Peaking factor and power profile

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Discussion Overview

The discussion revolves around the concepts of radial peaking factor and normalized radial power profile in the context of nuclear reactor fuel performance. Participants explore how these factors relate to local and core average power densities, and the implications for fuel integrity under various operational conditions.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants suggest that peaking factors are derived from normalized axial and radial power profiles, emphasizing the importance of local power in relation to core average power.
  • It is proposed that local power must be constrained to avoid fuel damage during anomalies or accidents, highlighting a safety consideration in reactor design.
  • Questions arise regarding the definition of peaking factors at specific axial and radial positions, particularly in relation to a single pin's power profile.
  • One participant describes the calculation of FdH and Fq(z) as ratios of total pin power to core power and local power density to core power density, respectively, indicating a multi-dimensional approach to understanding power profiles.
  • Another participant details the process of calculating local power density using core simulation codes, which account for neutron flux and local enrichment, suggesting a complex interplay of factors in determining peaking factors.
  • An example calculation is provided to illustrate how core average power density is derived from reactor specifications, though it remains unclear how this relates to the broader discussion of peaking factors.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and interpretation of peaking factors and their calculations, indicating that multiple competing views remain. The discussion does not reach a consensus on the definitions or methodologies involved.

Contextual Notes

Limitations in the discussion include assumptions about the definitions of power profiles and peaking factors, as well as the dependence on specific reactor configurations and simulation codes. Unresolved mathematical steps and the complexity of the calculations are acknowledged.

Vnt666Skr
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Is the radial peaking factor same as normalized radial power profile?
 
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Peaking factors are developed from normalized axial and radial/lateral power profiles.

One is interested in how the local power relates to the core average power, as well as the absolute magnitude of the power. Local power restricted by some margin to some absolute limit in order to ensure that under certain anticipated anomalies the fuel is not damaged, or in the event of a postulated accident, the fuel damage is limited and not underestimated.

From a fuel performance perspective, one wishes to 'flatten' the radial and axial profiles such that one minimizes corrosion and other irradiation-dependent behavior/consequences.
 
Thanks Astronuc.
Is it defined at each axial/radial position? Suppose I have a power profile of a single pin. How do I find out the peaking factors at various locations in the axial and radial direction?
 
Vnt666Skr said:
Thanks Astronuc.
Is it defined at each axial/radial position? Suppose I have a power profile of a single pin. How do I find out the peaking factors at various locations in the axial and radial direction?

FdH is ratio of the total pin power to the total core power divided by number of pins. This is a 2-D (radial) value and each pin as one value for FdH.

Fq(z) is the ratio of power density of the pin divided by the power density of the core. This is a 3-D (axial) value. Each pin has a Fq(z) as a function of height, and a peak Fq.

If your pin power profile is normalized, you need to first multiply by the assembly's relative power density. Fz is the maximum normalized power for the core, assembly, or pin.
 
Last edited:
Vnt666Skr said:
Thanks Astronuc.
Is it defined at each axial/radial position? Suppose I have a power profile of a single pin. How do I find out the peaking factors at various locations in the axial and radial direction?
A peaking factor would be determined from the local power density (or linear power) divided by the core average power density (or linear power). The average power density is found from the thermal rating of the reactor core divided by the total length of active fuel. The local power density is calculated with a core simulation code (e.g., SIMULATE or other proprietary code) which solves a multi-group neutron diffusion or transport problem. The codes calculate the neutron flux and local enrichment, which includes effects of depletion and transmutation, and from these determine the fission density, from power density is calculated.

An example of core average power. Given a 3700 MWt core, with 193 assemblies, 264 fuel rods per assembly, and an active fuel length of 12 ft (including blankets), the core average linear power in kW/ft is given by

3700000 kW / (193 * 264 * 12 ft) = 6.05 kW/ft or 19.85 kW/m
 

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