Table 1
Comparison of the model predictions with COPS and DFMS measurements in different time segments.
Acronym | Method | w | it | Time segment | δn | σn | ![]() |
![]() |
δCO | σCO | ![]() |
![]() |
---|---|---|---|---|---|---|---|---|---|---|---|---|
01.08-30.11 | 0.946 | 1.008 | 0.379 | 0.371 | 0.665 | 0.845 | 0.776 | 0.164 | ||||
f033c1w00 | EE | 0.0 | 0 | 15.09-30.10 | 1.192 | 1.227 | 0.412 | 0.445 | 0.797 | 1.130 | 0.757 | 0.193 |
08.10-12.10 | 1.196 | 1.264 | 0.334 | 0.383 | 0.423 | 0.515 | 0.767 | 0.164 | ||||
01.08-30.11 | 0.406 | 0.467 | 0.394 | 0.369 | 1.606 | 1.955 | 0.561 | 0.245 | ||||
f033c1w10 | EE | 1.0 | 0 | 15.09-30.10 | 0.450 | 0.605 | 0.467 | 0.392 | 2.168 | 2.401 | 0.608 | 0.219 |
08.10-12.10 | 0.509 | 0.534 | 0.377 | 0.381 | 1.668 | 1.538 | 0.634 | 0.207 | ||||
01.08-30.11 | 0.392 | 0.374 | 0.251 | 0.270 | 0.596 | 0.695 | 0.386 | 0.393 | ||||
f002a1w00 | EE | 0.0 | 2 | 15.09-30.10 | 0.466 | 0.475 | 0.260 | 0.298 | 0.690 | 0.930 | 0.431 | 0.495 |
08.10-12.10 | 0.497 | 0.483 | 0.160 | 0.200 | 0.364 | 0.424 | 0.305 | 0.295 | ||||
01.08-30.11 | 0.456 | 0.502 | 0.306 | 0.302 | 0.505 | 0.506 | 0.574 | 0.405 | ||||
f002a1w10 | EE | 1.0 | 2 | 15.09-30.10 | 0.502 | 0.628 | 0.348 | 0.330 | 0.589 | 0.662 | 0.552 | 0.391 |
08.10-12.10 | 0.593 | 0.666 | 0.294 | 0.322 | 0.438 | 0.323 | 0.470 | 0.298 | ||||
01.08-30.11 | ||||||||||||
f004a3w00 | EE | 0.0 | 4 | 15.09-30.10 | 0.309 | 0.229 | 0.289 | 0.284 | 0.707 | 0.861 | 0.475 | 0.487 |
08.10-12.10 | 0.298 | 0.227 | 0.199 | 0.221 | 0.412 | 0.333 | 0.326 | 0.252 | ||||
01.08-30.11 | ||||||||||||
m004a3w00 | DSMC | 0.0 | 4 | 15.09-30.10 | 0.275 | 0.285 | 0.188 | 0.186 | 0.581 | 0.681 | 0.327 | 0.328 |
08.10-12.10 | 0.338 | 0.291 | 0.119 | 0.134 | 0.227 | 0.200 | 0.226 | 0.164 |
Notes. Here method denotes the method of gas flow description (Euler equations or DSMC), w is the proportion of instantaneous and rotation-averaged energy input (see Eq. (1)), it is the iteration number of inhomogeneity factors adaptation, δn is the mean, σn is the dispersion of relative differences in the simulated and measured overall gas densities, and ,
, δCO are the means and σn,
,
, and σCO are the dispersions of relative differences in the simulated and measured relative abundances of H2O, CO, and CO2 at the position of the orbiter (see Eq. (8)).
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