1. Standoff distance for the fast wind condition
r_mp(fast wind) = 9.14 R_E, between the quiet-wind (9.81 R_E) and storm-sheath (7.15 R_E) values -- closer to the quiet-wind value, since the fast wind's lower density partially offsets its higher speed in the dynamic-pressure product.
| Criterion | Points |
|---|
| Correct standoff-distance arithmetic | 8 |
| Correct comparative placement | 7 |
3. Reference dipole energy sensitivity
A 5% increase in B0 changes E0 by a factor of 1.05^2=1.1025, i.e., a 10.2% increase in E0 -- since real secular changes in Earth's dipole field over 165 years are much smaller than 5% (of order a fraction of a percent per decade), this effect is negligible for comparing the 1859 and 2017/2024 ring-current energies at the precision used in this course.
| Criterion | Points |
|---|
| Correct E0 recomputation and percent-change arithmetic | 6 |
| Correct negligibility judgment for the real secular-change timescale | 4 |
4. Geosynchronous compression revisited
P_dyn(quiet)=1.61e-09 Pa. Required pressure factor = (r_mp,quiet/6.6)^6=10.8. Required P_dyn=1.73e-08 Pa. Solving for v at fixed quiet-wind density gives v=1314 km/s -- a very high, though not physically impossible, solar wind speed, consistent with only the most extreme storm-time sheath speeds compressing the magnetopause this far inward.
| Criterion | Points |
|---|
| Correct pressure-factor arithmetic | 5 |
| Correct solved speed | 10 |