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Table 4
Mean radiants and the numbers of particles in the individual filaments when the P-R effect is calculated according to two different formulas.
| Classical P-R formulas | Formulas according to Klačka | ||||||||
| fil. | β | λ⊙ | α | δ | Ns | λ⊙ | α | δ | Ns |
|
|
|||||||||
| Filament F1 | |||||||||
| F1 | 0.00001 | 117.5 ± 5.5 | 354.1 ± 4.5 | 12.7 ± 1.3 | 783 | 117.6 ± 5.6 | 354.3 ± 4.6 | 12.7 ± 1.3 | 778 |
| F1 | 0.001 | 114.7 ± 4.9 | 351.9 ± 4.0 | 12.1 ± 1.1 | 441 | 115.3 ± 4.8 | 352.4 ± 3.9 | 12.2 ± 1.1 | 443 |
| F1 | 0.002 | 112.6 ± 3.9 | 350.3 ± 3.2 | 11.7 ± 0.8 | 194 | 112.9 ± 4.1 | 350.5 ± 3.4 | 11.8 ± 0.9 | 219 |
| F1 | 0.003 | 109.7 ± 3.8 | 348.2 ± 3.1 | 11.1 ± 0.8 | 83 | 109.4 ± 4.5 | 347.8 ± 3.6 | 11.1 ± 0.9 | 82 |
| F1? | 0.004 | 104.9 ± 2.9 | 344.1 ± 2.2 | 10.3 ± 0.6 | 11 | 105.0 ± 3.6 | 344.6 ± 2.9 | 10.3 ± 0.7 | 19 |
|
|
|||||||||
| Filaments F2 and transitory | |||||||||
| F2 | 0.00001 | 295.9 ± 6.5 | 228.1 ± 5.8 | −31.3 ± 2.1 | 1378 | 296.2 ± 6.7 | 228.4 ± 6.0 | −31.5 ± 2.1 | 1364 |
| F2 | 0.001 | 294.6 ± 6.4 | 226.6 ± 5.6 | −30.8 ± 2.0 | 533 | 295.2 ± 6.9 | 227.3 ± 6.1 | −31.1 ± 2.2 | 537 |
| F2 | 0.002 | 293.7 ± 6.2 | 225.5 ± 5.4 | −30.4 ± 1.8 | 80 | 293.8 ± 7.2 | 225.6 ± 6.2 | −30.4 ± 2.1 | 94 |
| F2 | 0.003 | 292.0 | 223.2 | −29.7 | 1 | 288.5 ± 4.2 | 220.6 ± 3.6 | −28.9 ± 1.2 | 7 |
| TF2 | 0.004 | 238.4 ± 2.8 | 184.1 ± 1.8 | −15.0 ± 0.7 | 39 | 238.5 ± 3.8 | 184.2 ± 2.4 | −15.0 ± 1.0 | 36 |
| TF2 | 0.005 | 227.1 ± 8.2 | 176.8 ± 5.2 | −12.0 ± 2.1 | 365 | 226.9 ± 8.1 | 176.7 ± 5.2 | −12.0 ± 2.1 | 355 |
| TF2 | 0.006 | 226.6 ± 7.8 | 176.5 ± 5.0 | −11.9 ± 2.0 | 378 | 226.2 ± 7.6 | 176.2 ± 4.9 | −11.8 ± 2.0 | 376 |
| TF2 | 0.007 | 227.7 ± 7.6 | 177.2 ± 4.8 | −12.2 ± 1.9 | 397 | 227.6 ± 8.2 | 177.1 ± 5.2 | −12.2 ± 2.1 | 369 |
| TF2 | 0.008 | 225.1 ± 7.3 | 175.5 ± 4.7 | −11.5 ± 1.9 | 354 | 225.5 ± 7.2 | 175.8 ± 4.5 | −11.6 ± 1.8 | 343 |
| TF2 | 0.0083 | 222.0 ± 7.4 | 173.3 ± 4.6 | −10.6 ± 1.8 | 118 | 222.4 ± 7.8 | 173.5 ± 4.9 | −10.7 ± 1.9 | 125 |
Notes. All for tev = 20 kyr.
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