OPAL CNS Moderator Performance Weijian Lu OPAL CNS Reliability from - - PowerPoint PPT Presentation
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
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 (%)
OPAL Reactor Facilities
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
Heat Load vs Reactor Power
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)
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%
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)
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)
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.
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
Fuel Management Programs
- Cell code: CONDOR
- Diffusion code: CITVAP
– Flux and power density – Reactivity – Poison transients – Adjoint flux – Kinetic parameters
Core Power Density – Flux Tilt
CG4 beam tube CG1-3 beam tube D2O moderator D2 moderator Reactor Core
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
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