Table 5
Main characteristic values for several parameters found in the 4 analyzed simulations: maximum magnetic field intensity on the x axis, | B | max and position of this maximum and the width of the transition region Δxgrad B across the bow shock along the + x axis.
Process/run | Bow shock | Cometopause | |||||||
|
|||||||||
| B | max |
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Δxgrad B | Standoff | Curv. radius | Flaring | Standoff | Curv. radius | Flaring | |
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[nT] | [km] | [km] | [km] | [km] | [–] | [km] | [km] | [–] | |
|
|||||||||
PI | 27.7 | 500 | 400 | 830 ± 10% | 2920 | 2.65 | 210 ± 15% | 409 | 1.91 |
PI+EI | 29.2 | 800 | 500 | 2320 ± 10% | 10 203 | 2.99 | 540 ± 8% | 507 | 1.40 |
PI+CX | 25.7 | 700 | 1000 | 3840 ± 8% | 18 643 | 3.12 | 580 ± 12% | 492 | 1.30 |
PI+CX+EI | 25.9 | 800 | 1200 | 6570 ± 1% | 25 131 | 2.77 | 650 ± 9% | 916 | 1.68 |
Notes. Also tabulated, calculated from the quadric surface fits, are the mean bow shock (cometopause) standoff distance (
), the mean curvature radius
(
) around the nose of the surface and the average bow shock (cometopause) flaring ratio
(
). The runs considered include photoionisation only (PI run), photoionisation and electron ionisation (PI+EI run), photoionisation and charge exchange (PI+CX run) and all processes (PI+CX+EI run). All variables are defined in the text.
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