source specifications in mcnp presented by: f. rahmani shahid beheshti university department of...

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Source Specifications in MCNP Presented by : F. Rahmani Shahid Beheshti University Department of Radiation Application

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Page 1: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Source Specifications in MCNPPresented by:

F. Rahmani

Shahid Beheshti University

Department of Radiation Application

Page 2: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Input to Output Flow Diagram:

Page 3: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Source Commands:

SDEFKCODESSW / SSR

User subroutine

FixedReactorMCNP generated

surface source write your own

There are four possible source types:

Page 4: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Source Commands:

There are four possible source types:

Fixed (or general ) source (SDEF card) MCNP generated surface source (SSW to write and

SSR to read). Criticality Source (KCODE Card); needs also an

initial source (KSRC, SDEF card or SRCTP file from a previous calculation written by the SSW card).

User supplied source (if SDEF, SSR and KCODE are all missing)

Page 5: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

General Cards:

These general cards can be used with any of the above sources:

SI (source information), SP (source probability), SB (source bias), DS (dependent source)

MODE card implied the type of source particle.

Page 6: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

MODE card :

MCNP4c can be run in several different modes:

N — neutron transport only (default) N P — neutron and neutron-induced photon transport P — photon transport only E — electron transport only P E — photon and electron transport N P E — neutron, neutron-induced photon and electron transport

And can be run in similar way with other particles according to it’s version.

Page 7: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Source Specifications:

A particle source has:

Intensity, Energy, Direction, Shape, Temporal characteristics, A position somewhere within the phase space of the problem

We are concerned here with fixed sources, or primary sources; not secondary sources such as those generated by fission, neutron capture, or electron recoil.

The source strength in represented in MCNP by the starting weight, WGT, which is usually assigned to unity to represent a normalized source.

The frequency of occurrence of a particle of a particular attribute is determined by the source’s probability density function (pdf).

Page 8: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

General Source Card (SDEF):

The SDEF command with its many variables is one of the more complex MCNP commands and is capable of producing an incredible variety of sources

The SDEF command has many variables or parameters that are used to define all the characteristics of all sources in the problem

The source and type of radiation particles for an MCNP problem is defined by the SDEF command

Only one SDEF card is allowed in an input file

Page 9: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

SDEF variables:

Page 10: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

SDEF variables:

Page 11: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application
Page 12: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

SDEF variables defaults:

POS = x y z default is 0 0 0;

CEL = starting cell number

ERG = starting energy default is 14 MeV;

TME = time default is 0;

PAR = source particle type 1 for N, N P, N P

E; 2 for P, P E; 3 for E

and other particles

Page 13: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

SDEF variables:

Values of variables can be specified at three levels:

(1) explicitly (e.g., ERG=1.25), (2) with a distribution number (e.g., ERG=d5), (3) as a function of another variable (e.g., ERG=Fpos).

Specify variables at levels 2 and 3 requires the use of four other source cards: SI (source information), SP (source probability), SB (source bias), DS (dependent source)

Page 14: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Sdef par=2 erg=1.25 dir=1 vec=1 0 0 pos=0 0 0

Sdef pos=10 -2 0

Page 15: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Important Point

When developing a new source definition, always check and

recheck that source particles are truly being generated where

you think they should be.

HINT: Always use the VOID card and the PRINT 110 statement somewhere in data block of the input file. The PRINT 110 causes the starting locations.

directions, and energies of the first 50 particles to be printed

to the output file. Examine this output table to convince

yourself that particles are being generated as you expect.

Page 16: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Spatial Distribution (Shape):

Volume Sources :SUR=0 (default value). Cartesian (These ace specified with X, Y, and Z.)

Point: X, Y and Z are all constant. Line: one variable, the others are constant, Rectangular Plane: Fix one variable and vary the other two. Rectangular Polyhedron: vary the three variables.

In general, use SUR for a surface source and CELL for a volume source.

Page 17: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Spatial Distribution (Shape):

Spherical (These are specified by POS (center of sphere)

and RAD (radius), do not specify XYZ and AXS.) Point: RAD=0, or not specified at all. Spherical shell: specify two radii for RAD on an SIn card.

