A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

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IAEA Meeting on INPRO Collaborative Project “Performance Assessment of Passive Gaseous Provisions (PGAP)” 13-15 December, 2011, Vienna A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

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IAEA Meeting on INPRO Collaborative Project “Performance Assessment of Passive Gaseous Provisions (PGAP)” 13-15 December, 2011, Vienna. A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085. GFR DHR Analysis for Transient 1. - PowerPoint PPT Presentation

Transcript of A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Page 1: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

IAEA Meeting on INPRO Collaborative Project “Performance Assessment of Passive Gaseous Provisions (PGAP)”13-15 December, 2011, Vienna

A.K. Nayak, PhDReactor Engineering DivisionBhabha Atomic Research CentreTrombay, Mumbai 400085

Page 2: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

GFR DHR Analysis for Transient 1

Computer code used : RELAP5/MOD3.2

Power = 2400 MWth No. of DHR Loops = 1 Full reactor is simulated in the RELAP5/MOD3.2

to study the passive decay heat removal behaviour of the reactor.

Thermal inertia of all the components in the main circuit have been considered.

Heat exchange between DHR hot and cold ducts through the insulation has been considered.

Steady state calculations are continued until 500 sec.

Page 3: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Inputs for Analysis of Main LoopPhysical parameters

Main CKT:

Power = 0- 2400 MW increased linearly in 100 secondsPressure = 6.98 MPa at t=0 secMass Flow Rate = 0 kg/s at t=0 secTemperature = 673K at t=0 sec

Main Secondary CKT:

Mass flow Rate = 2685 kg/s at t = 0 to t = 500 secInlet Temperature = 839 K at t = 0 to t = 500 secInlet Pressure = 6.5 MPa at t = 0 to t = 500 sec

Page 4: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Steady State Analysis

Transient Calculations continued for 500 sec to achieve the steady state

CODE achieved Steady state after 125 sec

Page 5: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Inputs for Analysis of DHR Loop – Initial ConditionsDHR secondary mass flow rate = 0 DHR secondary pressure = 1.0 MPa DHR secondary Temperature = 323 K

POOL INITIAL CONDITIONS:Pool pressure= 0.1 MPaPool Temperature= 323 K

Page 6: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Assumptions Local resistances in the fuel element is considered such

that the pressure difference in the core part is matched with the steady state conditions given.

Since the geometry of the core is complex, the lumped model is used for the simulation of the core.

The core is divided into 7 channels (6 heat generating and one bypass). Each channel is divided into 25 volumes.

The flow area and the heat transfer area are same as in the actual reactor core.

Heat transfer coefficient in the heat structure parts viz: in the core, in main IHX, in DHR IHX and in the pool IHX, is decided by the RELAP5 inbuilt models.

Page 7: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Dimensions Considered

BLOWERMain features are:

– Flow Area= 3.14m2– Length =3.0m– Rated velocity= 470.24 rad/s– Initial blower velocity/rated velocity=1– Rated flow =340.0m3/s – Rated head= 30000m– Rated torque= 15019N.m– Moment of inertia=0.0676 Kg/m2– Rated density of fluid= 5.58 Kg/m3– Pump closing takes place in 50seconds as per the velocity given.

Page 8: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Important dimensionsComponents Area(m2) Length (m) Volume (m3)

MainHeat

TransportSystem

Reactor Pressure vessel

Lower plenum 3.2 68.63Core0 0.27

0.25058160.27

5.8

Core1 0.540.50116320.54

5.8

Core2 0.810.75174480.81

5.8

Core3 0.540.50116320.54

5.8

Core4 0.630.58469040.63

5.8

Core5 0.90.8352720.9

5.8

Bypass 1.9068 5.8Upper plenum1 32.3713 3.3Upper plenum2 3.2 68.63Downcomer 5.5 7.0

Primary Circuit

Primary hot leg 1.89 2.0Inlet main IHX 2.0126 7.95IHX primary side 10.73 0.821Outlet main IHX 2.0126 7.95Buffer volume 6.0 100.0Blower 3.0 9.42V Circol 20.0 2.5Primary cold leg 1.53 2.0

Page 9: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Important dimensionsComponents Area(m2) Length (m) Volume (m3)

DHRSystem

Primary Circuit

Lower plenum 3.2 68.63Core0 0.27

0.25058160.27

5.8

Core1 0.540.50116320.54

5.8

Core2 0.810.75174480.81

5.8

Core3 0.540.50116320.54

5.8

Core4 0.630.58469040.63

5.8

Core5 0.90.8352720.9

5.8

Bypass 1.9068 5.8Upper plenum1 32.3713 3.3Upper plenum2 3.2 68.63Downcomer 5.5 7.0

