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Summary of Aarhus workshop

Summary of Aarhus workshop. Some selected results. Intrinsic numerical accuracy. Compare models computed with a given code and given parameters Vary number of meshpoints Vary number of timesteps. Case 1.1 0.9 M ¯ , X c = 0.35. ASTEC. 3 He in equilibrium.

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Summary of Aarhus workshop

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  1. Summary of Aarhus workshop Some selected results

  2. Intrinsic numerical accuracy • Compare models computed with a given code and given parameters • Vary number of meshpoints • Vary number of timesteps

  3. Case 1.1 0.9 M¯, Xc = 0.35 ASTEC 3He in equilibrium Test effect of no. of meshpoints: ( N = 1200) – (N = 600)

  4. Case 1.1 0.9 M¯, Xc = 0.35 ASTEC 3He in equilibrium Test effect of no. timesteps: ( Nt = 24) – (Nt = 13) (D ymax = 0.025) - (D ymax = 0.05)

  5. Case 1.3 1.2 M¯, Mc = 0.1 M¯ ASTEC 3He in equilibrium Test effect of no. of meshpoints: ( N = 600) – (N = 1200)

  6. Case 1.3 1.2 M¯, Mc = 0.1 M¯ ASTEC 3He in equilibrium Test effect of no. of meshpoints: ( N = 600) – (N = 1200)

  7. Case 1.3 1.2 M¯, Mc = 0.1 M¯ ASTEC 3He in equilibrium Test effect of no. timesteps: ( Nt = 277) – (Nt = 546) (D ymax = 0.05) - (D ymax = 0.025)

  8. Case 1.5 2.0 M¯, Xc = 0.01, Overshoot 0.15 Hp ASTEC 3He in equilibrium Test effect of no. of meshpoints: ( N = 600) – (N = 1200)

  9. Case 1.5 2.0 M¯, Xc = 0.01, Overshoot 0.15 Hp ASTEC 3He in equilibrium Test effect of no. of meshpoints: ( N = 600) – (N = 1200)

  10. Case 1.5 2.0 M¯, Xc = 0.01, Overshoot 0.15 Hp ASTEC 3He in equilibrium Test effect of no. of meshpoints: ( N = 600) – (N = 1200)

  11. Case 1.5 2.0 M¯, Xc = 0.01, Overshoot 0.15 Hp ASTEC 3He in equilibrium Test effect of no. of timesteps: ( Nt = 208) – (Nt = 402)

  12. Case 1.5 2.0 M¯, Xc = 0.01, Overshoot 0.15 Hp ASTEC 3He in equilibrium Test effect of no. of timesteps: ( Nt = 208) – (Nt = 402)

  13. Case 1.5 2.0 M¯, Xc = 0.01, Overshoot 0.15 Hp ASTEC 3He in equilibrium Test effect of no. of timesteps: ( Nt = 208) – (Nt = 402)

  14. Case 1.1 0.9 M¯, Xc = 0.35, TGEC Test effect of no. of timesteps: ( D t = 2000 yr) – (D t = 1800 yr) Continuous: d ln T Dotted: d ln p Dashed: d ln r Dot-dashed: d ln c2 3dot-dashed: d ln G1 Long-dashed: d ln L Thick continuous: d ln X

  15. Case 1.1 0.9 M¯, Xc = 0.35, TGEC Test effect of no. of timesteps: ( D t = 2000 yr) – (D t = 2200 yr) Continuous: d ln T Dotted: d ln p Dashed: d ln r Dot-dashed: d ln c2 3dot-dashed: d ln G1 Long-dashed: d ln L Thick continuous: d ln X

  16. Case 1.1 0.9 M¯, Xc = 0.35, TGEC Test effect of no. of timesteps: ( D t = 2000 yr) – (D t = 2200 yr) Continuous: d ln T Dotted: d ln p Dashed: d ln r Dot-dashed: d ln c2 3dot-dashed: d ln G1 Long-dashed: d ln L Thick continuous: d ln X

