Table 1.
Key properties of the streamer waves for the simulation variants in the parameter study.
Variant | P [min] | λ [R⊙] | vph [km s−1] | λ/P [km s−1] |
---|---|---|---|---|
B1T1.32SSW | 324 | 7.25 | 283 | 259 |
B1T1.50SSW | 312 | 6.75 | 327 | 251 |
B1T1.63SSW | 300 | 6.5 | 320 | 251 |
B1T1.32 | 312 | 7.0 | 368 | 260 |
B1T1.50 | 336 | 7.5 | 392 | 250 |
B1T1.63 | 336 | 7.0 | 404 | 242 |
B2T1.32W4.5 | 180 | 5.0 | 383 | 322 |
B2T1.32 | 264 | 7.0 | 391 | 285 |
B2T1.32W8.5 | 336 | 9.0 | 403 | 294 |
B2T1.50 | 240 | 7.0 | 412 | 338 |
B2T1.63 | 252 | 7.0 | 424 | 322 |
B4T1.50 | 264 | 6.5 | 412 | 285 |
B4T1.63 | 264 | 6.5 | 424 | 285 |
B4T1.32FSW | 312 | 7.5 | 691 | 279 |
B4T1.50FSW | 384 | 9.0 | 667 | 272 |
B4T1.63FSW | 264 | 7.5 | 612 | 330 |
Notes. The names of the variants were chosen according to the values of the changing parameters: i.e. magnetic field (B) and temperature (T). The MSW variants are predominant, and so their names are not followed by an acronym, as in the case of SSW and FSW variants. An exception is variant B2T1.32, where the acronyms W4.5 and W8.5 indicate the additionally studied initial wavelengths of the induced perturbation.
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