Skip to content
DraconiticResearch
Search Sources API
186,631 studies31 sourcesUpdated 15 min ago
PreprintCC BY 4.0arXiv

Internal heating in rapidly rotating convection is not a shortcut to geostrophic turbulence

Abstract

Convective turbulence in planets and stars is often driven by internal heating. This forcing mechanism has also been proposed as a means of accessing the diffusion-free scalings of the geostrophic turbulence (GT) regime at modest forcing. We test this with the asymptotically reduced quasi-geostrophic model, which is formally valid in the limit of vanishing Ekman number, Ek → 0, and retains the Prandtl number as an independent parameter. We find no such shortcut: the Nusselt and Reynolds numbers are no closer to their diffusion-free predictions than in the boundary-heated case, and at Pr = 7 they are further from them; the predicted Pr−1/2 collapse fails; and the prefactor depends on the form of the heating. Our no-slip/stress-free cases track the radiatively driven simulations of Hadjerci et al. (2024) case by case, yet a 25% variation in Nu persists between sweeps that share the same reduced Rayleigh and Prandtl numbers but differ in Ekman number. Those data span only the narrow range of forcing over which the compensated Nusselt number is stationary; across the wider range accessible to the reduced model it rises to a maximum and then falls. We argue that bulk transport scalings are incomplete diagnostics of GT, whereas the saturation of the interior mean temperature gradient and of the vertical velocity kurtosis remain reliable indicators.

Related

  1. Interaction of eccentricity tide and convection
    Jiachen Zheng, Xing Wei
    Astronomy & AstrophysicsPeer-reviewedPublisher termsPlanetary science & exoplanetsCrossref
  2. Magnetic conditions governing the transition to penumbral magneto-convection
    David Korda, Jan Jurčák, Nazaret Bello González
    Astronomy & AstrophysicsPeer-reviewedPublisher termsSolar & stellar physicsCrossref
  3. Global solar compressible convection simulations on non-Cartesian mappings
    Grégoire Doebele, Allan Sacha Brun, Maxime Delorme
    Astronomy & AstrophysicsPeer-reviewedPublisher termsSolar & stellar physicsCrossref
  4. EPRV asteroseismology of the K dwarfs GJ 570 A and GJ 783 A with ESPRESSO. Empirical mode-amplitude scaling in tension with 3D convection simulations
    T. L. Campante, Y. Zhou, Y. Li +21
    Astronomy & AstrophysicsPeer-reviewedPublisher termsSolar & stellar physicsCrossref
  5. Interaction of eccentricity tide and convection
    Jiachen Zheng, Xing Wei
    arXivPreprintCC BY 4.0Full textPlanetary science & exoplanetsAtmospheric science & meteorologyarXiv
BibTeX
@misc{nicoski2026internal,
  title = {{Internal heating in rapidly rotating convection is not a shortcut to geostrophic turbulence}},
  author = {Justin A. Nicoski and Tobias G. Oliver and Stefano Maffei and Michael A. Calkins},
  howpublished = {arXiv},
  year = {2026},
  month = aug,
  doi = {10.48550/arxiv.2608.28756},
  eprint = {2608.28756},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2608.28756},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Internal heating in rapidly rotating convection is not a shortcut to geostrophic turbulence
AU  - Justin A. Nicoski
AU  - Tobias G. Oliver
AU  - Stefano Maffei
AU  - Michael A. Calkins
PY  - 2026
DA  - 2026/08/28
PB  - arXiv
DO  - 10.48550/arxiv.2608.28756
UR  - https://arxiv.org/abs/2608.28756
AB  - Convective turbulence in planets and stars is often driven by internal heating. This forcing mechanism has also been proposed as a means of accessing the diffusion-free scalings of the geostrophic turbulence (GT) regime at modest forcing. We test this with the asymptotically reduced quasi-geostrophic model, which is formally valid in the limit of vanishing Ekman number, Ek → 0, and retains the Prandtl number as an independent parameter. We find no such shortcut: the Nusselt and Reynolds numbers are no closer to their diffusion-free predictions than in the boundary-heated case, and at Pr = 7 they are further from them; the predicted Pr^−1/2 collapse fails; and the prefactor depends on the form of the heating. Our no-slip/stress-free cases track the radiatively driven simulations of Hadjerci et al. (2024) case by case, yet a 25% variation in Nu persists between sweeps that share the same reduced Rayleigh and Prandtl numbers but differ in Ekman number. Those data span only the narrow range of forcing over which the compensated Nusselt number is stationary; across the wider range accessible to the reduced model it rises to a maximum and then falls. We argue that bulk transport scalings are incomplete diagnostics of GT, whereas the saturation of the interior mean temperature gradient and of the vertical velocity kurtosis remain reliable indicators.
ER  -