  17. Physics comparisons Evaluate physics (EOS, opacity, energy-generation rate, rate of composition change, …, at fixed T, r, Xi Examples: comparing CESAM and CLES with ASTEC, showing, e.g., ln(kASTEC(rCESAM, TCESAM, …)/kCESAM)

  18. CESAM, Case 1.1 Note: consistency problems in OPAL. See also Boothroyd & Sackman (2003; ApJ 583, 1004) In ASTEC implementation: Directly from OPAL: p, rad, d, a, G1 cp = cv + p d2/(r T a)

  19. CESAM, Case 1.1

  20. CESAM, Case 1.1

  21. CESAM, Case 1.1

  22. CLES, Case 1.1

  23. CLES, Case 1.1

  24. CLES, Case 1.1

  25. CLES, Case 1.1

  26. Main project: compare different codes • Evolution tracks • Global parameters for selected models • Detailed comparison of structure • Comparison of oscillation frequencies

  27. CLES and ASTEC Case 1.3 1.2 M¯ X0 = 0.73, Z0 = 0.01 MHeC = 0.1 M¯

  28. CLES and ASTEC Mc/M Case 1.3 1.2 M¯ X0 = 0.73, Z0 = 0.01 MHeC = 0.1 M¯ Xc

  29. CLES, CESAM and ASTEC Case 1.5n 2.0 M¯ X0 = 0.72, Z0 = 0.02 Xc = 0.01 No overshoot

  30. CLES, CESAM and ASTEC Case 1.5n 2.0 M¯ X0 = 0.72, Z0 = 0.02 Xc = 0.01 No overshoot

  31. CLES, CESAM and ASTEC Case 1.5n 2.0 M¯ X0 = 0.72, Z0 = 0.02 Xc = 0.01 Overshoot 0.15 Hp

  32. CLES, CESAM and ASTEC Case 1.5n 2.0 M¯ X0 = 0.72, Z0 = 0.02 Xc = 0.01 Overshoot 0.15 Hp

  33. Detailed model comparison • Global quantities • Differences at fixed m/M, plotted against m/M or r/R • Differences at fixed r/R might be more illustrative for effects on oscillations (but not used yet)

  34. Hydrogen abundance 0.9 M¯ X0 = 0.7 Z0 = 0.02 Xc = 0.35 X

  35. Case 1.1 0.9 M¯, Xc = 0.35 CLES – CESAM2

  36. Case 1.1 0.9 M¯, Xc = 0.35 CLES – CESAM2

  37. Case 1.1 0.9 M¯, Xc = 0.35 CLES – CESAM0

  38. Case 1.1 0.9 M¯, Xc = 0.35 CLES – CESAM0

  39. Case 1.1 0.9 M¯, Xc = 0.35 CESAM2 – CESAM0

  40. Case 1.1 0.9 M¯, Xc = 0.35 ASTEC – CESAM0

  41. Case 1.1 0.9 M¯, Xc = 0.35 ASTEC – CESAM0

  42. Case 1.1 0.9 M¯, Xc = 0.35 ASTEC – CESAM0

  43. Case 1.1 0.9 M¯, Xc = 0.35 STAROX – CESAM0

  44. Hydrogen abundance 1.2 M¯ X0 = 0.7 Z0 = 0.02 Xc = 0.69 X

  45. CLES – CESAM0 Case 1.2 1.2 M¯ X0 = 0.7 Z0 = 0.02 Xc = 0.69

  46. CLES – CESAM0 Case 1.2 1.2 M¯ X0 = 0.7 Z0 = 0.02 Xc = 0.69

  47. CLES – CESAM0 Case 1.2 1.2 M¯ X0 = 0.7 Z0 = 0.02 Xc = 0.69

  48. STAROX – CESAM0 Case 1.2 1.2 M¯ X0 = 0.7 Z0 = 0.02 Xc = 0.69

  49. STAROX – CESAM0 Case 1.2 1.2 M¯ X0 = 0.7 Z0 = 0.02 Xc = 0.69

  50. Hydrogen abundance 1.2 M¯ X0 = 0.73 Z0 = 0.01 MHeC/M = 0.1 X

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