Title: ============== Non-Axisymmetric Large-Scale Photospheric Motions Lead Investigator: ======= R. S. Bogart Team Members: ================== T. Bai (if agreeable) P. H. Scherrer (if agreeable) Local Coordinator: ================== R. S. Bogart Lead Programmer: ===== J. Aloise Technical Summary: ================== Averaged MDI Dopplergrams show unmistakeable evidence for large-scale velocity features localized to narrow latitude bands. These bands may be evidence of steady zonal flows (torsional oscillation), localized meridional flows (convective rolls), radial flows or lineshifts. There is evidence that they are not continuous across the entire disc, however, indicating that they may be large-scale, but non-axisymmetric flows. They could also be associated with supergranule motions, as they are of comparable scale. I propose to investigate these structures with a view to (a) establishing their nature, i.e. the vector velocity fields or other phenomena responsible for them, (b) intially characterizing their size scale and lifetimes or stability, and (c) their probable effect on estimates of truly axisymmetric velocity structures. Proposal Text: ======================= The Dopplergrams taken during the first long uninterrupted set of MDI observations March 27-31, 1996, when averaged together, even before calibration, show clear alternating zonal bands of apparently enhanced and diminished velocity superimposed on the general pattern of global rotation (Fig. 1). The same structures are also plainly visible in only 6 hours of high-resolution Dopplergrams averaged together (Fig. 2). These zonal bands appear to be continuous over a sizeable portion of the globe (30 degrees in longitude), but *not* over the entire visible disc. Their width is about 3 degrees in latitude, with spacings of roughly 10 degrees in latitude. They show up clearly only at latitudes higher than about 30 degrees, but do not appear to be otherwise strongly affected by disc position. Their amplitude is of order 40-80 m/s. There are several possible explanations for these structures, and the immediate evidence for and against any of them is not obvious. They could be what they look like, bands of enhanced and diminished zonal velocity, similar to the torsional oscillation flows, but of sub-global extent. Their apparent continuity across the central meridian, or equivalently their lack of modulation with meridian distance, would argue against this. They could also be zones of meridional flow, or of radial flow, or of some more complicated velocity. The component vectors of the equivalent velocity field, if that is what the structures represent, can be determined by their symmetry properties with respect to the angle of observation, provided that the structures are sufficiently long-lived, and they appear to be. An alternative explanation is that the structures are artifacts caused by smaller stable velocity or line-shift structures rotating across the field of view, especially supergranules. Arguments against this are that the structures are not symmetric about the disc center (they do not appear at low latitudes even near the limb), and the length of the coherent bands seems to be independent of the length of the averaging interval. Nonetheless it should be possible to test this hypothesis simply by attempting to identify the endpoints of the zonal bands with corresponding supergranules. The method I propose to use to isolate and analyze the zonal bands is to first form a very accurate observational map of the limb shift (including the anisotropic component critical to measuring mean meridional flows) by forming long-term averages as simple functions of radius and azimuth as the apparent disc size changes over its full normal range; this will require 6 months of data, but reasonable range can be achieved with a much shorter interval if the radius is changing rapidly. Once this phenomenological limb shift is removed from the calibrated Dopplergrams, they can be mapped to appropriate heliographic grids as necessary and low-pass filtered to remove oscillations and granulation noise. In general remapping will not be necessary or desirable, as the distinctions among the various hypothetical sources depend on viewing angle. Whether or not the zonal velocity structures can be unambiguously explained, their mere characterization should suffice to estimate their effect on estimates of axisymmetric flows, provided that they can be followed for one or more complete rotations. Required Observations / Data: The data required for this project are simply full-disk Dopplergrams (high-res Dopplergrams may also be useful), suitably sampled and filtered to suppress oscillations and to be able to identify super-granulation. Dynamics Program data are ideal; any other long runs of Doppler data exceeding about 4 hours' duration, even data sampled as little as a few times an hour, may be useful. Certainly no special observations are required. However, one very useful, even critical observation for determining the phenomenological limb shift is a series of at least several hours of Dopplergrams made with a non-zero (and preferably large) position angle. I propose that the desirability of making such observations be considered when observing sequences are scheduled for the rare opportunities afforded by extended spacecraft roll maneuvers.