I am modeling depletion of VVER-440 fuel assembly using CoupledOperator and CECMIntegrator and want to compare the results of the OpenMC simulation with a similar SCALE6.2.4t-6 depl sequence results. However, there is a noticeable discrepancy in the k_{eff} - Burnupdepth results:
It looks like the OpenMC graph is squeezed horizontally by a factor of 10 compared to the SCALE’s one. I also fond a peak typical for that fuel composition and assembly profile between 10 and 20 MWd/kgU and the similar peak on OpenMC graph is about 1 and 2 MWd/kgU.
Could you please check the chunk of OpenMC code and hint me what am I doing wrong?
Hi imelnyk,
Since you use the burnup MWD/kg as x axis, I think there must be something in the composition. If you have made sure the geometry, power density, timestep and accumulation time was identic berween each code, you might want to compare the fuel and burnable poison BP composition calculated by each code during depletion. You can use time as x axis when comparing both results.
Also, you might want to check that the depleteable parameter on the material was set as True, either for the fuel or BP, and each should have a proper volume so that the initial isotope mass between each code was the same. The power density will be multiplied by the heavy metal mass, so you could also do a sensitivity analysis by directly supplying the fuel assembly power to the openmc.
Hi @doriangaboo,
Thanks for your answer! However, I’m not sure that the time steps are supposed to be cumulative, since the opposite is literally specified in the lecture on depletion:
Thanks for your advises! I double check the material and couldn’t find anything suspicious for the moment. I set the material for fuel pins with BA mixing UO2 and Gd materials. I thought that I any material contain Uranium it should be implicitly treated as a depletable, but probably it does not work for Gd. So, I set the Gd mat. to be depletable explicitly and start the calculations. I will see the results later …
Okay, you can also compare the decrease in fissile and BP isotope materials vs time or burnup between each code to find some clue, because I think the decrease in reactivity should have come from those isotopes; either your fissile atomic density decreases faster in openmc, or the BP is not depleted, suppressing the reactivity without even burning it.
Reading back what I said I definitely wrote that poorly, my apologies. I was trying to communicate what they state there, how a burn up calculations with 6 time steps of 30 days, would be defined like [30,30,30,30,30,30] instead of [30, 60, 90, 120, 150, 180]
Unfortunately I can’t speak to whether that could be the cause, I’m not familiar enough with burnup mechanics, but hopefully you get it! Best of luck
Regarding “a burn up calculations with 6 time steps of 30 days”, it would be [30,30,30,30,30,30] or [30] * 6. you can also check the depletion notebook from openmc.
But as long as that plot of you use the pregenerated time you are getting from openmc depletion result, i.e. deptime, kinf = depletion_results.get_keff(time_units='d') or deptime, atom_U235 = depletion_results.get_atoms(mat=fuel, nuc='U235', nuc_units='atom/b-cm', time_units='d'), then the depletion time was a cumulative time, not the time step.
I’m sorry for the late reply since I slightly suspended these studies. Recently, I re-ran the simulation with explicitly specified depletable property for UO2 + Gd2O3 material and got the following graph for e.g. ^{157}Gd nuclei number density:
It looks like that for BP/BA fuel type (the blue line) gadolinium-157 burns up almost immediately, might it suggest that something is wrong with depletion rate? This drop in the Gd number density suspiciously matches with that small peak you might’ve seen on the K_{eff} vs. burn-up depth graph which appears to be the same as for the previous runs (w/o depletable property).
Cheers,
Ihor
P.S.
Giving the shape and numerical ranges of the two curves below:
Since you already mentioned the power density, I see that you use the power density in your integrator, power_mass_density = 35. # W/gU as power density.
So, just to make sure, have you declared the depleted material volume in your input? You can check the initial heavy metal mass with get_mass from your fuel material definition. From the depletion manual, “openmc will multiply the power density by initial heavy metal inventory to get the total power if power is not specified”. openmc.deplete.CECMIntegrator — OpenMC Documentation
I havent use the power_density parameter in the integrator since most of the time, I am declaring the total heavy metal volume in my model and applied specific power for this volume of HM, so I have no experience with this kind of power density input.
A typical VVER-440 fuel assembly consists of 126 fuel pins and one central tube. In the current problem 4 types of fuel (depending on uranium enrichment and presence/absence of BA) are considered: only one type among these 4 has Gd. So, therefore the FA contains 4 different types of fuel rods (pins). A typical pin is represented as a cylinder with another hollow cylinder centered inside the outer one (actually filled with helium). The FA configuration of interest has 6 pins with BA, 30 pins filled with fuel_type1, 6 with fuel_type2 and rest are fuel_type3 filled.