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distributions_of_shocks_in_simulations [2020/06/18 15:30] tr |
distributions_of_shocks_in_simulations [2020/06/19 10:38] (current) tr |
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| **__Reminder :__** | **__Reminder :__** | ||
| - | - The sound speed in the code units is 0.25. | + | - The sound speed in the code units is 0.25. |
| + | - Slow shocks are in blue. | ||
| + | - Fast shocks are red. | ||
| + | - Rotational discontinuities are green. | ||
| + | - Parker sheets are cyan. | ||
| **__Info :__** | **__Info :__** | ||
| - | Distributions are no longer normalised, so numbers on the y axis are the number of scans. | + | Distributions are no longer normalised, the numbers on the y axis are therefore numbers of scans. I kept only the best identifications we have (purest wave decompositions). It just makes distributions cleaner and analysis simpler. |
| {{:abc_v_scan.png?540 |}} | {{:abc_v_scan.png?540 |}} | ||
| Line 59: | Line 63: | ||
| **Thibaud**: | **Thibaud**: | ||
| I am actually doing it, but it's a lot of data and my internet connection is not very fast here... I'll tell you if is bimodal too. | I am actually doing it, but it's a lot of data and my internet connection is not very fast here... I'll tell you if is bimodal too. | ||
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| + | [Update :] | ||
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| + | {{:abc_b_scan.png?540 |}} | ||
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| + | {{:ot_b_scan.png?540 |}} | ||
| **Andrew**: | **Andrew**: | ||
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| So as usual higher shock velocities lead to higher shear velocities. But for a fixed shock velocity lower magnetic field strength gives higher shear velocity. | So as usual higher shock velocities lead to higher shear velocities. But for a fixed shock velocity lower magnetic field strength gives higher shear velocity. | ||
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| + | **__Magnetic field increments__** | ||
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| + | {{:abc_b_perp.png?540 |}} | ||
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| + | {{:ot_b_perp.png?540 |}} | ||
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| + | {{:abc_b_perp1.png?540 |}} | ||
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| + | {{:ot_b_perp1.png?540 |}} | ||
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| + | {{:abc_bperp_norm.png?540 |}} | ||
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| + | {{:ot_bperp_norm.png?540 |}} | ||