OPAL CNS Moderator Performance Weijian Lu OPAL CNS Reliability from - - PowerPoint PPT Presentation

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OPAL CNS Moderator Performance Weijian Lu OPAL CNS Reliability from - - PowerPoint PPT Presentation

OPAL CNS Moderator Performance Weijian Lu OPAL CNS Reliability from Commissioning (Nov 2006) to Present 100 90 80 70 CNS Reliability (%) 60 50 40 30 20 10 0 1 3 5 7 9 11 13 15 17 19 21 23 25 27 29 31 33 35 37 39 41 43 45 47 49 51


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SLIDE 1

OPAL CNS Moderator Performance

Weijian Lu

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SLIDE 2

10 20 30 40 50 60 70 80 90 100 1 3 5 7 9 11 13 15 17 19 21 23 25 27 29 31 33 35 37 39 41 43 45 47 49 51 53 55 57 59 61 63 65 67 69 71 73 75 77 79 81 83 85 87 89 91 93 95 97 99 CNS Reliability (%) Reactor Cycle No.

OPAL CNS Reliability from Commissioning (Nov 2006) to Present

CNS Reliability (%) OPAL Reliability (%)

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SLIDE 3

OPAL Reactor Facilities

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SLIDE 4

What Happened to CNS Flux?

  • In early 2017, neutron users have noticed a

significant drop in cold neutron flux ~ -20%

  • Possible causes

– Neutron guides (fault discovered in 2011) – Source flux

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SLIDE 5

Heat Load vs Reactor Power

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85% 90% 95% 100% 105% 110% 115%

CNS Heat Load vs Reactor Power

Nuclear Heat Load (normalised to 3.6 kW) OPAL Thermal Power (normalised to 20 MW)

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Helium Temperature Sensor Drift

  • Sensors had recently been checked
  • Measured a stable bias of ~1 K subject to slow

drift (years), but no evidence for cycle-to-cycle “oscillation”

Process Conditions (nominal) Sensitivity Typical Operational Variation by Conservative Estimation Resultant CNS Flux Variation Helium temp. sensor drift 15%/K ~ -1 K

  • 15%
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SLIDE 8

200 400 600 800 1000 1200 1400 1600 1800 2000 2200 2400 2600 2800 3000 3200 3400 3600 3800 4000 4200 4400

CNS Heat Load (watts)

Heat Load (watts)

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CNS Flux Sensitivity (1)

Process Conditions (nominal) Sensitivity Typical Operational Variation by Conservative Estimation Resultant CNS Flux Variation D2O purity (99.5%) 6.66%/% ±0.5% ±3.33% D2O temp. (35 °C)

  • 0.0228%/°C

±1 °C ±0.0228% D2O gap between CNS thimble and beam tube (1 mm)

  • 5.52%/mm

negligible negligible LD2 temp. (24.5 K)

  • 4.38%/K

±0.5 K ±2.2% LD2 ortho/para ratio (3:1) 0.288%/% Unknown but expected to be small ±1% (order of magnitude estimation)

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MCNP Calculation vs Measurement

0,95 0,96 0,97 0,98 0,99 1,00 1,01 1,02 1,03 1,04 1,05 1,06 1,07 1,08 1,09 1,10 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 Ratio Neutron Wavelength

CNS Gain from 20.5 K to 19.6 K (4 Dec 2016)

BILBY 5-Dec / 3-Dec MCNP Calc.

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SLIDE 11

CNS Flux Sensitivity (2)

Process Conditions (nominal) Sensitivity Typical Operational Variation by Conservative Estimation Resultant CNS Flux Variation Control rod positions (critical positions for the first core) 5.58% between actual configuration and that after 180° rotation Control rod movement pattern is repeated in every reactor cycle N/A Reactor core (first core and equilibrium core) 4.56% between the two cores Fuel management strategy To be assessed further

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Fuel Management Programs

  • Cell code: CONDOR
  • Diffusion code: CITVAP

– Flux and power density – Reactivity – Poison transients – Adjoint flux – Kinetic parameters

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Core Power Density – Flux Tilt

CG4 beam tube CG1-3 beam tube D2O moderator D2 moderator Reactor Core

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0,90 0,95 1,00 1,05 1,10 85% 90% 95% 100% 105% 110% 115%

CNS Heat Load vs Reactor Power

Nuclear Heat Load (normalised to 3.6 kW) OPAL Thermal Power (normalised to 20 MW) Flux Tile N-S biased to average

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SLIDE 15

Conclusions

  • CNS heat load is an excellent indicator of

source flux

  • Core configuration can have a significant

impact on the CNS flux

  • Can be predicted by numerical calculations
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SLIDE 16
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