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Helioseismology and the Solar Cycle
- Rachel Howe - 2006
Mads L. Severinsen, Kristian Jerslev & Lars V. T. Occhionero
- d. 18. Maj 2010
Introduktion
 Direct observations of Solar Activity → From
Photosphere
 Activity originates from within the Convective
Zone
 Measure of solar interior → Helioseismology
Helioseismology 101
 Sun oscillates in Spherical Harmonic
Oscillations
Y l
m
 ,=−1m
clm Pl
m
cosei m
Helioseismology 101
l = 1, m = 0 l = 10, m = 5
Helioseismology 101
 l = 0
 l = 2
 l = 20
 l = 25
 l = 75
Helioseismology 101
 gravity modes
 Surface gravity
modes
 pressure modes
(acoustic)
Article Data
Sun as a Star l < 4 Whole Sun
Medium Degree l < 300 10''
High Degree l > 200 Very Local
Article Data
Changes in interior dynamics
- Torsional oscillation change
Changes in interior dynamics
- Phase and amplitude changes
Observations
 Changes in torsional
oscillation during period
 Possible changes all way
through convection zone
 Zonal flows: constrains
dynamo models
 Changes in meridional
flow oserved through
high l oscillations
Changes in mode-parameters
- Frequency shifts
Changes in mode-parameters
- Frequency shifts
Changes in mode-parameters
- Mechanisms
 Clear change in frequency as function of
activity and time
 No clear mechanism
 Not only a magnetic effect
Changes in mode-parameters
- Amplitude and Width
Changes in mode-parameters
- Width and Amplitude
Results:
 Damping due to surface activity
 Width and amplitude inversly related to lifetime
Subsurface structural changes
 Subsurface changes still unknown
– High l-modes drown in surface variations
– High l-modes hard to observe
 Better results with SDO ?
 We can only see the outermost part of surface
(R=99%)
Conclusion
 Chance to look into the Sun's Convection zone
 Gives experimental data to dynamo-model
confinement
 See changes in the suns hydrodynamics during
cycles

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Helioseismology and the solar cycle