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32 10 2 29 1 9 26 23 20 16 17 14 13 4 15 3 18 21 12 11 RPP(1) 25 22 RPP(4) 19 6 5 24 27 30 33 NX=5 31 NY=3 NTPIN=6 NDPIN=2 IDIVP=1 TY(1)=90 TY(2)=210 TY(3)=330 7 8 28 θ RX(5) RPP(1)=RPP(2)=RPP(3) THETA(1)=90 THETA(2)=210 THETA(3)=330 RPP(4)=RPP(5)=RPP(6) THETA(4)=30 THETA(5)=150 THETA(6)=270 If IDIVP=1, RPP(i) must not accross the pin rods on RPP(j) different from RPP(i). IGT=12 (Hexagonal assembly with asymmetric pin rods) TY(5) TY(4) TY(3) TY(2) TY(1)=0.0 RDP(1,12)=0.0 RDP(2,12) NX=4 NY=4 Y RDP(3,12) NTPIN=13 NDPIN=3 RDP(4,12) IDIVP=1 (1,5) 47 50 53 4849 13 14 15 16 42 43 5152 45 46 54 55 (1,4) 41 44 40 34 9 10 37 11 12 33 36 39 (1,3) 32 35 38 28 5 6 7 8 27 30 31 (1,2) 26 29 19 1 2 3 4 18 17 2021 22 25 24 23 (IXP,IYP)=(1,1) (2,1) (3,1) (4,1) (5,1) X RX(1)=0.0 RX(2) RX(3) RX(4) RX(5) Sub-Region number for each pin rod is in order of (IXP,IYP). (IXP,IYP)=(1,1), (3,1),(5,1),(2,2),(4,2),(1,3),(3,3),(5,3),(2,4),(4,4),(1,5),(3,5),(5,5) IGT=13 (X-Y 2D cell with pin rods on arbitrary grid points) Fig.2.4-4 Geometries for PIJ (IGT=12, 13) 62
RDP(1)=0.0 RDP(2) RDP(3) 14 13 12 RPP(2) 11 RPP(1)=0.0 1 2 3 4 5 6 7 8 9 10 NX=2 NTPIN=19 NAPIN=3 NDPIN=2 IDIVP=2 NPIN(1)=1 NPIN(2)=6 NPIN(3)=12 RPP(3) RX(3) RX(2) IGT=14 (Concentric layers of hexagons with equi-distant pin rod arrays) TY(Relative Length) NX=7 TY(5)=1.0 NY=4 NTPIN=91 NAPIN=5 NDPIN=2 IYP=5 33 29 TY(4) 25 65 IYP=4 64 24 28 32 TY(3) 16 61 23 63 IYP=3 60 62 15 22 9 55 14 57 21 59 31 TY(2) IYP=2 54 56 58 8 13 20 27 4 47 7 49 12 51 19 53 IYP=1 46 48 50 52 3 6 11 18 30 26 34 35 1 37 2 5 10 17 38 39 41 43 45 36 40 42 44 (IXP,IYP)=(0,0) 60°Rotational B.C. IXP=1 IXP=2 IXP=3 IXP=4 IXP=5 TY(1)=0.0 X RX(1)=0.0 RX(1) RX(2) RX(3) RX(4) RX(5) RX(6)RX(7) RX(cm) (IXP,IYP)=(0,0),(1,0),(2,0),(3,0),(4,0),(5,0),(2,1),(3,1),(4,1),(5,1),(3,2),(4,2),(5,2),(4,3),(5,3),(5,4), (1,1),(1,1),...............(1,1) : dummy input (automaticaly set in symmetric position) IGT=15 (Hexagonal assembly with triangular pin rod arrangement) Fig.2.4-5 Geometries for PIJ (IGT=14, 15) 63
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JAEA-Data/Code 2007-004 SRAC2006 :
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Contents 1. General Descriptions ..
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5.5 BWR Fuel Assembly Calculation (
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目次 1. 概要 ................
