2. The physics of fast breeder reactors
2.1 Principle of plutonium regeneration (over-, iso- or under-generation)
Fission of the nucleus of an atom, typically 239 Pu, releases energy of around 200 MeV, essentially in the form of kinetic energy carried by the fission products (FPs) within the fuel. This kinetic energy is then dissipated in thermal form by slowing down the FPs in the surrounding environment. So, to produce 1 TWh of heat, you need to fission around 44 kg of fissile material. Expressed in kg per TWh of electricity (noted TWhe), we need to take into account the electrical efficiency of the reactor-turbine assembly, which varies according to the type of nuclear reactor. For LWRs, with an efficiency of around 33%, fission is required at around 130 kg/TWhe. For RNRs...
Exclusive to subscribers. 97% yet to be discovered!
You do not have access to this resource.
Click here to request your free trial access!
Already subscribed? Log in!
The Ultimate Scientific and Technical Reference
This article is included in
Nuclear engineering
This offer includes:
Knowledge Base
Updated and enriched with articles validated by our scientific committees
Services
A set of exclusive tools to complement the resources
Practical Path
Operational and didactic, to guarantee the acquisition of transversal skills
Doc & Quiz
Interactive articles with quizzes, for constructive reading
The physics of fast breeder reactors
Bibliography
- (1) - CEA Direction de l'énergie nucléaire - La gestion durable des matières radioactives avec les réacteurs de 4e génération. - Déc. 2012 http://www.cea.fr/
- (2) - Loi n° 91-1381 du 30 décembre...
Exclusive to subscribers. 97% yet to be discovered!
You do not have access to this resource.
Click here to request your free trial access!
Already subscribed? Log in!
The Ultimate Scientific and Technical Reference