Can Thorium Outperform Uranium in Energy Production Per Kilogram?

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SUMMARY

Thorium-232 (Th-232) can be used as a fertile material to breed fissile Uranium-233 (U-233) in nuclear reactors, potentially outperforming Uranium-235 (U-235) in energy production per kilogram. The energy released per fission for U-233 is 197.9 MeV, compared to 202.5 MeV for U-235 and 207.1 MeV for Plutonium-239 (Pu-239). In light water reactors (LWRs), fuel enrichment is typically limited to 5%, while fast reactors can utilize higher enrichments of 20% or more. The fission rate and energy recovery from neutron capture reactions significantly influence the overall energy output of these systems.

PREREQUISITES
  • Understanding of nuclear fission processes
  • Familiarity with isotopes U-233, U-235, and Pu-239
  • Knowledge of reactor types, specifically light water reactors (LWRs) and fast reactors
  • Basic principles of energy release in nuclear reactions
NEXT STEPS
  • Research the energy production capabilities of Thorium reactors
  • Learn about the design and operation of fast reactors
  • Explore the differences in fuel enrichment requirements for various reactor types
  • Investigate the neutron capture processes and their impact on energy recovery
USEFUL FOR

Nuclear engineers, energy policy analysts, researchers in alternative fuel sources, and anyone interested in the comparative analysis of thorium and uranium in energy production.

DLHill
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In a reactor using Th232 as a fertile material to breed fissile U233, what is the amount of energy released per kg Th232 compared to a reactor using about 20% enriched uranium?
 
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DLHill said:
In a reactor using Th232 as a fertile material to breed fissile U233, what is the amount of energy released per kg Th232 compared to a reactor using about 20% enriched uranium?
The rate of energy release depends on two things: 1) energy per fission, and 2) fission rate.

The fission rate is carefully controlled such that the fuel state (e.g., temperature) remains within certain specified design limits, and would be constrained to certain limits if the system is upset.

20% enrichment would be rather high for a commercial (LWR) reactor, for which fuel is limited to 5%. Some small research reactors use highly enriched fuels since the core are small, and the fuel is not so optimized for the core size. Fast reactors, do use higher enrichments of 20% or more, and usually Pu-239 in the form of (U,Pu) ceramics (MO2, MN or MC, where M = U, Pu).

The energy per fission is:

Code:
Isotope                         U-233   U-235   Pu-239 
Energy per fission   (MeV)      197.9   202.5    207.1
Energy in anti-neutrinos (MeV)    6.9     8.8      7.1
Recoverable energy    (MeV)     191.0   193.7    200.0
Another ~ 3 - 12 MeV can be recovered from capture gammas from the neutron capture (n, γ) reaction. The neutrons may be captured by fuel, but not cause fission, or they are captured by the coolant and structural (non-fuel) material, e.g., cladding.

Ref: http://www.kayelaby.npl.co.uk/atomic_and_nuclear_physics/4_7/4_7_1.html

In a thermal Th-breeder system, there would be some fissile species, e.g., U-233 or U-235, usually U-235 in the beginning and later U-233 as it becomes available.

In LWRs, about 8-10% of fissions are fast-neutron induced fissions in U-238, with the remaining fissions mostly due to thermal neutrons fissioning U-235 and Pu-239, as the Pu is produced in the reactor.
 

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