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5.4 三次元拡散計算 (CI
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1. General Descriptions 1.1 Functio
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essential programs of the integrate
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Sphere (Pebble, HTGR) 1D-Plate (JRR
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ecause the scattering cross-section
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As shown in Fig.1.4-1, one PDS file
Page 23 and 24: 1.5.1 Fast Fission Energy Range (10
Page 25 and 26: i n m≠n i n i n i n i 1 i i g( C
Page 27 and 28: mixture(s) having resonant nuclides
Page 29 and 30: thermal energy range. In the fixed
Page 31 and 32: 1.10 Calculation Scheme In Fig.1.10
Page 33 and 34: 3 2 1 CALL MICREF [20] CALL REACT C
Page 35 and 36: homogenized P 1 spectrum obtained a
Page 37 and 38: Consequently next step ’CALL MACR
Page 39 and 40: 1.11 Output Information Major calcu
Page 41 and 42: (4) A floating number may be entere
Page 43 and 44: 2.2 General Control and Energy Stru
Page 45 and 46: cell. = 2 The PEACO routine (hyperf
Page 47 and 48: should be avoided for the core wher
Page 49 and 50: Note: Usually IC15=1 is used in FBR
Page 51 and 52: Behrens’ term of the Benoist mode
Page 53 and 54: Only the first character (capital l
Page 55 and 56: NET ∑ i= 1 NEGT( i ) =(Total numb
Page 57 and 58: Block-1 Control integers /18/ 1 IGT
Page 59 and 60: asymmetric cell is surrounded by en
Page 61 and 62: = 0 Isotropic (white) reflection =
Page 63 and 64: degree for the numerical angular in
Page 65 and 66: 3 EPSG Extrapolation criterion 4 R
Page 67 and 68: Block-10’ Required if IGT=11, or
Page 69 and 70: = 2 Neutron from moderator = 3 Neut
Page 71 and 72: Unit Cell Periodic B.C. 4 2 3 1 RX(
Page 73: NX=4 NTPIN=6 NAPIN=1 NPIN(1)=6 6 ID
Page 77 and 78: 2.5 ANISN ; One-dimensional S N Tra
Page 79 and 80: 7 IBR Right boundary condition, sam
Page 81 and 82: 22 IPM Angular dependent incident s
Page 83 and 84: EV = best guess for α or 0.0 when
Page 85 and 86: Block-04* Positions of interval bou
Page 87 and 88: 2.6 TWOTRAN ; Two-dimensional S N T
Page 89 and 90: Note: The original TWOTRAN uses two
Page 91 and 92: = 0 (internally set) 19 IHM Total n
Page 93 and 94: = 3 R-θ 31 IEDOPT Edit options. =
Page 95 and 96: = 1 Yes Block-4 Control floating po
Page 97 and 98: Repeat Block-20 through Block-21, N
Page 99 and 100: 2.7 TUD ; One-dimensional Diffusion
Page 101 and 102: = 1 Monitor print at each inner ite
Page 103 and 104: equation is applied to meshes, the
Page 105 and 106: Pin Plate D2 D2 D1 D1 In cylindrica
Page 107 and 108: XYZ(1,2) Y-abscissa of the top side
Page 109 and 110: READ(9) (WORK(J+I),I=1,NDATA) END D
Page 111 and 112: absorption cross-section, each of w
Page 113 and 114: ITMX19 The upper limit of CPU time
Page 115 and 116: corner and there are the same numbe
Page 117 and 118: NUAC19 Override use of Chebychev po
Page 119 and 120: NUAC17 > 0 The constant for all gro
Page 121 and 122: ottom starting with a new card. For
Page 123 and 124: Card-006-3 Specification of meshes
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4 SIG3 Absorption cross-section (
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2 NFX2 Optional print control = 0 N
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Region 1 Region 2 Left Right X/R/R
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X T 22*11 Meshes 1 Mesh = 1 Region
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2.9 Material Specification ’Mater
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fuel pin: MU08F0U2 and those in MOX
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hydrogen, add character ‘0’ to
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Usually, enter IRES=2 for the heavy
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2.10 Reaction Rate Calculation The
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Block-1 Control integers for reacti
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3 U238 The position of the second n
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2.11 Cell Burn-up Calculation The i
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= 2 Information for debugging = 3 D
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chains under consideration is enlar
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MACROWRK file. 2 INTSTP Step number
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Block-8-1 Required if IBC6=1 /1/ NM
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e avoided. Because U08W and U080 ar
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2.12 PEACO ; The hyperfine Group Re
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3. I/O FILES We shall describe the
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(E(g),g=1,NGF+1) structure. Boundar
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LTH(1) = (LD(1)+1)*LA(1), ordered a
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Background cross-sections Member Yz
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INT(2) = 0 K-member only without sc
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Member name Contents **************
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(WEIGHT(g),g=1,NGF) Lethargy widths
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3.1.5 Fine Group Macroscopic Cross-
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Member mmmmebfM or caseebxM /10*ng+
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Member caseBNUP Material-wise burn-
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Initial inventory in the restart ca
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(YDIOX(j),j=1,NOWSTP) Fission yield
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(n/cm 2 /sec*cm 3 ), NRR is number
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3.2.1 Common PS Files The following
