Lab 05: Jeans Escape and Magnetopause Standoff: Earth versus Jupiter

Combine atmospheric-escape and magnetosphere pressure-balance physics to compare Earth's and Jupiter's protective magnetic environments.

Apparatus and Setup

This lab combines the Jeans-escape formalism (Lecture 09) with the magnetopause pressure-balance model (Lecture 10), using real measured planetary magnetic-field strengths, to compare Earth's and Jupiter's magnetospheric standoff distances quantitatively.

Materials and Data

PlanetEquatorial surface field B₀ (T)Radius (km)
Earth3.1 × 10⁻⁵6371.0
Jupiter4.28e-0469911.0

Assume typical solar-wind conditions at 1 AU (ρ_sw ≈ 8.4e-21 kg/m³, v_sw ≈ 400 km/s) for Earth; for Jupiter, note that the solar wind is roughly 27 times less dense at 5.2 AU than at 1 AU (inverse-square dilution), a correction you must apply.

Procedure

  1. Using the magnetopause pressure-balance formula from Lecture 10, compute Earth's magnetopause standoff distance in Earth radii, using the solar-wind density and speed given above.
  2. Correct the solar-wind density for Jupiter's greater distance (5.2 AU versus 1 AU) using the inverse-square dilution law, then compute Jupiter's magnetopause standoff distance in Jupiter radii.
  3. Compare your computed standoff distances (in units of each planet's own radius) to the observed values (∼10 R_E for Earth; ∼50-100 R_J for Jupiter, which varies substantially with solar-wind pressure) and discuss whether the order of magnitude matches.
  4. Using the Jeans-escape parameter formula from Lecture 09, compute λ for atomic hydrogen at Jupiter's cloud-top temperature (∼165 K) using Jupiter's escape velocity (59.5 km/s, from Lecture 01's table), and compare it to Earth's value from Lecture 09's worked example. Explain why Jupiter, despite its much colder cloud tops, retains hydrogen far more effectively than Earth does.
  5. In one paragraph, explain how a much larger magnetopause standoff distance (relative to the planet's own radius) might, in principle, provide additional protection against non-thermal atmospheric escape, and state why this is a plausible but not fully quantified effect (per Lecture 10's discussion).

Analysis and Uncertainty

Solar-wind density and speed both vary substantially with solar activity (by roughly a factor of a few), so the specific standoff-distance values computed here should be understood as representative, not exact, and should be reported with this caveat.

Deliverables

Assessment Criteria

References and Provenance