as those presented in Table l5.5-1b.
b. The amount of fuel element cladding tbat reacts chemically with water or steam does not exceed 1 perceât of the total amount
of Zircaloy iu the reactor.
The clad temperature transient is teminated at a time when the core geometry is still amenable to cooling. The cladding oxidation limits of 17 percent are not exceeded during oz after quenching.
d. The core temperature is reduced and decay heat is removed for an extended period of time, as required by the long-lived radioactivity remaining in the core.
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1 5 . A -1 ri
Reading and Homework Assignment
1. Read Knief Chapter 14
2. Problems: 14.9, 11, 12, 21, 23
Department of Nuclea r S c ien ce & Engineering
Prof. Andrew C. Kadak, 2008 Page 29
MIT OpenCourseWare http://ocw.mit.edu
22.091 Nuclear Reactor Safety
Spring 200 8
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