Cylindrical (These are specified with POS (point on axis),

AXS (direction cosines of axis), RAD (radius of

cylinder), and EXT (distance form POS). Disk :set EXT=0, which provides a source with circular symmetry on a

plane.

Page 18: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Energy Spectrum:

ERG= starting energy (default 14 MeV):Use an SP card to define a distribution from Built-In

Functions for Source Probability and Bias Specification

Page 19: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application
Page 20: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application
Page 21: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Directional distribution:

The default is isotropic distribution. VEC defines a reference vector (which can be itself a

distribution); the default for a surface source is the normal to the source in a

direction defined by NRM. DIR defines the cosine of the polar angle;cosine distribution for a surface source is the default. The azimuthal angle is sampled uniformly. DIR=l gives a mono-directional source (beam) in

the ,direction of VEC.DIR can be biased to a preferred direction,

Page 22: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Temporal distribution:

TME = time (in units of shakes, default=O). SP with f=-1 defines a Gaussian distribution with time.

Alternatively, DS can be used to define a discrete distribution.

Page 23: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Others:

See manual for :Repeated source structure (use CEL with a path

from level 0 to level n).Surface source write (SSW card).Surface source read (SSR card)Criticality source (KCODE and KSRC cards).User supplied source (Subroutines SOURCE and

SRCDX).

Page 24: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Examples:

Point Isotropic Sources: Two Point Isotropic Sources at Different PositionsSDEF ERG=1.00 PAR=2 POS=d5SI5 L -10 0 0 10 0 0 $ SP5 .75 .25 Point Isotropic Source with Discrete Energy PhotonsSDEF POS 0 0 0 ERG=d1 PAR=2SI1 L 0.3 0.5 1 2.5 $ the 4 discrete energies (MeV)SP1 0.2 0.1 0.3 0.4 $ frequency of each energy

Page 25: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

Work Problems:

Write the SDEF card, and associated cards, explaining each instruction, for: An inward directed source cm spherical surface. A monodirectional source emitted from a surface in the

direction of the direction positive to the surface. A point source in which the low-energy particles are

emitted with a cosine distribution,Criticality source (KCODE and KSRC

cards).

Page 26: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application
Page 27: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

SDEF SUR=12 RAD=D2 nrm=-1 ERG=d1 POS=0 15.275 0 SI1 0.1 29i 3 SP1 0 1 30r SI2 0 .5 SP2 0 1

Page 28: Source Specifications in MCNP Presented by: F. Rahmani Shahid Beheshti University Department of Radiation Application

sdef pos=0 0 0 vec=0 1 0 DIR=D1 ERG=FDIR D2 par=2 SI1 -1 -.9 -.8 -.7 -.6 -.5 -.4 -.3 -.2 -.1 0 & .1 .2 .3 .4 .5 .6 .7 .8 .9 1 Sp1 0 2.66E-02 2.66E-02 2.66E-02 2.60E-02 2.56E-02 2.45E-02 2.33E-02 2.12E-02 1.77E-02 1.03E-02 5.22E-03 6.03E-03 7.90E-03 1.14E-02 1.52E-02 1.91E-02 2.41E-02 2.96E-02 3.82E-02 5.89E-02 DS2 s 4 5 6 7 c Sc4 cosine=-1 to -0.9 SI4 0 1 2i 4 Sp4 0 2.38E-02 2.37E-03 4.04E-04 1.80E-05 sb4 0 1 3r Sc5 cosine=-0.9 to -0.8 SI5 0 1 2i 4 SP5 0 2.38E-02 2.36E-03 4.39E-04 2.70E-05 Sb5 0 1 3r Sc6 cosine=-0.8 to -0.7 SI6 0 1 2i 4 SP6 0 2.35E-02 2.66E-03 4.75E-04 3.30E-05 Sb6 0 1 3r Sc7 cosine=-0.7 to -0.6 SI7 0 1 2i 4 SP7 0 2.26E-022.89E-03 5.12E-04 4.60E-05 Sb7 0 1 3r