CCC-0082 ANISN. (Abstract last modified 04-APR-2003)
1.
NAME OR DESIGNATION OF PROGRAM - ANISN. 2.
COMPUTER FOR WHICH PROGRAM IS DESIGNED AND OTHER MACHINE VERSION PACKAGES AVAILABLE -
To request or retrieve programs click on the one of the active versions below.
A password and special authorization is required. Explanation of the status codes.
Machines used:
Package-ID Orig.Computer Test Computer
CCC-0082/08 IBM 370 series IBM 370 series
3.
NATURE OF PHYSICAL PROBLEM SOLVED - The ANISN system treats neutron and gamma transport in one- dimensional plane, spherical and cylinder geometry. The multigroup cross sections prepared by the programs LIANE and SUPERTOG are processed by the program RETTOG, which produces a binary library with Legendre expansions. The binary library can be updated and edited with the program LGR/B. The photon multigroup cross sections are created with the program GAMLEG/A. If the bulk of the data is too large, the program TAPEMA produces a special group-by-group library. The volume sources are calculated from a reduced set of input data and punched in a format suitable for input to ANISN, using the program PRESOU. 4.
METHOD OF SOLUTION - ANISN solves the one-dimensional Boltzmann transport equation for neutrons or gamma-rays in slab, sphere, or cylinder geometry. The source may be fixed, fission or a subcritical combination of the two. Criticality search may be performed on any one of several parameters. Cross sections may be weighted using the space and energy dependent flux generated in solving the transport equation. 5.
RESTRICTIONS ON THE COMPLEXITY OF THE PROBLEM - In ANISN, the complexity of the problem is limited by storage size. 6.
TYPICAL RUNNING TIME - 7.
UNUSUAL FEATURES OF THE PROGRAM - 8.
RELATED AND AUXILIARY PROGRAMS - ANISN Library generators. 9.
STATUS 10.
REFERENCES - 11.
MACHINE REQUIREMENTS - 12.
PROGRAMMING LANGUAGE(S) USED - 13.
OPERATING SYSTEM OR MONITOR UNDER WHICH PROGRAM IS EXECUTED - 14.
ANY OTHER PROGRAMMING OR OPERATING INFORMATION OR RESTRICTIONS - ANISN supersedes DTF-II (NAA-SR-10951, March 25, 1966) which followed a series of developmental efforts over a period of years. 15.
NAME AND ESTABLISHMENT OF AUTHOR - 16.
MATERIAL AVAILABLE - 17.
CATEGORIES - Keywords: ABSORPTION, ANISOTROPIC SCATTERING, BUCKLING, CROSS SECTIONS, CYLINDERS, DISCRETE ORDINATE METHOD, FISSION, GAMMA RADIATION, NEUTRON TRANSPORT THEORY, ONE-DIMENSIONAL, SHIELDING, SLABS, SPHERES, TRANSPORT THEORY
Program-name Package-ID Status
ANISN-F CCC-0082/01 Obsolete
ANISN-JR CCC-0082/02 Obsolete
ANISN CCC-0082/04 Obsolete
ANISN CCC-0082/05 Obsolete
ANISN CCC-0082/06 Obsolete
ANISN-C CCC-0082/07 Obsolete
ANISN-E CCC-0082/08 Tested
ANISN-E CCC-0082/09 Obsolete
ANISN CCC-0082/10 Obsolete
ANISN CCC-0082/11 Obsolete
ANISN CCC-0082/12 Obsolete
ANISN calculates fluxes by groups, space intervals, angle and any number of reaction rates. The energy and space dependent fluxes are stored on tape and can be reprocessed, edited and plotted with the program ANISEX, which also permits to calculate supplementary reaction rates. The program ANISN can condense cross sections into a reduced number of groups. The ANISN system is used as a reference system for the evaluation of approximation methods (space-diffusion or point kernel) or for the preparation of multigroup libraries for two-dimensional transport codes (DOT). In particular it is used for shielding problems with high attenuation in water reactors and fast reactors.
ANISN-E solves the same problems as the original ANISN code. Some modifications concern weighted cross sections output and fixed distributed sources input/output.
ANISN-E (CCC-0082/09): The CYBER 175 version of ANISN-E also contains the free-format input capability.
ANISN-JR extends the applicability of the original ANISN code for shielding analyses by adding options of calculating the reaction rates distributions from detector response, generating the volume- flux weighted cross sections in arbitrary regions or zones and plotting the neutron or gamma-ray spectra and the reaction rates distributions.
ANISN-E : Besides diamond and weighted difference supplementary equations, exponential supplementary equations are available.
The new model:
(1) always gives positive solutions, without using any 'fixup' technique provided that the source is non-negative;
(2) allows, especially in deep penetration problems, the use of larger spatial meshes, hence requires shorter computer times than the ones requested by the diamond model combined with various types of fixup techniques or by weighted difference schemes to get the same accuracy;
(3) supplies solutions that are always reasonable overestimates of the exact solution.
