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2017 | OriginalPaper | Buchkapitel

12. Reactor Dynamics

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Abstract

In order for nuclear fission power to operate at a constant power level, the rate of neutron production via fission reactions must be exactly balanced by neutron loss via absorption and leakage. If we deviate from this simple balancing role, it would cause in a time dependence of neutron population and therefore the power level of the reactor. Such situation may take place, for a number reasons, such as reactor operator may have a requirement to change the reactor power level by temporarily altering the control fuel rod so it will change the core or source multiplication, or there may be long-term changes in core multiplication due to fuel depletion and isotopic buildup. Other examples may also be encountered that requires attention and adjustment to the day-to-day operation of the reactor, such as unforeseen accident or failure of primary coolant pump system, etc. The topic of nuclear kinetic reactor as we have learned in the previous chapter is handling this situation by allowing us to be able to predict the time behavior of the neutron population in a reactor core driven by changes in reactor multiplication, which is not a circumstance that is totally controlled by the operator of power plant and reactor core. Furthermore, variables such as indirect accessibility to control such fuel temperature or coolant density distribution throughout the reactor do have impact to the situation. However, these variables depend on the reactor power level and hence the neutron fluxes itself. Additionally, the study of the time dependence of the related process, which is involved with determining the core multiplication as a function of power level of the reactor multiplication, is the subject of our study in this chapter, and it is called nuclear reactor dynamics. This usually involves with detailed modeling of the entire nuclear steam supply system, which is part of feedback system as well.

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Literatur
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Zurück zum Zitat Net electrical MWe and gross MWe vary slightly from summer to winter, so normally the lower summer figure, or an average figure, is used. If the summer figure is quoted plants may show a capacity factor greater than 100% in cooler times. Watts Bar PWR in Tennessee is, reported to run at about 1125 MWe in summer and about 1165 MWe net in winter, due to different condenser cooling water temperatures. Some design options, such as powering the main large feed-water pumps with electric motors (as in Evolutionary Power Reactor (EPR)) rather than steam turbines (taking steam before it gets to the main turbine-generator), explains some gross to net differences between different reactor types. The EPR has a relatively large drop from gross to net MWe for this reason. Net electrical MWe and gross MWe vary slightly from summer to winter, so normally the lower summer figure, or an average figure, is used. If the summer figure is quoted plants may show a capacity factor greater than 100% in cooler times. Watts Bar PWR in Tennessee is, reported to run at about 1125 MWe in summer and about 1165 MWe net in winter, due to different condenser cooling water temperatures. Some design options, such as powering the main large feed-water pumps with electric motors (as in Evolutionary Power Reactor (EPR)) rather than steam turbines (taking steam before it gets to the main turbine-generator), explains some gross to net differences between different reactor types. The EPR has a relatively large drop from gross to net MWe for this reason.
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Metadaten
Titel
Reactor Dynamics
verfasst von
Bahman Zohuri
Copyright-Jahr
2017
DOI
https://doi.org/10.1007/978-3-319-42964-9_12