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MARS Simulation

MARS Simulation. Tweaking the material (Dose vs. Shield Composition) Next steps. Tom Diehl 03/10/2004. Tweaking the Material I. Change the material that makes up the shield (thickness = 2 cm). Lower Z is a little better than higher Z. More weak evidence for “more shield is more bad”.

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MARS Simulation

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  1. MARS Simulation • Tweaking the material (Dose vs. Shield Composition) • Next steps Tom Diehl 03/10/2004

  2. Tweaking the Material I • Change the material that makes up the shield (thickness = 2 cm). • Lower Z is a little better than higher Z. More weak evidence for “more shield is more bad”. • Carbon fiber mix was a little better than everything else that I tried.

  3. Tweaking the Material II • Changed the material but kept the shield mass at 25 kg. • Possibly lower Z is a little better.

  4. Summary • Shield Composition Studies • At constant thickness, lower Z (lower density) is a little better (less energy in silicon). Weak supporting evidence that “more shield is worse”. • At constant mass, lower Z looks a little better. • Next • I need to talk to NVM to understand details of the output. • Study Solar Protons and galactic electrons.

  5. MARS Simulation Progress • Tweaking the geometry • Dose vs. Shield thickness • Dose w/ vs. w/o a satellite • Next steps Tom Diehl 01/21/2004

  6. Recent History • Igor Rakhno & Co. wrote • Preliminary Results from MARS Calculations: FNAL Technical Memo 2221 Mokhov, Rakhno, Striganov, Peterson “Radiation Load to the SNAP CCD” 09/15/03. • Modeling the Cosmic Rays • SNAP Satellite Model • Preliminary Dose Calculations • We know we have some things to improve. • We know we have some systematic tests to carry out. • Igor sent me his code.

  7. Shielding and Detector Model (Rakhno)

  8. The Rakhno Model • The total mass included amounts to 276 kg. • Shield is 2 cm thick, 35 to 41 kg aluminum. • Cold Plate is 99 kg moly. • Silicon substrate is 5 kg mixture. • Silicon itself is 200 m thick amounting to 107 g. • Radiator is 69 kg aluminum. • The rest is deck, optical bench, supports, etc … amounting to 61 kg. • I modified the cold plate to 49 kg, close to the nominal design.I did this by halving the density of the molybdenum.

  9. Progress Dec. 10th to Dec 31st. • I learned MARS 14 tricks, pictures, plots. • Reran Igor’s code • Same Orbit (solar minimum) 10M galactic protons => 6.8 R/y. Igor had 7.9 R/y. • Same orbit (solar minimum) 100M trapped protons => 34 kR/y. Igor had 21 kR/y. • The program is functioning properly when I run it. Well … I get approx. the same results as Igor does using that geometry.

  10. Dose vs. Shield Thickness (AL) • The shield in the nominal geometry is 2 cm thick aluminum cone. Is there an optimal thickness? • Test dose in the silicon as change thickness (AL density) of the shield. • A much thicker shield will block these protons effectively. • No apparent reason to make the shield 35 kg. 2.7 g/cc

  11. Material vs. No Material • Jodi L. has a fast cosmic ray simulation using 4 charged particles/cm^2/s. That’s the textbook “unprotected” rate.I can calculate a scale factor that accounts for the material. • I set all the material to vacuum, except the silicon, and reran MARS, 10 M galactic protons & 10M galactic electrons, elliptical orbit. • Dose (silicon) = 4.7 R/y, less than with the material around the detector. • Ratio (satellite vs. no satellite) = 1.5 +- 0.1 from galactic protons. • R = 2.0+- 0.2 from galactic electrons. But the electrons are ~100 x less than the protons, anyway.

  12. More Progress since Dec. 10th • “Nibble File” (Cease, Page, Lanfranco) • Solidworks Model -> IDEAS CAD Program • Step through the satellite volume in small cubes • Report the material in each cube, it’s position, density, name, mass, and volume. • I can turn this into a table suitable for MARS. Maybe it will be suitable for GEANT, as well.

  13. Summary & Immediate Plan • Change to L2 Orbit. • The galactic spectrum will be similar to the elliptical orbit spectrum. • Trapped radiation goes away • Verify the shield thickness calculation • Test some different materials • Dose vs. Z at constant mass • Polyethylene & Lithiated polyethylene (may not be wise to use poly, but want to check that anyway) • 2 material sandwich • Start importing simple “nibbled” Solidworks parts.

  14. Buffer slide • Stuff here on isn’t part of this talk.

  15. Shielding and Detector Model (1) • The trick with MARS is to select the appropriate level of detail. • Include the most important shielding components. Consideration is given to proximity to detector and components mass. • Put a lot of effort into detailing the detector.

  16. Microsoft Project Stuff Done = x • I sketched this up ~ Nov. 2003 @ Collaboration Meeting. • I only show details for MARS stuff. • I rolled up the rest. • This isn’t up to code • & it could already stand to be updated. x x x 12/30/2003

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