arXiv News

First-hand information for everyone

Site

AboutPrivacy PolicyTerms of Use

© 2026 arXiv News

Energy cascade rate in Earth’s magnetosheath is several orders of magnitude higher than in the solar wind, but decreases with distance from the bow shock | arXiv News

arXiv News

EnglishJapanese

Switch language

EnglishJapanese
Loading account…

First-hand information for everyone

Back to front page
Solar and Stellar AstrophysicsEnglishPublished

Energy cascade rate in Earth’s magnetosheath is several orders of magnitude higher than in the solar wind, but decreases with distance from the bow shock

November 3, 2026arXiv: 2610.41773v1

The 2023 Magnetospheric Multiscale spacecraft measured the rate at which turbulent magnetic energy cascades from large to small scales after solar‑wind plasma crosses Earth’s bow shock. Using the incompressible Hall–MHD Kármán–Howarth–Monin equation, the study found that the cascade rate is 100 to 1000 times higher than in the undisturbed solar wind. The mean rate in the magnetosheath reached about 4×10⁶ J kg⁻¹ s⁻¹, and the data span several orders of magnitude.

The measured cascade rate decreases only slightly with distance from the bow shock. A power‑law fit of the rates versus the relative distance, DB, gives ε∝DB^γ with γ≈−0.10. In other words, even two spacecraft radii downstream of the shock the turbulence remains strong and the cascade rate remains high.

Histogram of cascade‑rate values and a log‑log log‑linear plot of ε versus distance from bow shock displaying a decreasing trend
Figure 7. Figure 7 shows (a) the histogram of KHM cascade‑rate values, with a mean of ≈4 × 10⁶ J kg⁻¹ s⁻¹, and (b) the power‑law fit ε∝DB^γ with γ≈–0.10 for all convergent intervals.Montagud-Camps, Victor, Hellinger, Petr, Toledo-Redondo, Sergio, Verdini, Andrea, Sorriso-Valvo, Luca, Pecora, Francesco et al. · ·
arXiv:2610.41773v1 · Figure 7:
CC BY 4.0

Spectral analysis shows that magnetic‑field fluctuations become steeper in the inertial range as the plasma travels from the bow shock toward the magnetopause. The slope changes from roughly –1 near the shock to –1.8 near the magnetopause, indicating progressively more energetic small‑scale activity.

Plot of inertial‑range spectral index versus distance from bow shock, showing a steady steepening trend
Figure 4. Figure 4 displays the inertial‑range spectral index α as a function of the relative distance to the bow shock (DB). As DB increases from 0 (bow shock) to 1 (magnetopause), α steepens from about –1 to –1.8, while the sub‑ion spectral index slightly flattens.Montagud-Camps, Victor, Hellinger, Petr, Toledo-Redondo, Sergio, Verdini, Andrea, Sorriso-Valvo, Luca, Pecora, Francesco et al. · arXiv:2610.41773v1 · Figure 4: · CC BY 4.0

These measurements demonstrate that the bow shock dramatically amplifies turbulent energy transfer in the magnetosheath, with the cascade lasting across the entire sheath region.

Source paper

Decay of space plasma turbulence downstream of bow shocks: MMS magnetosheath unbiased campaign observations

Solar and Stellar AstrophysicsPhysics
View on arXiv