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T. Kunugi, T. Nakai, Z. Kawara Department of Nuclear Engineering

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Presentation on theme: "T. Kunugi, T. Nakai, Z. Kawara Department of Nuclear Engineering"— Presentation transcript:

1 Falling Liquid Film Flow along Cascade-type First Wall of Laser-Fusion Reactor
T. Kunugi, T. Nakai, Z. Kawara Department of Nuclear Engineering Kyoto University, Japan Collaborated with T. Norimatsu ILE Osaka University, Japan Lijiang river

2 Design specification of KOYO-Fast
Net output MWe (300 MWe x 4) Reactor module net output 300 MWe Laser energy 1.2MJ Target gain 167 Fusion pulse out put 200 MJ  Reactor pulse rep-rate 4 Hz Reactor module fusion outputr MWth Blanket energy multiplication 1.13 Reactor thermal output 904 MWth Total plant thermal output MWth (904 MWth x 4 ) Thermal electric efficiency %(LiPb Temperature ~500 C) Total electric output MWe laser efficiency 8.5% (implosion) , 5% (heating) Laser pulse rep-rat 16 Hz Laser recirculating power 240 MWe(1.2 MJ x 16 Hz / 0.08) Net plant out put power 1200 MWe(1519MWe - 240MWe - 79MWe Aux.) Total plant efficiency %( 1200 MWe/ 3616 MWth)

3 Basic design concept for PbLi chamber
No pressurized pipe or vessel in the chamber for avoiding high pressure in chamber in accidents, and for achieving simple maintenance and long life use. Free surface fast cooling using divergent flow thorough from bulk flow (small holes or slit structure ⇒ Cascade-typed FW) Feritic steal is used for cylindrical vessel and upper dome cover vessel SiC/SiC is used as separate wall without pressure bulkhead Adjusting holes or slits on the separate to control divergent flow for stabilizing and fast cooling free surface (200ms for renewal of FW) Two layers PbLi blankets (~20 cm for free surface first wall and ~80 cm for blanket) and ~45cm graphite neutron reflector. SiC wall Feritic Steal C PbLi PbLi 50 mm 450 mm 800 mm 200 mm

4 Cascade-typed FW Concept
LiPb Flow Graphite 45 cm SiC/SiC porous wall container The coolant flows downward along FW → into reservoir behind FW → flows laterally to a slit → goes upward into the slit → past the exit of the slit → some of the overflowed coolant forms a falling liquid-film flow Ablation control by FW inclination Free-surface flow control by cascade passage

5 KOYO reactor cross-sectional view
LiPb flow inlet ( oC) Laser fusion modular power plant "KOYO" design, which has four reactor chambers driven by one laser system, was proposed . Reflector Gas coolant outlet Gas coolant inlet Cascade typed Liquid wall LiPb flow outlet( oC) KOYO laser-fusion reactor

6 Thermal flow of KOYO-F ( One module)
300 MWe 200MJ /shot x 4Hz hther-elec=30%

7 Cascade-typed Liquid Wall
Mixing is not sufficiency Surface temperature rises As a result, the fluid does not mix well, and the surface temperature of the first wall is continuously rising. Some flow resistances to maintain the surface shape. Difficult to keep thickness of liquid film Primary design proposal Redesigned Cascade-typed liquid wall The fluid covering the surface heated at the upper unit does not enter the backside of FW. Making space between reservoir units ⇒ static pressure drop for each units could be kept constant 30cm The height of the first wall of each unit is set to 30cm corresponding to the surface renewal time: 4 Hz laser repetition

8 Proof-of-principle experiment
The flow visualization experiment was performed as a POP experiment. In order to examine the performance of the new cascade-typed FW concept, numerical simulation was performed using STREAM code with k-e turbulent model.

9 Similarity Law and Flow Condition of Visualization Test
In the actual reactor, Li17Pb83 will be working fluid and SiC/SiC composite material will be used for the first wall. In this case, the wall surface might have a lower wettability. In the present experiment, we used the acrylic resin board as the FW because of its lower wettability.    The major concern of this experiment is to know the stability feature of the liquid film flow, therefore, the Weber number is the key parameter ,where is based on the film thickness , velocity   , density   , and surface tension coefficient   . According to the similarity law, we can estimate the flow velocity ratio. Water:  =7.275×10-2[N/m]   =9.98×102 [kg/m3]   Li17Pb83:  =4.80×10-1[N/m]   =9.6×103 [kg/m3] 9

10 Experimental Setup Flow Condition Re:4800~9600 T=17.5[。c] Tank Pump
Drain Valve Flow Meter Electric Balance Flow Condition Re:4800~9600 T=17.5[。c]

11 Experimental results Overflow Liquid Film Flow
At the overflow regions, there are many small waves. The liquid-droplet generation from the liquid surface and the large wave on the liquid-film surface were not observed. These small waves might trigger free surface unstable motion of the falling liquid-film flow on FW. Liquid Film Flow The average flow velocity is 1.75 times (14 l/min) of Weber number coincident condition (8.0 l/min) with the actual reactor.

12 Break-up of FW liquid film
Film Break-up Film Break-up The averaged flow velocity is 0.75 times (6.0 l/min) of Weber number coincident condition (8.0 l/min) with an actual reactor condition.

13 Numerical Simulation Flow Direction Liquid Film Flow Overflow
 We performed the two-dimensional thermo-fluid simulation by using the MARS function of the STREAM (commercial 3-D thermo- fluid code, Software Cradle Co. Ltd. in Japan). Experiment Flow Direction 3mm Numerical Simulation Liquid Film Flow Overflow

14 Comparison between Exp. & CFD
3mm 3mm Computational Conditions Mesh:782800 Fluid1:Air Fluid2:Water Material:Acrylic resin Re=5806, T=20.0[。c] Experiment Numerical Simulation

15 CFD animation

16 Comparison between Water and LiPb
Water/Acrylic plate Li17Pb83/SiC

17 Comparison between Water and LiPb
Water/Acrylic plate Li17Pb83/SiC

18 Conclusions We proposed the cascade typed liquid wall concept, and conducted the POP experiments and the numerical simulation (CFD) based on the consideration of the similarity law. The CFD result qualitatively agreed with the POP flow visualization experiment, so that the cascade-typed liquid film system will be realized. We also confirmed that the stable liquid film with sufficient thickness (liquid wall covering the first wall) could be naturally formed. Therefore, it seems that this liquid wall concept might be possible to apply to the real reactor.


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