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Hale Sector Boundaries.pdf - Leif and Vera Svalgaard's

Hale Sector Boundaries.pdf - Leif and Vera Svalgaard's

Hale Sector Boundaries.pdf - Leif and Vera Svalgaard's

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<strong>Hale</strong> <strong>Sector</strong> <strong>Boundaries</strong>Similarly the Eastern portion of active regions in these environs can gather fieldpreferentially with these orientations (those orientations which are supported by<strong>Hale</strong>’s laws). In other words, any little instability in this preferential orderingwould grow from pre-existing field with the orientations from their inherentenvironment.The geometry of the modern dynamo has a differing evolution than this shallowmodel: in conventional dynamo models, fields erupt from the Sun’s interioroutwards, whereas in the percolation model, field lines coalesce from small activeregions where field lines are shed from the granulations’ churning of Ephemeralregions. This temporal pattern is thus a difference between the st<strong>and</strong>ard dynamotheory <strong>and</strong> this new model.Aside from these differences, however, the geometry of fields at any time,in the shallow model is similar to the Babcock-Leighton field geometry (bothof course consistent with <strong>Hale</strong>’s laws), hence either view of the Solar dynamomight equally fit our observations. So, perhaps it is too early to tell whetherthe observations are preferentially supporting which theory. So, although we arefinding out some very important things about how field lines are evolving on <strong>and</strong>in the Sun, at present, it may be too early to distinguish whether the observationsprovide conclusive evidence on the exact location of the Sun’s dynamo.5. ConclusionAcknowledgementsThe authors thank Ken Schatten for fruitful discussions.SOLA: <strong>Hale</strong>Bx.tex; 21 July 2010; 7:55; p. 9

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