Secondary Circuit

Primary hot leg 1.89 2.0Inlet main IHX 2.0126 7.95IHX primary side 10.73 0.821Outlet main IHX 2.0126 7.95Buffer volume 6.0 100.0Blower 3.0 9.42V Circol 20.0 2.5Primary cold leg 1.53 2.0

Page 10: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

RELAP 5 Nodalization of Main circuit of GFR

Page 11: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

GFR Nodalization

Page 12: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Mass Flow rate (Various Channels)

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Mass Flow rate (total core)

Page 14: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Pressure in the lower and upper plenum

Page 15: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Helium temperature in lower and upper plenum

Page 16: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Variation of clad surface temperature along the height

Page 17: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Fuel Centre line Temperature (Steady State)

Page 18: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Individual Channel power at Steady State

-500 -400 -300 -200 -100 0-5.00E+007

0.00E+000

5.00E+007

1.00E+008

1.50E+008

2.00E+008

2.50E+008

3.00E+008

3.50E+008

4.00E+008

4.50E+008

5.00E+008

5.50E+008

6.00E+008

P

ow

er

(W)

Time(S)

Power Core0 Power Core1 Power Core2 Power Core3 Power Core4 Power Core5

Page 19: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Total Core Power at Steady State

-500 -400 -300 -200 -100 0

-2.00E+008

0.00E+000

2.00E+008

4.00E+008

6.00E+008

8.00E+008

1.00E+009

1.20E+009

1.40E+009

1.60E+009

1.80E+009

2.00E+009

2.20E+009

2.40E+009

2.60E+009

T

ota

l Po

we

r (W

)

Time(S)

Total Power To Core

Page 20: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

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Model Qualification – summary of Steady-state results

3. Error defined as:(Design value)-(RELAP5 value)

*100Design value

Reference RELAP5 Error(%)

Main Vessel Inlet/Outlet Gas Tempreratures (°C) 400/850 400/851

Core Outlet Gas Temperature (°C) 900 902 0.22

Main Vessel Inlet/Outlet Gas Pressure (MPa) 7.12/6.98 7.13/6.98

∆P Vessel (Uppper Plenum/Lower Plenum) (MPa) 0.14 0.12 14.28

Main Loop Mass Flow Rate (kg/s) 340.8x3 1019 0.09

Core Inlet Mass Flow 1020 1019 0.09

Main Loop IHX Exchanged Power (Mw) 803.3x3 2400

Page 21: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Model Qualification – summary of Steady-state results

Qchannel (kg/s) (reference) RELAP5 Error (%)

Downcomer 1020.2 1019 0.09

Core0 74.5 76.0 -2.01342

Core1 145.7 144.0 1.166781

Core2 208.4 206.0 1.151631

Core3 130.1 132.0 -1.46042

Core4 166.8 165.0 1.079137

Core5 193.3 194.0 -0.36213

Bypass 101.4 102.0 -0.5917

Page 22: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

SBO Transient

Page 23: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

DHR Analysis for SBO

100%

0 t_Q3% t_Q3%+ 3 s

t_Q3%+ 5 s

3%

t_Q3%+ 11 s

time

Core inletmass flow

SCRAM

Main loops isolating valves opening fraction

DHR loops isolating valves opening fraction

2 s 6 s

NCDHR phase

“DHR sequence”5 s

t_Q3%+ 16 s

Time lag for DHR blowersstart-up

100%

0 t_Q3% t_Q3%+ 3 s

t_Q3%+ 5 s

3%

t_Q3%+ 11 s

time

Core inletmass flow

SCRAM

Main loops isolating valves opening fraction

DHR loops isolating valves opening fraction

2 s 6 s

NCDHR phase

“DHR sequence”5 s

t_Q3%+ 16 s

Time lag for DHR blowersstart-up

After 500 sec transient calculation were continued for the DHR

Reactor Was Tripped at 500 sec

Blower Stops in 50 sec after 500 sec– valves in main

loops start closing at 47 sec and gets completely closed at 49 sec after 500 sec.

DHR Circuit Was Valved In After 55 sec Seconds And Valve Fully Opened In 60 Sec after 500 sec.

Page 24: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Main vessel pressure

Page 25: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

DHR secondary side pressure

Page 26: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

DHR secondary side Temperature

Page 27: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

DHR water side flow rate

Page 28: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Gas Temperature at Main Vessel Inlet/ Outlet

Page 29: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Channel Flow rate

Page 30: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Total core flow rate

Page 31: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Power to the various channels

Page 32: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Power to the Core

Page 33: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Power to and from DHR secondary loop

Page 34: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Sensitivity analysis – Parameters considered and their variations

• Core ∆P variation ±15%• Core Power variation ±2%• Residual Power variation ±10%• Heat Transfer area variation ±25%• DHR Heat Transfer area variation ±25%• DHR inlet Loss coefficient variation ±200%• DHR outlet Loss coefficient variation ±200%• Thermal Inertia variation ±15%• Main Circuit Pressure variation ±2bar• Primary Blower Inertia ±25%

