Status of helium-cooled Plate-Type Divertor Design, CFD and Stress Analysis

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Status of helium-cooled Plate-Type Divertor Design, CFD and Stress Analysis Presented by: X.R. Wang Contributors: R. Raffray, S. Malang and the ARIES Team ARIES-TNS Meeting March 3-4, 2008 UCSD, La Jolla, CA

Helium-Cooled Plate-Type Divertor 5 mm W Tile 3 mm Modified to 2 mm 5 mm 50 cm 20 cm W (Old) 8 mm Symmetry plane Based on initial thermo-fluid and thermo mechanical results, the configuration of the flat plate divertor has been modified: 10 mm (New) Reducing the thickness of the front structure to reduce the maximum structure temperature Increasing the thickness of the back plate to rise the temperature level at the back Making the front structure (high pressure container) with a large curvature to reduce local stresses

Cooling Methods Three Impinging jet cooling schemes are investigated to enhance heat transfer coefficient in order to meet design requirements: Max. structural temperature < 1300 o C; 1. Slot jet 2. Slot jet with micro-channel (H~0.25 mm) Max. structure stress <450 MPa (3Sm); Ratio of the pumping power to thermal power, P p /P th < 10% 3. Multiple impinging jet arrays

CFD Thermo-fluid Model for Slot Jet Cooling Heat transfer of a single impinging jet depends on the nozzle-to-wall distance, H, width of the nozzle, D. ARIES-CS reference design parameters are assumed: Nozzle-to-wall distance H=1.2 mm*, Nozzle width D=0.5 mm*, q =10 MW/m 2, q =53 MW/m 3 Inlet pressure=10 MPa Toutlet-Tinlet=950-873 K *S. I. Abdel-Khalik et al., to be published in Fusion Sic.& Tech *T. Ihli, A.R. Raffray et al., Fusion Eng.& Des., 82 (2007) Only 2 cm plate-length (in z-direction) is simulated because huge amount of elements and computer memory are required for full length plate (~0.65 million elements for this model). Standard turbulent flow model, K-epsilon is used in CFD model. Rough wall is assumed. Roughness height=10 micron. Helium W ODS Inflated boundary layers (fine elements) are used at helium/w structure interface. 2 cm

Thermo-fluid Results for Slot Jet Cooling Max. v=254.6 m/s Velocity distribution Max. h=3.84x10 4 W/m 2 K (Nozzle width d=0.5 mm, Jet-to-wall distance H=1.2 mm; mass flow=0.005925 kg/s)

Thermo-fluid Results for Slot Jet Cooling (Cont.) W Structure temperature distribution W Tile temperature distribution The max. structure temperature is 1579 K (~1573 K, allowable temperature) Pressure drop P =10.183-10=0.183 MPa P p /P th ~8.7% (<10%, design limit)

CFD Thermo-fluid Model for Micro-channel Cooling Nozzle width d=0.5 mm, channel space H=0.25 mm Thermal loads and mass flow rate are the same as the slot jet cooling model. 0.25 mm 2 cm Standard turbulent flow model, K-epsilon is used in CFD model. Rough wall is assumed. Roughness height=10 micron.

Thermo-fluid Results for Micro-channel Cooling Max V=305.6 m/s Velocity distribution Max. h=5.7x10 4 W/m 2 K (Nozzle width d=0.5 mm, micro-channel space H=0.25 mm; mass flow=0.005925 kg/s)

Thermo-fluid Results for Micro-channel Cooling (Cont.) Structure temperature distribution Coolant temperature distribution The max. structure temperature is 1521 K (<1573 K, allowable temperature). Pressure drop P =10.295-10=0.295 MPa. P p /P th ~14% (>10% design limit)

CFD Thermo-fluid Model for Multiple Impinging Jet Arrays Multiple jet flow characteristics: Three flow regions as the same as a single impinging jet 2 cm W-alloy ODS 2 cm Possible interaction prior to their impingement (jet space too close, or H too large) Possible interaction due to collision of the wall jets Cross-flow for the jets on the edge of the arrays. Mass flow=0.005925 kg/s In-line Helium H=1.2 mm D=0.6 mm A jet_arrays =A slot_jet Holes/cm =18 S/D=5.56~6 Thermal loads are the same S (pitch) Total elements=0.76 million

CFD Results for Multiple Impinging Jet Arrays (18 Holes/cm) H=1.2 mm, D=0.6 mm, S/D=5.56~6 Mass flow rate=0.005925 kg/s Max. v=291.3 m/s, Max. local h.t.c. h=3.22x10 4 W/m 2 K Max. He/W interface temperature=1548 K Max. W structure temperature=1703 K (>1573 K) Pressure drop=10.26-10=0.26 MPa P p /P th ~12.3% (>10% design limit)

