4.7 Article

Does Misalignment between Magnetic Field and Angular Momentum Enhance or Suppress Circumstellar Disk Formation?

期刊

ASTROPHYSICAL JOURNAL
卷 868, 期 1, 页码 -

出版社

IOP PUBLISHING LTD
DOI: 10.3847/1538-4357/aae4dc

关键词

magnetic fields; magnetohydrodynamics; protoplanetary disks; stars: protostars

资金

  1. JSPS KAKENHI [17KK0096, 17K05387, 17H06360, 17H02869, 18K13581]
  2. Grants-in-Aid for Scientific Research [17KK0096, 18K13581, 17K05387] Funding Source: KAKEN

向作者/读者索取更多资源

The effect of misalignment between the magnetic field B and the angular momentum J(ang) of molecular cloud cores on the angular momentum evolution during the gravitational collapse is investigated by ideal and non-ideal MHD simulations. For the non-ideal effect, we consider the ohmic and ambipolar diffusion. Previous studies that considered the misalignment reported qualitatively contradicting results. Magnetic braking was reported as being either strengthened or weakened by misalignment in different studies. We conducted simulations of cloud core collapse by varying the stability parameter a (the ratio of the thermal to gravitational energy of the core) with and without including magnetic diffusion. The non-ideal MHD simulations show the central angular momentum of the core, with theta = 0 degrees (J(ang) parallel to B) being always greater than that with theta = 90 degrees (J(ang) perpendicular to B), independently of a, meaning that circumstellar disks form more easily in a core with theta = 0 degrees. The ideal MHD simulations, in contrast, show the central angular momentum of the core with theta = 0 degrees being greater than with theta = 0 degrees for small a and smaller for large a. Inspection of the angular momentum evolution of the fluid elements reveals three mechanisms contributing to the evolution of the angular momentum: (i) magnetic braking in the isothermal collapse phase, (ii) selective accretion of the rapidly (for theta = 90 degrees) or slowly (for theta = 0 degrees) rotating fluid elements to the central region, and (iii) magnetic braking in the first core and the disk. The difference between the ideal and non-ideal simulations arises from the different efficiencies of (iii).

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