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MAGNETIC TWIST OF EUV CORONAL LOOPS OBSERVED BY TRACE

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MAGNETIC TWIST OF EUV CORONAL LOOPS. OBSERVED BY TRACE. RyunYoung Kwon, ... There is a tendency that the twist in the middle of the loop is larger than both ... – PowerPoint PPT presentation

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Title: MAGNETIC TWIST OF EUV CORONAL LOOPS OBSERVED BY TRACE


1
MAGNETIC TWIST OF EUV CORONAL LOOPS OBSERVED BY
TRACE
  • RyunYoung Kwon, Jongchul Chae
  • Astronomy Program, School of Earth and
    Environmental Science
  • Seoul National University

2
Whats the issue?
3
Why does plasma of the coronal loop not disperse?
4
Why does plasma of the coronal loop not disperse?
Magnetic Tension
Gas Pressure
Magnetic Tension
5
Method
  • We decompose the coronal magnetic field B into a
    large-scale component B0 and small-scale
    component B1
  • Using the force-free condition for the
    large-scale field
  • The magnetohydrostatic equation describing the
    force balance across a loop at the small scale is
    given by
  • Pressure profile

6
  • Twist profile

7
  • Constant temperature (isothermal)
  • Electron density profile
  • Intensity profile
  • FWHM
  • Pressure excess

8
Method
  • Large Scale Field
  • Linear Force Free Model
  • Small Scale Field
  • Twisted Flux Tube Model
  • Combining the large-scale and small-scale yields
    the twist of the loop.
  • Data
  • TRACE EUV(17.1nm) Data
  • SOHO/MDI 96minutes Magnetogram

9
Small Scale Field
Sample2
  • Use TRACE MDI data taken by almost at the same
    time.
  • Select 11 points
  • align the TRACE and MDI

10
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11
FWHM
Pressure Excess
12
Large Scale Field,
Linear Force Free (C.E. Alissandrakis, 1981)
SOHO/MDI 96minutes Magnetogram
13
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14
  • To find the field line that best matches the
    loop,
  • we calculate a number of field lines using
    linear force-free extrapolations with different
    values of force-free alpha.
  • we choose the field line that minimizes by the
    distance d between the loop and the curve.

15
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16
Field Strength
17
Result
18
Result
19
Conclusion
  • The on-axis magnetic twist of the loop is found
    to be about from 1.5 to 2.5 which corresponds
    to a winding number about from 0.75 to 1.25.
  • There is a tendency that the twist in the middle
    of the loop is larger than both footpoint.

20
Further Work
  • We will extend this work to a number of EUV loops
    observed by TRACE and X-ray loops observed by
    Yohkoh.

21
REFERENCE
  • Jongchul Chae, 2005, ApJ, in press
  • C. E. Alissandrakis, 1981, AA, 100, 197
  • Handy, B. N., et al 1999, Sol. Phys., 187, 229
  • Priest, E. R. 1982, Solar Magnetohydrodynamics
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