ML20082R685

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Forwards Neutron Transport Calculations Supporting Proposed Renewal of License,In Response to Committee to Bridge the Gap 831118 Request.Related Correspondence
ML20082R685
Person / Time
Site: 05000142
Issue date: 12/07/1983
From: Cormier W
CALIFORNIA, UNIV. OF, LOS ANGELES, CA
To: Bright G, Frye J, Luebke E
Atomic Safety and Licensing Board Panel
References
NUDOCS 8312130263
Download: ML20082R685 (47)
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73 UNIVERSITY OF CALIFORNIA, LOS ANGELES

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DEC 12 All:33 OFFICE OF Tile CilANCELLOR LOS ANCELES, dMillf 0E sE 9652S R t. IA t1 00CKEilNG & SEf<VICL December 7, 1983 BRANCH John H. Frye, III, Chairman Dr. Emmeth A. Luebke Administrative Judge Administrative Judge Atomic Safety and Licensing Bd.

Atomic Safety and Licensing Bd.

U.S. Nuclear Regulatory Comm.

U.S. Nuclear Regulatory Comm.

Washington, D.C.

20555 Washington, D.C.

20555 Glenn 0. Bright Administrative Judge Atomic Safety and Licensing Board U.S. Nuclear Regulatory Commission Washington, D.C. 20555 In the Matter of THE REGENTS OF THE UNIVERSITY OF CALIFORNIA (UCLA Research Reactor)

Docket No. 50-142 (Proposed Renewal of Facility License)

'le : Neutron Transport Calculations Requested by CBG

Dear Administrative Judges:

l Enclosed are the raw data underlying the neutron transpurt calculations of Mr. Ostrander which were described in connection with the Wigner energy calculation in University's rebuttal testimony. This material was requested by CBG in Mr. Hirsch's letter of November 18, 1983.

Also enclosed is Mr. Ostrander's "Correctio6" to those calcu-f lations. The relevant effect of the correction is to change the reported a

MA result of the " Monte Carlo" calculation of the percentage of fission Oo' neutron energy deposited in the graphite (and fuel region) from 15% (and 58 85%) to 19% (and 81%). A separate correction is made to the uncollided l

og flux calculation which changes the reported result from 85% to 71%; howev-

[

n er, this calculation does not directly enter any of the analyses nor is it M

relied upon by any of University's witnesses.

(In this regard, I note that l

00 I inadvertently over-stated the significance of these corrections on page l

30 18 of " University's Response to CBG's Objections to Rebuttal Testimony",

i dated December 2, 1983: the only significant changes are the caange in the gh reported percentage of fission neutron energy absorbed in the water, which is noted at several places in University's rebuttal testimony, from 85% to 81'L; and the change from 15% to 19% for the percentage of fission neutron energy deposited in the graphite which enters into the last step of the Wigner energy calculation.)

f Administrative Judges 2

4 December 7,1983 We had intended to respond to CBG's request by reproducing the computer code listing and data for the Monte Carlo calculation with further explanations in a more presentable form, but because of CBG's insistence that the calculations be presented now, we have abandoned that time-consuming effort.

Very truly yours, DL4"".

William H. Cormier Enclosures cc: Service List i

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ei RAHAEEllpN IQ THE DISTRIBUTION OF FISSION NEUTRON ErlERGY DEPOSITION BETWEEN FUEL REGIONS AND GRAPHITE IN AN ARGONAUT RESEARCH REACTOR BY N.C. OSTRANDER Two calculations were performed to determine the percentage of fission neutron energy deposited in the fuel region and graphite of an Argonaut research reactor. The first calculation was based on a model of the "uncollided flux" which reached the graphite. The second calculation utilized a detailed " Monte Carlo" method which traced the paths and energy deposition of individual neutrons. As previously reported, the Monte Carlo calculation yielded the result that approximately 85% of the fission i

neutron energy was deposited in the fuel region and only 15% was deposited in the graphite. This result was stated to be consistent with the result obtained based on the "uncollided flux" model calculation. Two corrections are to be noted.

l l

The Uncollided Flux Calculation f

The model of the uncollided flux used and previously reported yields the fraction of the fission neutrons which reach the center graphite

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island at high energy. That fraction is approximately 15%. However, an approximately equal fraction reaches the graphite reflector opposite the.

center island. As a result, the total fraction of fission neutrons which reach the graphite at high energy is approximately 29%. As previously reported, the result failed to properly account for the " mirror image" symmetry of the calculational model.

The Monte Carlo Calculation The Monte Carlo calculation is not affected by the correction made in the uncollided flux calculation. However, verification of the calculation disclosed that of the population of 45 neutrons whose paths were traced, only 19 of the neutrons initially started in.the direction of i

the graphite while 24 of the neutrons moved toward the interior of the fuel box. The initial directions of two of the neutrons could not be ascer-tained. Although the initial directions were determined by means of a l

l random number sub-routine in the program, the selection produced an obvious bias in the procedure which could have affected the results.

In order to remove the bias, eliminate the two neutrons of l

uncertain initial direction, and to improve the statistics by providing a more uniform sampling of the initial directions, thirteen neutrons of the initial population have been discarded and eighteen new neutron samples l

were run to provide a population of 50 neutrons. Of the discarded

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e neutrons, only three had reached the graphite and that sub-population deposited only 5.7% of its total energy in the graphite.

For the new population of 50 neutrons, the estimate of energy deposition in the graphite is 19%, instead of approximately 15% as previously reported, and, accordingly, 81% of the energy is deposited is the fuel region.

Comoarison of the Two Calculations The Monte Carlo calculation indicates that about 34% of the fast neutrons enter the graphite above 0.8 mev. The corrected unco 111ded flux model suggests 29%. The 34% of the fast neutrons that enter the graphite transport an average energy of 1.88 mey pe'r neutron to the graphite.

However, these neutrons rarely stay in the graphite and much of their energy is ultimately deposited in the fuel box. The Monte Carlo calcu-lation demonstrates that an average net deposition of 0.94 mev per fast neutron (greater than 0.8 mev) occurs in the graphite.

In othcr words, the uncollided flux does not deposit the entirety of its energy in the graphite, but more nearly 50% of its energy. The other source of energy deposited in the graphite is due to a small fraction (approximately 10%) of the population that occasionally migrate into the graphite but at much lower average energy levels.

l Thus, there is a relationship between the uncollided flux and the energy deposition in graphite, but it cannot be interpreted without more s

4-i precise.information concerning the energy deposition due to the flux and f

the lower energy neutrons which are responsible for a small contribution to the total energy deposited in the graphite.

These factors cannot be accounted for the calculation based on the uncollided flux model, but they

- are accounted for}in the Monte Carlo calculation.

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