TUBRNP (Transuranus/FRAPCON) model

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Hello,

I am currently trying to understand the TUBRNP model which is used to calculate the isotope compositions and the radial power profile evolution with the burnup. I am talking about the basic model (the one from 1994 with only 6 isotopes taken into account) in the case of a LWR with UO2.

In order to understand it, I try to create a simple algorithm doing the same thing. i will be the burnup step and n the inner iteration index for convergence.
1) From an initial composition vector N_0 (determined with the enrichment), calculate the parameter A.

2) Determine the matrix M so that I can calculate the next composition N(n)_i+1 with N(n)_i+1*M=b with b depending on the old concentration N_old (see below the code for a given position):
Code:
function [M,b]=create_matrices(delta_BU,A,sigma_abs,sigma_capt,radial_pos,shape_function,N_average,N_old)
f_r=shape_function(radial_pos);

M=zeros(6);
%U235
M(1,1)=1+sigma_abs(1)*A*delta_BU;
%U238
M(2,2)=1;
%Pu239
M(3,3)=1+sigma_abs(3)*A*delta_BU;
%Pu240
M(4,3)=-sigma_capt(3)*A*delta_BU;
M(4,4)=1+sigma_abs(4)*A*delta_BU;
%Pu241
M(5,4)=-sigma_capt(4)*A*delta_BU;
M(5,5)=1+sigma_abs(5)*A*delta_BU;
%Pu242
M(6,5)=-sigma_capt(5)*A*delta_BU;
M(6,6)=1+sigma_abs(6)*A*delta_BU;

b=N_old;
b(2)=b(2)-N_average(2)*sigma_abs(2)*f_r*A*delta_BU;
b(3)=b(3)+N_average(2)*sigma_abs(2)*f_r*A*delta_BU;
3) Calculate the inverse diffusion length (kappa) from this new composition, then the flux with the Bessel function.
4) Calculate the power profile from the average power that I want and the flux.
5) Determine the burnup increment from the power, the initial uranium mass and the simulated time increment
6) Compare the compositions N(n)_i+1 and N(n-1)_i+1. If the difference is small enough, go to next burnup step, otherwise take N(n-1)_i+1 to calculate a new A and a new matrix M, ...

First, does this reproduce properly TUBRNP? I took the cross sections and the p_i parameters for the shape function from the FRAPCON user manual.

Then I have several issues with the shape function f(r). As there is a volumetric normalization step, the outer radius value matters. Thus, the unit of this parameter influences the results and unfortunately in the publication, no unit is given. If I try to reproduce the Plutonium radial profiles given in this paper with cm as units, the shape is not peak enough, but if I try with mm, it is not working either.

Finally, I face some problems calculating the conversion factor alpha. From what I understand, it is a factor created to convert time to burnup units. As I am working with MWd/kg_HM as burnup unit and cm as spatial unit, we have : [BU]=[alpha]*(fission/cm^3)/(kg/cm^3) =MWd/kg_HM
So for me : [alpha]=MWd/fission
alpha=200MeV/reac*1.602e-19/(24*3600)=3.7088e-22
If my calculation is correct, then why in the Lassman's paper the value of alpha is 3.35e-16 in the case of MWd/t_HM ? This 1e6 factor does not make sense to me.

I would really appreciate your help on this ! And if you have questions or if I have not been clear enough on a point, please ask me.
 

Astronuc

Staff Emeritus
Science Advisor
18,491
1,611
Which version of Frapcon? Besides the Frapcon manual, what are one's references?
I presume one references: K. Lassmann et al, Journal of Nuclear Materials 208, Issue 3, February 1994, pp. 223-231

Also, 1 MeV = 1.60218e-13 J.
 
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Hello and thank you for you answer,

I based this on the FRAPCON 3.4 Manual that can be found here : https://www.nrc.gov/docs/ML1110/ML11101A005.pdf from page 2.15 to 2.18

Moreover, the reference you put is the one I was talking about.

Regarding the conversion, I am using 1 Mev = 1.602e-19 MJ because the burnup unit is MWd/kg_HM, and in the case of the paper it is MWd/t_HM. Therefore, to my mind, this cannot be the reason of this 1e6 factor.
 

Astronuc

Staff Emeritus
Science Advisor
18,491
1,611
1 Mev = 1.602e-19 MJ
This is correct, but since one did not put the units, it looked like one off by a factor of 1e6.

In the paper, Lassmann states burnup in units of MWd/tHM, and 1 tHM = 1000 kgHM. Also, I expect he used SI or MKS for other numbers, e.g., density in kg/m3. In one's equation, one uses density in (kg/cm^3). I would recommend caution in mixing units.

Frapcon uses a conversion factor of 3.8e-16 with burnup given in terms of MWd/t, and density of the fuel is in terms of kgHMO2/m3, which is converted to kgHM/m3 by a factor of 0.8815. The FALCON code also uses this approach.
 
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