ML092600643

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Handout 3 - Kewaunee Power Station, Agenda Setting Meeting 09/15/09
ML092600643
Person / Time
Site: Kewaunee Dominion icon.png
Issue date: 09/15/2009
From:
Dominion Energy Kewaunee
To:
Office of Nuclear Reactor Regulation
Tam P
Shared Package
ML092600030 List:
References
TAC MC4691
Download: ML092600643 (7)


Text

Kewaunee Power Station NRC Agenda Setting Meeting 9/15/2009 ALDEN Solving flow problems since 1894

RAI E9j: Concentrated sources of drainage

  • No concentrated spray and drainage sources are located in the immediate vicinity of the strainer
  • The closest source is modeled in the transport calculation and the flume wall calculation
  • The influence of the source can be seen in the calculated approach velocity profile
  • The drainage source influence was represented in the large flume test ALDEN Solving flow problems since 1894

Kewaunee Power Station NRC Agenda Setting Meeting 9/15/2009 ALDEN Solving flow problems since 1894

RAI E9j: Concentrated sources of drainage

  • No concentrated spray and drainage sources are located in the immediate vicinity of the strainer
  • The closest source is modeled in the transport calculation and the flume wall calculation
  • The influence of the source can be seen in the calculated approach velocity profile
  • The drainage source influence was represented in the large flume test ALDEN Solving flow problems since 1894

E13a--e: CFD modeling of containment flow E13a

  • Simulations were conducted using Fluent and followed the standard calculation methodology
  • The standard k- model was used for turbulence calculations
  • Debris transport calculations were conservatively performed at the water level for the start of recirculation
  • High transport fractions were obtained for most zones up to a tumbling velocity of 0.2 ft/sec ALDEN Solving flow problems since 1894

E13a--e: CFD modeling of containment flow E13a

  • Detailed accounting was performed to model spray and break flow drainage into the recirculation pool
  • Concentrated sources of falling water were treated ideally converting all water potential energy into kinetic energy
  • The debris interceptor curb was modeled with few simplifying assumptions
  • No assumptions with regard to debris interceptor debris loading were necessary
  • No credit was taken for lift-over-curb transport limitations over the debris interceptor curb ALDEN Solving flow problems since 1894

E15: Turbulence in containment and flume / test configuration

  • Flume configuration based on long-term recirculation conditions

- Achieved 14 minutes after recirculation start

  • Water level in containment for analysis and test maintained at 40.5

- 40.5 is water level for the start of recirculation

- Actual water depth is more than 2 ft higher for long-term recirculation

  • Velocity and turbulence levels in vicinity of strainer are low
  • Containment structure divides break flow into three sources distributing break flow momentum Long-term recirculation velocity magnitude (ft/s) Long-term recirculation TKE (ft2/s2)

ALDEN Solving flow problems since 1894

E15: Turbulence in containment and flume / test configuration

  • Debris interceptor, despite its low height blocks most break flow from reaching strainer
  • Flume Reynolds numbers are in the turbulent range
  • Flume effective turbulence is on par with that calculated in containment
  • Turbulence levels calculated in containment correspond to a maximum of 0.02 ft/sec RM 0.0025 0.002 Distance from Velocity Flume Width Hydraulic Radius screen (ft) (ft/sec) (in) (ft) Reynolds #

Turbulent kinetic Energy (ft2/s2)

Containment Turbulence Flume Turbulence 0.0015 1 0.10 10.4 0.39 6704 2 0.10 9.9 0.37 6045 3 0.10 11.3 0.41 6644 0.001 6 0.08 14.3 0.51 6435 10 0.09 11.7 0.42 6617 0.0005 21 0.12 8.9 0.33 6821 25 0.13 8.5 0.32 6852 0

0 5 10 15 20 25 30 35 30 0.13 8.4 0.32 6861 Distance Back From Strainer (ft)

ALDEN Solving flow problems since 1894

E16: Pool fill transport & distance traveled by debris

  • Preferential pool fill transport is limited except during sump C fill-up
  • Sump C fill-up preferentially causes debris to move away from strainer bank
  • No credit for this transport is taken in the analysis
  • The average distance traveled by debris is greater than 30 when considering calculated zone exit flow splits
  • TempMat calculated transport fraction was increased by 20% of debris generated for conservatism in determining test quantity
  • Transport testing at Alden showed 3x - 4x approach velocity profile only yielded partial transport of TempMat smalls.

ALDEN Solving flow problems since 1894