Page 35: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Failure Criteria

Criterion

SBO Transient

(DHR loop structural integrity)Maximum temperature of DHR structural material

850 °C

Maximum clad temperature

1600 °C

(Core upper structures integrity)Maximum temperature of gas at hot channel outlet

1050 °C

Page 36: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Blower Inertia ±25%

Page 37: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Blower Inertia ±25%

Page 38: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Blower Inertia ±25%

Page 39: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Core Power ±2%

Page 40: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Core Power ±2%

Page 41: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Core Power ±2%

Page 42: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Residual Power variation ±10%

Page 43: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Residual Power variation ±10%

Page 44: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Residual Power variation ±10%

Page 45: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Core ∆P variation ±15%

Page 46: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Core ∆P variation ±15%

Page 47: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Core ∆P variation ±15%

Page 48: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Heat Transfer area variation ±25%

Page 49: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Heat Transfer area variation ±25%

Page 50: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Heat Transfer area variation ±25%

Page 51: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of DHR Heat Transfer area variation ±25%

Page 52: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of DHR Heat Transfer area variation ±25%

Page 53: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of DHR Heat Transfer area variation ±25%

Page 54: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Thermal Inertia variation ±15%

Page 55: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Thermal Inertia variation ±15%

Page 56: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Thermal Inertia variation ±15%

Page 57: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Main Circuit Pressure variation ±2bar

Page 58: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Main Circuit Pressure variation ±2bar

Page 59: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of Main Circuit Pressure variation ±2bar

Page 60: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of DHR inlet/outlet Loss coefficient variation ±200%

Page 61: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of DHR inlet/outlet Loss coefficient variation ±200%

Page 62: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of DHR inlet/outlet Loss coefficient variation ±200%

Page 63: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of variation of all parameters (conservatively)

Page 64: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of variation of all parameters (conservatively)The maximum clad surface

temperature is 1190 deg CThe maximum temperature of the

gas at channel outlet is 1167 deg C DHR structural temperature is 425

deg C.

Page 65: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Summary of results of sensitivity analysis Parameters Clad Surface

Temperature (0C)Nominal (1013 0C)

Gas Temperature at Core Outlet (0C) Nominal (1008 0C)

DHR Structural Temperature (0C)Nominal (386 0C)

Blower Inertia 1056.56 1053.00 388.50

Power 1043.78 1039.00 394.18

Residual Power 1033.00 1030.00 416.67

Pressure 1032.00 1028.00 385.90

Primary heat Transfer Area

1042.00 1041.00 382.0

Core Pressure Drop 1030.00 1025.00 390.50

Thermal Inertia 1013.33 1008.83 396.70

DHR Heat Transfer Area 1013.30 1008.79 390.60

Inlet Loss Coefficient 1013.44 1008.83 402.02

Outlet Loss Coefficient 1013.54 1008.93 402.35

Failure limits; Clad T > 1600 deg C

Gas T > 1050 deg C

DHR Structural T > 850 deg C

Page 66: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Statistical treatment on the effects of most critical parameters

Page 67: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Statistical analysis on the effects of most critical parameters

Clad Surface Temp (0C) Gas Temp at Channel Outlet(0C)

DHR Structural Temp(0C)

Average(µ) 1029.59 1011.75 389.8463

Standard Deviation( )σ 42.6107 54.62799 10.0725

Variation Coefficient( / µ) in %σ

4.138609 5.4 2.58

Minimum 962.61 901.18 374.00

Maximum 1134.22 1134.00 409.00

X90%1084.131 1081.674 402.7391

X95%1099.897 1101.886 406.4659

X99%1128.871 1139.033 413.3152

X99.99%1191.508 1219.336 428.1218

Page 68: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Reliability Assessment of Passive Decay Heat Removal System of GFR using APSRA Methodology

Page 69: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Identification of natural circulation failure

CriterionFailure limit

(DHR loop structural integrity)Maximum temperature of DHR structural material

 850 °C

Maximum clad temperature1600 °C

(Core upper structures integrity)Maximum temperature of gas at hot channel outlet 1050 °C

For SBO conditions, natural circulation failure in GFR is considered to occur according to the conditions given in Table

Page 70: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Important parameters affecting the performance of the system

1. Core power2. Residual Power 3. Main Circuit Pressure4. Fuel Heat Transfer coefficient 5. Heat Transfer coefficient in DHR secondary side 6. DHR primary side inlet Loss coefficient 7. DHR primary side outlet Loss coefficient 8. Pressure drop in fuel channels9. Thermal Inertia of primary system components 10. Primary Blower Inertia  Out of these parameters listed above parameters 1-3 are the

operating process parameters of DHR primary circuit & 4-10 are the model parameters.

