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265 | 265 | ! Limits to timestep controls give by fm, fr and fe.
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266 | 266 | ! As these three quantities evolve naturally to zero,
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267 | 267 | ! following strictly the timestep limit given by fX would
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268 |
| -! reduce timesteps infinetely. These fX_limit avoid this problem |
| 268 | +! reduce timesteps infinitely. These fX_limit avoid this problem |
269 | 269 | ! by computing the limit to the timestep as
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270 | 270 |
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271 | 271 | ! ::
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537 | 537 | ! explicit mass transfer computation.
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538 | 538 | ! ___________________________________
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539 | 539 |
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540 |
| -! MESA can compute mass transfer rates either explicitly (at the beggining |
| 540 | +! MESA can compute mass transfer rates either explicitly (at the begging |
541 | 541 | ! of the step) or implicitly (iterating the solution until the mass transfer
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542 | 542 | ! rate matches the value computed at the end of the step). The explicit method
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543 | 543 | ! is used if ``max_tries_to_achieve <= 0``.
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863 | 863 | ! ~~~~~~~~~~
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864 | 864 |
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865 | 865 | ! Include loss of angular momentum via mass loss. The parameters
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866 |
| -! ``mass_transfer_*`` determine the fractions of mass lost from the vincinity |
| 866 | +! ``mass_transfer_*`` determine the fractions of mass lost from the vicinity |
867 | 867 | ! of the donor, the accretor, or a circumbinary coplanar toroid.
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868 | 868 |
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869 | 869 | ! ::
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1330 | 1330 |
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1331 | 1331 | ! During CE, if the star spends this amount of time detached, terminate CE even if
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1332 | 1332 | ! CE_rel_rlo_for_detachment has not been reached.
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1333 |
| -! If set to a large number mass loss will only stop when the star definetely wants |
| 1333 | +! If set to a large number mass loss will only stop when the star definitely wants |
1334 | 1334 | ! to detach. If set to a low number system will likely switch to stable mass transfer.
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1335 | 1335 |
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1336 | 1336 | ! ::
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