IAEA meeting Evaluation of creep during dry storage in low and high burnup fuels F.

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Transcript IAEA meeting Evaluation of creep during dry storage in low and high burnup fuels F.

IAEA meeting

Evaluation of creep during dry storage in low and high burnup fuels

F. Feria, L.E. Herranz CONTENTS 1.

2.

3.

4.

Motivation and objective Extension of FRAPCON-3.3 creep law Creep assessment Final remarks Nuclear Safety Research Unit Vienna (Austria), 31.05-4.06.2010

1. MOTIVATION AND OBJECTIVE

Safety objectives:

-

Radiation dose Subcriticality Confinement Retrievability Cladding integrity Degrading mechanisms IAEA meeting SCC Creep DHC Evaluation in low and high burnup Nuclear Safety Research Unit Vienna (Austria), 31.05-4.06.2010

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2. EXTENSION OF FRAPCON-3.3 CREEP LAW

In-FRAPCON modelling

 i   i e   i p  d  i p   i T i   , z , r d  p  c  dt

Creep law:

  c  4  c ( f 1 (   )· f 2 ( T )· f 3 (  )) 2

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f 1 (   )     725.2

exp( 4.967·10 -8   ) f 2 ( T )  exp(  10000 / RT ) f 3 (  )  5.129·10 -29 

Vienna (Austria), 31.05-4.06.2010

2. EXTENSION OF FRAPCON-3.3 CREEP LAW

Creep law validity range IAEA meeting Restricted to in-reactor conditions Extension of the creep law is needed to apply the code to dry storage conditions Nuclear Safety Research Unit Vienna (Austria), 31.05-4.06.2010

2. EXTENSION OF FRAPCON-3.3 CREEP LAW

Zircaloy-4 database (EDF) IAEA meeting Generic correlation Nuclear Safety Research Unit

 c   c p   c s  i c  f 1 i (   )· f 2 i ( T )· f 3 i (  t )· f 4 i ( t ) i  p , s

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2. EXTENSION OF FRAPCON-3.3 CREEP LAW

CIEMAT creep law

  f 1 (   )· f 2 ( T )· f 3 (  t )· t  0 .

5 f 1 (   f 2 ( T ) )  a 2  b   exp   T   c 273   f 3 (  t )  exp(  d ·  t )

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2. EXTENSION OF FRAPCON-3.3 CREEP LAW

CIEMAT creep law

0.2

CIEMAT EDF 0.1

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0 0 200 400

t(h)

600 800 1000 0.3

0.2

0.1

CIEMAT EDF 0.0

0 100 200 300

t(h)

400 500

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600

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2. EXTENSION OF FRAPCON-3.3 CREEP LAW

Implementation Together with a suitable logic that allows choosing between the “in-reactor” equation and the dry storage equation, according to the prevailing conditions at the calculation time The extension splits in two hoop stress ranges:

  

≥ 121 MPa → Creep law parameters derived from irradiated claddings data

  

≤ 121 MPa → Creep law parameters derived from non-irradiated claddings data No experimental data is available with irradiated material under low hoop stress Nuclear Safety Research Unit Vienna (Austria), 31.05-4.06.2010

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3. CREEP ASSESMENT

40 35 30 25 20 15 10 5 0 0

Postulated scenarios a) Zircaloy-4 45 GWd/tU

500 1000

t(days)

1500 2000 0.8

0.6

0.4

0.2

0.0

0

Nuclear Safety Research Unit 1º) In-reactor irradiation 2º) Pool storage (1 year) 3º) Dry out (1 day) 4º) Dry storage (2 years)

200

Phases

400

t(days)

600 800 35 30 25 20 15 10 5 0 0 500

b) Zircaloy-4 63 GWd/tU

1000

t(days)

1500 2000 2500

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Trillo

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3. CREEP ASSESMENT

Results

0.2

0.1

0 -0.1

-0.2

-0.3

-0.4

-0.5

-0.6

-0.7

-0.8

0 400

a) Zircaloy-4 45 GWd/tU

In-pool cooling Dry storage Trillo2 800 1200

t(days)

1600 2000 2400 1.5

1 0.5

0 -0.5

-1 0 400 800

b) Zircaloy-4 63 GWd/tU

In-pool cooling Dry storage 1200

t(days)

1600 

Once dry storage starts hoop stress causes a creep-out situation

2000 2400

Nuclear Safety Research Unit Vienna (Austria), 31.05-4.06.2010

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3. CREEP ASSESMENT

Results

0.8

0.7

0.6

0.5

0.4

0.3

0.2

0.1

0 0 45 GWd/tU 63 GWd/tU 100 200 300 400

t(days)

500 600 700 800 

The creep main impact would take place during the first months

In no case creep reaches 1 % strain limit

Nearly 4 times higher hoop strain as burn-up is increased by 40 % Nuclear Safety Research Unit Vienna (Austria), 31.05-4.06.2010

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4. FINAL REMARKS

High burn-up effect seems substantial and causes major differences in the nuclear fuel response in terms of creep

The results would have a conservative nature because the irradiation hardening effect is not considered at low stresses

Further work:

Extend CIEMAT creep law to irradiated fuel rods submitted to low stresses

Extend the study up to 100 years to estimate the final creep asymptotic value Nuclear Safety Research Unit Vienna (Austria), 31.05-4.06.2010

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ACKNOWLEDGMENTS

The authors are indebted to ENRESA for their financial support and the technical discussions held and to the FRAPCON-3 developers for their technical support during this work Nuclear Safety Research Unit Vienna (Austria), 31.05-4.06.2010

IAEA meeting THANK YOU FOR YOUR ATTENTION Nuclear Safety Research Unit Vienna (Austria), 31.05-4.06.2010