Axial xenon distribution in a PWR

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Discussion Overview

The discussion revolves around the axial distribution of xenon in a pressurized water reactor (PWR) core, particularly how it relates to power distribution and equilibrium conditions. Participants explore the factors influencing the differing shapes of axial xenon and power distributions, including thermal and neutron flux characteristics, as well as operational parameters affecting xenon behavior over time.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that when power distribution shifts towards the bottom of the core, the xenon concentration shifts towards the top, raising questions about the equilibrium conditions and the shape of the distributions.
  • Another participant suggests that the fast-to-thermal flux ratio at the top of the core affects neutron capture by xenon, although they have not performed quantitative analysis on this effect.
  • Participants discuss the influence of fuel temperature and moderator density on xenon distribution, indicating that the top of the core is hotter and has lower moderator density, which may impact xenon behavior.
  • There is mention of the axial offset (AO) being influenced by burnable absorber distribution and operational parameters like the RCCA program and ascension rate, which may affect xenon swings at the beginning of cycle (BOC).
  • One participant agrees with another's explanation that xenon is more sensitive to a harder neutron spectrum than the fuel, leading to a greater production of xenon at the top of the core compared to absorption.

Areas of Agreement / Disagreement

Participants express various viewpoints on the factors affecting axial xenon distribution, with some agreeing on the influence of neutron flux and temperature, while others raise additional considerations. The discussion remains unresolved regarding the precise mechanisms and their relative impacts.

Contextual Notes

Participants highlight the dependence of their claims on specific operational conditions and parameters, such as burnup, fuel temperature, and neutron flux characteristics. There is also mention of the need for quantitative analysis to better understand the effects discussed.

Who May Find This Useful

This discussion may be of interest to professionals and students in nuclear engineering, particularly those focused on reactor physics and core behavior in pressurized water reactors.

ulriksvensson
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Hi all. I discovered a thing the other day that I've known for a long time but never really thought about.

If power distribution is shifted towards the bottom of the core the xenon concentration is shifted towards the top of the core. This is equilibrium conditions, i.e. only very small axial oscillations. Can someone explain this? If you raise power, xenon (equilibrium) concentration goes up. Why doesn't the axial xenon distribution have the same shape as the power distribution at equilibrium?

The difference between the "axial xenon offset" and axial offset vary some with burnup, but overall they are "opposite" in shape. Also, in coast down the tend to meet, suggesting a power level where the axial xenon distribution gets the same shape as axial power distribution.

Thanks in advance.

//Ulrik
 
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Fast-to-thermal flux ratio is one thing that has an effect in that direction: at the top of the core the average neutron velocities are faster; thus less neutrons are captured by Xenon.

Never done any quantitative analysis of the magnitude of that effect, though,
 
Yeah, that's probably it. Should've thought of that. It also explains the phenomenon at coast down when T-in is lowered.
 
Fuel temperature is slightly hotter in the top of the core, and moderator density is slightly lower in the top than the bottom of the core. Typical Tin ~ 285-293 C, and exit is something like 320-330 C depending on flow rates and power density.

AO is also affected by burnable absorber distribution. Some plants may have a slight axial offset on the IFBA loading. I haven't heard that for Gad though.

I have had some experience with looking at the Xe swings at BOC. The magnitude is affected by RCCA program and ascension rate. I believe there is also an effect from delta AO between EOC and BOC, as well as outage length.
 
Astronuc said:
Fuel temperature is slightly hotter in the top of the core, and moderator density is slightly lower in the top than the bottom of the core. Typical Tin ~ 285-293 C, and exit is something like 320-330 C depending on flow rates and power density.

AO is also affected by burnable absorber distribution. Some plants may have a slight axial offset on the IFBA loading. I haven't heard that for Gad though.

I have had some experience with looking at the Xe swings at BOC. The magnitude is affected by RCCA program and ascension rate. I believe there is also an effect from delta AO between EOC and BOC, as well as outage length.

I believe what the OP was inquiring was how can you have a xenon offset different from your axial offset in equilibrium conditions (i.e. steady state, no xenon transient). I agree with rmattila's answer - the reason is that xenon is more sensitive to a harder neutron spectrum than the fuel is. At the top of the core, you have a greater production of xenon compared to absorption, and thus a balanced positive xenon offset.
 

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