Impinging Jets Reduced to 13 Holes/cm to Increase Velocity and Heat Transfer H=1.2 mm, D=0.6 mm, S/D=5.56 Mass flow rate=0.005925 kg/s Arrangement of the Jet Arrays Max. v=336.1 m/s, Max. local h.t.c. h=3.89x10 4 W/m 2 K Max. He/W interface temperature=1454 K Max. W structure temperature=1609 K (>1573 K) Pressure drop=10.441-10=0.441 MPa, P p /P th ~20.9% (>10% )

Parametric Study for Multiple Jets (13 Holes/cm, Jet-to-wall Distance H=1.2 mm) Nozzle Diameter D=0.4 mm Nozzle Diameter D=0.6 mm Nozzle Diameter D=0.8 mm Nozzle Diameter D=1mm Slot Jet D=0.5 mm Max. Velocity [m/s] 703.4 336.1 202.2 140.5 254.6 Max Local Heat Transfer Coefficient 5.736x10 4 3.899x10 4 2.808x10 4 2.659x10 4 3.839x10 4 [W/m 2 K] Max W/He Interface Temperature, [K] 1303 1454 1650 1677 1406 Max W Structure Temperature, [K] 1449 1609 1785 1831 1579 P [Pa] 24.5 x 10 5 4.41 x 10 5 1.43 x 10 5 0.60 x 10 5 1.83x10 5 P p /P th, % 116.1 20.9 6.8 2.8 8.7

Parametric Study for Multiple Jets (13 Holes/cm, Nozzle Diameter D=0.6 mm) Jet-to-Wall Jet-to-Wall Jet-to-wall Slot Jet Space Space Space H=1.2 mm H=1.5 mm H=1.2 mm H=0.9 mm D=0.5 mm Max. Velocity [m/s] 312.8 336.1 339.2 254.6 Max Local Heat Transfer Coefficient 3.661x10 4 3.899x10 4 3.901x10 4 3.839x10 4 [W/m 2 K] Max W/He Interface Temperature, [K] 1495 1454 1443 1406 Max W Structure Temperature, [K] 1650 1609 1592 1579 P [Pa] 4.13 x 10 5 4.41 x 10 5 4.42 x 10 5 1.83x10 5 P p /P th, % 19.6 20.9 21.0 8.7

Parametric Study for Multiple Jet (13 Holes/cm, Jet-to-wall Distance H=1.2 mm) Effective Heat Transfer Coefficient, MW/m 2 28000 26000 24000 22000 20000 18000 16000 14000 12000 10000 0.4 0.6 0.8 1 Nozzle Diameter, mm Max. Tungsten Structure Temperature, K 1900 1800 1700 1600 1500 1400 1300 1200 1100 1000 Temperature Design Limit 0.4 0.6 0.8 1 Nozzle Diameter, mm 120 110 100 90 80 70 60 50 40 30 20 10 0 Ratio of the Pumping Power to Thermal power, % h eff =q /(T max at interface T ave. helium )

Full-length Model for Thermo-mechanical Analysis The flat plate divertor with slot jet cooling scheme is selected as the reference for stress analysis. ODS insert manifold is excluded from thermo-mechanical model. Temperature at the interface of the He/W is assumed to be uniform in Z- direction (CFX results) in ANSYS thermal analysis. 1 m Two different support conditions are assumed for the thermomechanical simulation. The plate is not allowed to bend, but free to expand. The plate is allowed to expand and bend. Y Z X Helium Temperature distribution from CFX

Temperature Distribution from ANSYS Multi-physics Max. Temperature at W tile T~1800 o C Max. Temperature at W structure T~1300 o C Y Z X

Stress and Deformation for Support Condition 1 Max. von-mises Stress σ~ 540 MPa Y Z X Max. Thermal Deformation δ~0.54 mm

Stress and Deformation for Support Condition 2 Max. von-mises Stress σ~ 651 MPa Z Y X Max. Thermal Deformation δ~1.25 mm

Summary Thermo-fluid and thermo-mechanical analyses have been performed for the helium-cooled flat plate and T-tube divertor concepts with heat loads up to 10 MW/m 2. T-tube Divertor Concept with the slot jet cooling has been considered as reference design of the ARIES-CS stellarator power plant and it will also be suited for tokamak power plant. The thermo-fluid and thermo-mechanical results are re-produced by CFX and Workbench. Heat transfer, High (~3.7x10 4 W/m 2 K) Pumping power, Ok W Temperature, Ok Stress, Ok 75,000~110,000 T-tubes for one plant (for divertor area: 100~150 m 2 ) Flat Plate Divertor Concept with the slot jet, the micro-channel and the multiple jet arrays have been investigated. The thermo-mechanical analysis have been performed only for the flat plate divertor with the slot jet cooling scheme. Heat transfer, high (~3.9x10 4 W/m 2 K) Pumping power, Ok W Structure temperature, Ok Stress, > the 3Sm (450 MPa) 500~750 flat plates for one plant (for divertor area:100~150 m 2 ) Further to look into the multiple jets to see if the performance could be improved Further to look into the flat plate divertor concept to see if it is possible to improve the design to reduce the thermal stress