Page 71: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of process parameters in combination on failure without consideration of modeling uncertainty

Fig shows an example of the effects of increase of residual power and initial operating power from their nominal values on system behavior while the system operates at nominal pressure of 6.98 MPa. It can be observed that the gas temperature exceeds the failure criteria limits even though the clad surface temperature and DHR structural temperatures have large margins to failure.

0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000 5500 6000

200

300

400

500

600

700

800

900

1000

1100

Te

mp

era

ture

(0 C)

Time(s)

Clad Surface Temperature(0C)

DHR Structural Temperature(0C)

Gas Temperature at Channel outlet(0C)

Fig: Nominal Pressure Residual power and initial power varied (Without model uncertainty)

Page 72: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of process parameters on failure without consideration of modeling uncertainty

Fig shows an example of the effect of decrease of main circuit pressure together with increase of nominal operating power on system behavior. In this case also the gas temperature at hot channel outlet exceeds the failure limit. Such failure cases are summarized in table.

0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000 5500 6000

200

250300350

400450500

550600650

700750

800850900

95010001050

1100

T

empe

ratu

re (

0C

)

Time(s)

DHR Structural Temp. Clad Surface Temp. Gas Temp. at Channel out

Fig: Pressure decreased nominal Residual power and initial power increased

Parameters/Cases Normalized

Pressure

Normalized Residual

Power

Normalized Power

1 0.98 1.1 1.02 0.98 1.0 1.013 1.01433 1.1 1.014 0.99 1.1 1.0125 1.0 1.1 1.0156 0.98 0.9 1.027 1.02 1.1 1.028 1.01433 1.05 1.029 0.99 0.99 1.02

Page 73: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Effect of model uncertainty on failure

Fig-40 shows an example of the effect of the variation of operating power which is decreased by 2% and residual power which is decreased by 10% keeping the system pressure at nominal value. The system in this case is found to be safe. However when model uncertainty is applied to this case the system is found to fail as shown in Fig-41. The model uncertainty is treated by considering the worst combination of all model parameters in this case.

0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000 5500 6000

200

300

400

500

600

700

800

900

1000

Tem

pera

ture

(0C

)

Time(s)

Clad Surface Temp. DHR structural Temp. Gas Temperature at channel outlet

Fig-40 Nominal Pressure, Residual power and initial power decreased

(Without model uncertainty)

0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000 5500 6000100

200

300

400

500

600

700

800

900

1000

1100

Te

mp

era

ture

(0 C)

Time(s)

Clad Surface Temperature(0C)

DHR Structure Temperature(0C)

Gas Temperature at Channel outlet (0C)

Fig-41 Nominal Pressure, Residual power and initial power decreased

(With model uncertainty)

Page 74: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Failure cases with Process and Model parameters

Parameters/Cases Normalized

Pressure

Normalized Residual

PowerNormalized Power

1 1.0 1.0 1.0

2 1.0 0.9 0.98

3 1.02 0.9 1.0

4 1.01433 0.9 0.987

5 1.02 1.0 0.98

6 1.01433 0.99 0.98

7 1.01433 0.985 0.985

8 1.019 0.9 0.995

Page 75: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Failure surface generation

Pressure

Residual Power

Page 76: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Root Diagnosis The root causes for the variation of the process

parameters are not known for GFR. Hence, the causes for failure are assumed in this exercise as an example of demonstration of application of APSRA methodology and not to accurately predict its reliability.

The failure probability of the PDHRS, depends on the variation of the three process parameters of the main heat transport system as discussed before.

Page 77: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Typical Fault Tree considering deviation of process parameters

Page 78: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Typical Fault Tree considering deviation of process parameters along with model uncertainty

Page 79: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Failure Frequency without model uncertainty

Page 80: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Failure Frequency with consideration of model uncertainty

Page 81: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

The failure frequency of PDHR system in the GFR has been calculated and found to be 7.052 × 10−6/h, considering variation of process parameters only. With considerations of model uncertainty (all model parameters varied to their worst combination) the system is found to fail at nominal operating conditions.The failure frequency of the PDHRS system is found to be 7.3× 10−6/h by considering the model uncertainty. The result shows that contribution of model uncertainty is negligible (around 4%).

Page 82: A.K. Nayak, PhD Reactor Engineering Division Bhabha Atomic Research Centre Trombay, Mumbai 400085

Conclusions For the benchmark-1 exercise during SBO

transient it is found that only one DHR natural circulation loop is sufficient for removing all the decay heat of the reactor to keep the reactor safe.

Even though the operating parameters of the reactors are varied to a possible range then no failure is found.

Clad surface temperature and DHR structural temperature are far below their failure limit. There is least margin in gas temperature at channel outlet which is also sufficient.