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3.2.5 PS files for TUD The PS files
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at the first column. Block-1-1 Numb
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= ‘DAYS’ days = ‘YEARS’ yea
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GD156 XGD60001 641560 154.660 0 0 0
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: ZZ050 1.50080E+00 *FP-Yield-Data
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Kr83 Zr95 fission β + decay, EC (n
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Ge73 Ge74 As75 Ge76 fission β + de
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4. Job Control Statements In this c
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~SRAC/tool/lmmake/lmmk/lmmk.sh, whi
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5. Sample Input Several typical exa
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613.0 650.0 760.0 769.0 & cooling 7
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5 5 5 5 5 5 & 5 5 5 5 5 5 & 1 2 3 4
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5.3 S N Transport Calculation (PIJ,
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XFEN0001 2 0 5.78720E-02 XNIN0001 2
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Water reflector Extrapolated B.C. B
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1 1 1 1 1 1 1 2 3 008 -2 1 1 999 /
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Note: This sample is time consuming
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XCRN0008 0 0 1.55546E-02 XNIN0008 0
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****** Input for material specifica
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T-Region R-Region X-Region Reflecti
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6. Utility for PDS File Management
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To read in the microscopic cross-se
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7. Mathematical Formulations 7.1 Fo
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scattering kernel at point r’ fro
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The integration by R between R j- a
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G j Pij ( lattice) = Pij ( isolated
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We, however, should take care of th
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2 = ρ 2 + x r sin β = ρ R = x
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1 i ∑ − 1 k = j+ 1 λ ij = λ k
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where λ λ 1 is 2 is = = N ∑ k k
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2π ri −1 Pij = − Σ ∫ ρdρ
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In Fig.7.1-5, the line PQ’ define
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pin rod are divided into four regio
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the arrays T and II, respectively.
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Note that among four terms appearin
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If a group-dependent form of Fick
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7.3 Optional Processes for Resonanc
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7.3.2 Table-look-up Method of f-tab
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has been introduced for the correct
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ϕ i ( 0 u ) = ∑ Pij ( u) W j ( u
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Geometry b i m f b f −( γ + γ )
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will be seen in the reference 65) .
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The lattice cell under study may co
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(2) Two resonance-absorbing composi
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One of the physical problems associ
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and V = V + V , F f m where Σ m ,
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We shall discuss the following two
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where X = 2R p ( Σ C = 2R πρ R p
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• the reduced collision probabili
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The root mean square (RMS) residual
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group flux and for the fast group f
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Table 7.5-1 (1/2) Nomenclature Symb
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7.5.1 Smearing Smearing or spatial
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7.5.2 Spectrum for Collapsing The f
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Here, an equivalent relation holds
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1 F = K ∑∫ g * χ g ( r) ϕ g (
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M dN i ( t) M = ∑ f j→iλ j N i
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8. Tables on Cross-Section Library
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Table 8.1-2 (2/2) Element index (zz
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JEFF-3.0 are based on other nuclear
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Table 8.2-1 (1/8) List of SRAC publ
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Page 313 and 314:
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8.3 Energy Group Structure The ener
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(4) Upper Boundary of PEACO Routine
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References 1) K. Tsuchihashi, H. Ta
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Experiment,” J. Nucl. Sci. Techno
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75) K. Tasaka : “DCHAIN: Code for
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