In ANISN-JR, some optional functions are added to increase the utility of the code:
(1) print the total fluxes at boundary points of all mesh intervals. (The original ANISN prints the total fluxes at midpoint only.) (2) calculate, print and plot the lethargy width spectra. (3) print the angular fluxes at only required mesh boundaries or midpoints (maximum 10 points). The original ANISN prints at mid- point of all meshes, and therefore the number of print pages becomes vast according to the number of spatial and angular meshes.
(4) use the asymmetric quadrature set.
(5) calculate and plot the reaction rates for neutron and gamma-ray detectors, and collapse the response functions of detectors.
(6) generate volume-flux weighted cross sections for arbitrary zone or region. In the original ANISN, the cross sections can be collapsed only for a homogeneous zone or region.
(7) collapse into few group cross sections in ANISN, DOT, or TWOTRAN format. (In TWOTRAN format, the l-th Legendre coefficient of the scattering cross section is divided by (2l + 1) and the cross section of (n,2n) reactions is added for use of the coarse-mesh rebalancing technique.)
(8) multiply the average cross section by the density factor, when an option of density factors is used (IDFM=1).
ANISN-E: Exponential equations to compute mesh centre fluxes.
ANISN-JR uses, by input option, either group independent cross section sets produced by the code RADHEAT-V3, or those written in the original ANISN format. In the original ANISN and the present version, the adjoint calculations can not be performed with the group independent cross section tape (ID2=1) but with the tape generated from the step 3 of RADHEAT-V3. The data for the additional options are given before the ANISN original input data. If the reaction rates are required, the response functions of detectors follow after the ANISN data. A utility code of ANISN will be used for plotting the energy spectrum and flux or reaction rate distributions calculated by ANISN-JR.
CCC-0082/01: 08-APR-1982 Obsolete
CCC-0082/02: 06-DEC-1999 Obsolete
CCC-0082/04: 04-APR-1984 Obsolete
CCC-0082/05: 04-APR-1984 Obsolete
CCC-0082/06: 01-AUG-1975 Obsolete
CCC-0082/07: 01-MAY-1974 Obsolete
CCC-0082/08: 01-FEB-1978 Tested at NEADB
CCC-0082/09: 18-JUN-1997 Obsolete
CCC-0082/10: 17-AUG-2001 Obsolete
CCC-0082/11: 04-APR-2003 Obsolete
CCC-0082/12: 04-APR-2003 Obsolete
- R. Douglas O'Dell and Raymond E. Alcouffe:
Transport Calculations for Nuclear Analyses: Theory and Guidelines for Effective Use of Transport Codes
LA-10983-MS and UC-32 (September 1987).
CCC-0082/08:
- W.W. Engle, Jr. :
A Users Manual for ANISN - A One-Dimensional Discrete Ordinates
Transport Code with Anisotropic Scattering
K-1693 (March 1967)
- R.W. Roussin:
Using ANISN to Reduce the DLC-2 100 Group Cross-Section Data to a
Smaller Number of Groups
ORNL-TM-3049 (May 7, 1969)
- W.W. Engle, M.A. Boling and B.W. Colston :
DTF II, A One-Dimensional Multigroup Neutron Transport Program
NAA-SR-10951 (March 1966)
- E. Sartori :
Lecture Notes on the Discrete Ordinates Transport
Codes ANISN & DOT.
"Course on Radiation Shielding Methods" Ispra (Nov. 20-24, 1978)
- P. Barbucci and F. Di Pasquantonio :
Exponential Supplementary Equations for SN Methods:
The One-Dimensional Case.
Reprint from "Nuclear Science and Engineering":
63, pp. 179-187 (1977)
- Enrico Sartori:
Note to all recipients of various versions of ANISN
NDB/93/0931 (27 August, 1993)
CCC-0082/08: FORTRAN-IV
Contributed by: Oak Ridge National Laboratory
Oak Ridge, Tennessee, U.S.A.
ANISN-E : P. Barbucci and F. Di Pasquantonio:
ENEL Centro di Ricerca termica e nucleare
Bastioni di Porta Volta 10
20121 Milan, Italy
ANISN-JR : Japanese Atomic Energy Research Institute
CCC-0082/08:
CCC0082_08.001 SOURCE PROGRAM (F4,EBCDIC) 4178 records
CCC0082_08.002 PROG. TO GENERATE DISTRI. SOURCE(F4,EBCDIC) 16 records
CCC0082_08.003 PROG. TO LIST GAMMA SOURCES (F4,EBCDIC) 9 records
CCC0082_08.004 SAMPLE PROBLEM 1 INPUT DATA 41 records
CCC0082_08.005 SAMPLE PROBLEM 2 INPUT DATA 44 records
CCC0082_08.006 JCL & INFORMATION 64 records
CCC0082_08.007 SAMPLE PROBLEM 1 PRINTED OUTPUT 359 records
CCC0082_08.008 LIST OF DISTRIBUTED SOURCE(SAMPLE PROB. 2) 6 records
CCC0082_08.009 SAMPLE PROBLEM 2 PRINTED OUTPUT 441 records
CCC0082_08.010 LIST OF GAMMA SOURCES 16 records
- C. Static Design Studies
- J. Gamma Heating and Shield Design
Home - About Us - Work Areas - Data Bank - Publications - Press Room - List of acronyms - Search