We discuss the dynamical interpretation of evidence for an azimuthal tilt of the global magnetic field from the radial direction at the photosphere. We point out that the Reynolds stresses of supergranular convective motions might produce the required small tilt of intense flux tubes, without implyi
Average photospheric poloidal and toroidal magnetic field components near solar minimum
β Scribed by Thomas L. Duvall; Philip H. Scherrer; Leif Svalgaard; John M. Wilcox
- Publisher
- Springer
- Year
- 1979
- Tongue
- English
- Weight
- 564 KB
- Volume
- 61
- Category
- Article
- ISSN
- 0038-0938
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β¦ Synopsis
Average (over longitude and time) photospheric magnetic field components are derived from 3' Stanford magnetograms made near the solar minimum of cycle 21. The average magnetograph signal is found to behave as the projection of a vector for measurements made across the disk. The poloidal field exhibits the familiar dipolar structure near the poles, with a measured signal in the line Fe I h.5250 ~k of 1 G. At low latitudes the poloidal field has the polarity of the poles, but is of reduced magnitude (= 0.1 G). A net photospheric toroidal field with a broad latitudinal extent is found. The polarity of the toroida!, field is opposite in the nothern and southern hemispheres and has the same sense as subsurface flux tubes giving rise to active regions of solar cycle 21.
These observations are used to discusse large-scale electric currents crossing the photosphere and angular momentum loss to the solar wind.
π SIMILAR VOLUMES
Daily solar radio flux observations have been examined for a relationship to the large-scale photospheric magnetic field structure. Interplanetary magnetic field sector boundaries were used to indicate boundaries between photospheric field regions of opposite polarity. An enhancement in emission was
Doing numerical calculations of axially symmetric force-flee fields, have noticed that there seem to be no solutions if the toroidal component of the field exceeds a certain limit. In the present paper this problem is reexamined in the approximation of a plane stellar surface using a very simple an