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An ADS core dedicated for MA transmutation (MA-ADS) [8] bases the present design for Pu transmutation. As listed in Table 19.1, the MA-ADS is a medium-size core loaded with nitride fuel cooled by lead-bismuth eutectic (LBE). Nitride fuel is diluted by zirconium-nitride with a weight fraction of around 50 % (volume fraction around 65 %) that can be changed so that criticality becomes an appropriate level (keff = 0.97). The ADS is operated for 600 effective full-power days (EFPDs) without any fuel reloading while the interval for maintenance of an accelerator can occur. In other words, the ADS is a one-batch core that implies large reactivity drop after depletion in the case of Pu transmutation. Because control rods for criticality are not equipped in the ADS, the drop must be supplemented by
Thermal power |
800 MWt |
Electricity generation |
260 MWe |
Proton energy |
1.5 GeV |
Transmutation rate |
250 kg/300 EFPDs |
Coolant |
LBE |
Upper limitation of keff |
0.97 |
Operation period |
600 EFPDs |
Batch number |
1 |
Fuel composition |
(Pu+MA)N+ZrN |
Pin outer diameter |
7.65 mm |
Pin pitch |
11.48 mm |
Table 19.1 Parameters of minor actinides-accelerator — driven system (MA-ADS) [8] |
MA-ADS (%) |
|
Np-237 |
49.5 |
Am-241 |
32.2 |
Am-243 |
13.4 |
Cm-244 |
4.4 |
Cm-245 |
0.4 |
Table 19.2 MA composition fed to MA-ADS |
ADS case |
Pu (%) |
Pu+U (%) |
U-235 |
— |
0.1 |
U-238 |
— |
49.9 |
Pu-238 |
2.4 |
1.2 |
Pu-239 |
54.5 |
27.2 |
Pu-240 |
24.2 |
12.1 |
Pu-241 |
11.9 |
6.0 |
Pu-242 |
7.0 |
3.5 |
increasing proton beam current. Fortunately, MAs are fertile material that becomes fissile after capturing one neutron, and the drop is very small, as shown in the following section. Table 19.3 provides weight composition of MA fed to MA-ADS. Figure 19.2 illustrates the R-Z model for calculation.