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Table 1
Comparison between several magnitudes at t = 698 yr of evolution of the SNR computed using IAD0 and STD schemes.
| Model | Scheme | Particles | Ejecta | Perturbation δ | | ΔE|/E0 | |Δrcm|/ |
|L|/(∑ i|Li|) | ||
| (× 106) | (km s-1) | ||||||||
|
|
|||||||||
| A1 | IAD0 | 1.46 | rnd | 0 | 6.5 × 10-3 | 8 × 10-5 | 10-4 | ||
| A2 | STD | 1.46 | rnd | 0 | 1.3 × 10-2 | 8.2 × 10-5 | 4 × 10-4 | ||
| B1 | IAD0 | 1.46 | rnd | 500 | 6.5 × 10-3 | 7.5 × 10-5 | 5.5 × 10-5 | ||
| B2 | STD | 1.46 | rnd | 500 | 1.3 × 10-2 | 8.4 × 10-5 | 4 × 10-4 | ||
| B3 | IAD0 (vector) | 1.46 | rnd | 500 | 7 × 10-3 | 7.5 × 10-5 | 3 × 10-4 | ||
| C1 | IAD0 | 1.46 | Stretch | 0 | 6.5 × 10-3 | 9 × 10-12 | 4 × 10-12 | ||
| C2 | STD | 1.46 | Stretch | 0 | 1.3 × 10-2 | 7 × 10-11 | 9 × 10-9 | ||
Notes. The deviation of the center of mass is normalized to
pc.
∑ i|Li| = ∑ i(| Lxi| + |Lyi| + |Lzi|).
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