Table 4.
Case | A | B | C | D | E | F | G | H | I | R ss | R td,y | R td,z |
---|---|---|---|---|---|---|---|---|---|---|---|---|
Gruesbeck et al. (2018) a | 0.049 0 | 0.157 0 | 0.153 0 | 0.026 0 | 0.012 0 | 0.051 0 | 0.566 0 | −0.031 0 | 0.019 0 | 1.557 | 2.624 | 2.495 |
All points, this work | 0.176 9 | 0.160 9 | 0.155 9 | 0.005 7 | 0.004 4 | 0.028 1 | 0.377 3 | −0.032 3 | 0.014 3 | 1.539 | 2.595 | 2.487 |
MY32, this work | 0.136 9 | 0.141 9 | 0.140 0 | 0.038 1 | 0.017 8 | 0.054 7 | 0.378 3 | 0.004 4 | 0.027 9 | 1.654 | 2.639 | 2.575 |
MY33, this work | 0.166 0 | 0.151 6 | 0.150 1 | 0.023 5 | −0.006 1 | 0.020 3 | 0.380 7 | −0.028 4 | −0.001 8 | 1.562 | 2.664 | 2.587 |
MY34, this work | 0.171 9 | 0.174 2 | 0.155 1 | −0.011 2 | −0.006 8 | 0.016 5 | 0.395 5 | −0.025 6 | 0.012 7 | 1.522 | 2.470 | 2.499 |
MY35, this work | 0.557 7 | 0.224 5 | 0.200 0 | −0.050 9 | −0.010 3 | 0.096 3 | −0.142 1 | 0.001 1 | −0.011 9 | 1.472 | 2.108 | 2.266 |
Ls = [315°–45°], this work | 0.155 4 | 0.162 5 | 0.158 7 | −0.026 5 | −0.008 1 | 0.002 3 | 0.426 0 | 0.001 3 | 0.004 4 | 1.513 | 2.477 | 2.496 |
Ls = [45°–135°], this work | 0.171 9 | 0.176 1 | 0.155 5 | −0.027 5 | 0.004 8 | 0.056 4 | 0.410 7 | −0.028 7 | 0.005 7 | 1.497 | 2.466 | 2.518 |
Ls = [135°–225°], this work | 0.249 0 | 0.147 3 | 0.262 4 | 0.040 9 | 0.041 5 | 0.109 8 | 0.236 8 | −0.094 1 | −0.151 0 | 1.584 | 2.945 | 2.261 |
Ls = [225°–315°], this work | 0.155 9 | 0.148 4 | 0.140 0 | 0.004 7 | 0.022 7 | 0.040 0 | 0.358 3 | −0.007 2 | −0.019 7 | 1.632 | 2.620 | 2.744 |
EUV flux ≥ 0.002 8 W m−2 | 0.109 6 | 0.148 0 | 0.150 0 | 0.027 4 | 0.003 1 | 0.035 5 | 0.432 9 | −0.029 3 | 0.004 5 | 1.634 | 2.700 | 2.567 |
EUV flux W m−2 | 0.213 8 | 0.180 7 | 0.157 7 | −0.023 1 | −0.005 1 | 0.031 4 | 0.347 3 | −0.020 7 | 0.018 5 | 1.498 | 2.410 | 2.460 |
Quasi‐⊥ | 0.179 8 | 0.160 7 | 0.153 9 | 0.001 6 | 0.004 0 | 0.033 0 | 0.377 7 | −0.034 8 | 0.012 4 | 1.531 | 2.605 | 2.509 |
Quasi‐‖ | 0.142 7 | 0.167 5 | 0.166 6 | −0.000 4 | 0.005 1 | 0.005 0 | 0.399 2 | −0.009 8 | 0.023 0 | 1.595 | 2.473 | 2.382 |
Note. See Equation (9) for the definition of parameters A to I and Equations (11), (12), and (13) for those of the subsolar standoff distance R ss along the X MSO axis and the terminator standoff distances R td along the Y MSO and Z MSO axes. Uncertainties on the parameters are of the order of 1% in a least squares sense. All quadrics here are ellipsoids. The domain of validity for each fit is shown in Figure 9: fits are valid for X MSO ≥ −0.5 R p on average. The number of fitting points used for each case is the same as for the 2D fits, see Table 3 (last column). Also, see Appendix A for a physical interpretation of the tabulated parameters. R ss and R td are expressed in units of Mars radius R p = 3,389.5 km.
For all points considered in their data subset.