Lecture 3: K-effective  Material specification  K-effective calculations  Beam sources  Collecting particles by energy  Collection particle by direction.

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Presentation transcript:

Lecture 3: K-effective  Material specification  K-effective calculations  Beam sources  Collecting particles by energy  Collection particle by direction

Photon coefficients

3 Material Description: Mm Card  Materials are described by (isotope,density) pairs  Isotope—specified by ZZAAA 1001  H  H  O  O  U  U-235  If AAA is 000, specifies the natural isotopic mix for an element  natural lead  natural lead 8000  natural oxygen 8000  natural oxygen  Density—Relative number (+) or mass (-) for each isotope  Example: Water M M OR OR M M

4 Case 2: Lead sphere Simple point source in lead ; Tally = surface crossing c ********************************************************************* c * c Cells * c * c ********************************************************************* imp:p= imp:p=0 c ********************************************************************* c * c Surfaces * c * c ********************************************************************* 1 sph c ********************************************************************* c * c Data cards * c * c ********************************************************************* mode p sdef par 2 pos erg 2 m f1:p 1 nps Result: /- 3.31%

5 Criticality card: KCODE Syntax: Description: Criticality equivalent of SDEF card. Sets up number of cycles, number of histories per cycle, number of cycles to skip, etc. NSRCK=#histories per cycle RKK=initial keff guess IKZ=#cycles to skip KCT=#cycles to be done MCNP5 Manual Page: 3-75

6 Initial source card: KSRC Syntax: Description: Source locations for initial cycle of criticality calculations. [You can ALSO use the regular SDEF card.] MCNP5 Manual Page: 3-76

7 HW 3.1  Use MCNP to find the critical radius of a solid sphere of uranium 235  Repeat with one inch of water outside the uranium (Consider k-effective of to be critical. Run 310 histories of 1000 neutron each, skipping the first 10.)

8 Beam sources SDEF variables used:  POS=Position of the source center  VEC=Vector of direction of the beam  DIR=Direction cosine vs. VEC Example: 1.5 MeV beam of neutrons travelling up from point (1,2,3): SDEF par 1 erg 1.5 pos vec dir 1

9 HW 3.2  Use MCNP with a beam source and a small cylindrical sample to estimate the total and scattering cross section for a 10 MeV neutron impinging on lead  Find the energy distribution of scattered neutrons  Repeat for 1 keV and 1 eV