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P'K' Manoharan

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Title: P'K' Manoharan


1
Radio Scintillation Imaging of Solar
Wind Structures from Sun to Earth
Radio Scintillation Imaging of Solar
Wind Structures from Sun to Earth
P.K. Manoharan Radio Astronomy Centre National
Centre for Radio Astrophysics Tata Institute of
Fundamental Research Ooty 643001,
India mano_at_ncra.tifr.res.in
P.K. Manoharan Radio Astronomy Centre National
Centre for Radio Astrophysics Tata Institute of
Fundamental Research Ooty 643001,
India mano_at_ncra.tifr.res.in
Low-Frequency Radio Universe December 8 12,
2008 NCRA-TIFR, Pune
2
This presentation is dedicated toLate Prof.
N.V.G. Sarma
3
Outline of the talk
Ooty Scintillation Studies
  • Outline
  • Interplanetary Scintillation
  • Coronal Structures and associated solar wind
  • Solar-wind Speed and Density Turbulence images
  • Solar Cycle 23 Changes in 3-D Solar wind
  • Propagation of CME in the inner heliosphere
  • Summary

4
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5
Solar Wind
  • Solar wind collisionless, magnetized plasma
  • Continual, but variable, out flow from the Sun
  • Composed of approximately equal numbers of ions
    and electrons
  • Ions predominantly of protons (95) small
    amount of doubly ionized helium and trace amounts
    of heavier ions
  • Drags coronal magnetic field
  • Supersonic (and super Alfvenic)
  • Hot gt 105 K
  • Rarified (few particles/cm-3 at 1 AU)
  • Complex (due to solar variability, solar
    rotation, in-situ processes)
  • Carries waves and turbulence
  • Evolution of solar wind turbulence in the
    near-Sun region is important
  • Role of turbulence in accelerating the solar wind
  • Origin of fluctuations themselves
  • Interplanetary scintillation (IPS) technique is
    useful to probe the level of turbulence in the
    solar wind

6
Interplanetary Scintillation Studies
7
Interplanetary Scintillation
Radio source
L-O-S
Sun
Earth
8
Intensity scintillation
Intensity, I(t)
Time (t)
9
IPS Power Spectrum
Space and time correlation of Intensity
fluctuations
Transformation of the autocorrelation function
gives the power spectrum
Radial dependence of density fluctuations
Scintillation Index (m) measure of density
fluctuations (turbulence)
10
Solar wind Density Turbulence
  • Density Turbulence
  • Scintillation index, m, is a measure of
    level of turbulence
  • Normalized Scintillation index, g m(R) /
    ltm(R)gt
  • g gt 1 ? enhancement in ?Ne
  • g ? 1 ? ambient level of ?Ne
  • g lt 1 ? rarefaction in ?Ne

Scintillation enhancement w.r.t. the ambient wind
identifies the presence of solar wind transients
along the line-of-sight to the radio source
11
  • Interplanetary Scintillation measurements
  • Provide 3-D view of the inner heliosphere
  • Level of density fluctuations (or) turbulence
  • Scale-size of density irregularities
  • Speed of the solar wind
  • Information on angular size of radio source
  • Solar wind speed and Density turbulence
  • spectrum, FNe(q)
  • By suitably transforming and calibrating the
    intensity scintillation time series

12
Solar wind Relation to coronal Structures
13
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14
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15
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16
Origin of low-speed wind
17
What determines the solar wind speed ?
18
Spectra associated with ambient low- and
high-speed solar wind flows
Solar wind Density turbulence spectrum
Density turbulence spectrum associated with
propagating CME
cut-off (inertial) scale VA/?P
N1/2 VA Alfven speed ?P
Proton cyclotron frequency N Plasma density
19
Interplanetary Scintillation at Ooty
Importance of IPS technique increases when the
day to-day monitoring of heliosphere (solar wind)
is made on a grid of large number of radio
sources.
  • ORT can observe Solar wind
  • 20 250 Rsun
  • at all helio latitudes
  • large number of sources observed (900 per day)
  • provide density turbulence and speed images in
    3-D

20
Distribution of IPS Sources
4500 sources
21
Solar rotation and radial outward flow of the
solar wind provide the 3-d structure of the
solar wind at different view angles
Computer Assisted Tomography analysis
can remove the line-of-sight integration imposed
on the solar wind parameters also provides high
spatial resolution
22
Solar Wind Density Turbulence and Speed (3 days)
23
Ooty IPS measurements Density Turbulence and
Speed of the Solar Wind in the Inner heliosphere
February 25 March 25, 2005
CR2027
24
Distribution of IPS Sources
(angular size of compact component)
25
Solar Cycle 23 - Photospheric Magnetic Field
Latitude (deg)
1
Year
26
Solar Cycle 23 Solar Wind Density Distribution
Solar Wind Density Turbulence (Ooty)
27
Solar Cycle 23 Solar wind Speed Distribution
28
Interaction and Shock formation
  • An interaction region compresses the magnetic
    field of the ambient solar wind by an amount such
    that its pressure equals the rate of change of
    the momentum of the diver.
  • In the region between the shock and driver, thus
    a strong amplification of magnetic field is
    possible.

29
Radial Evolution of Coronal Mass Ejections
30
Coronal Mass Ejections
Coronal Mass Ejections
  • ? Largest phenomenon associated with the
    dissipation of
  • magnetic flux at and above the surface of
    the Sun
  • ? Travel outward at range of speeds, 10 -- 2500
    km/s
  • ? Mass involved in each ejection is 1014
    1015 g
  • ? Main cause of large geo-magnetic storms
  • ? CMEs appear to be an important factor of
    space weather,
  • which has multiple geospheric, biospheric,
    and technological
  • effects.
  • ? A great interest in understanding the
    propagation and arrival
  • of Earth-directed CMEs, which cause major
    storms at the
  • Earths magnetosphere.
  • ? However, there are many open questions
    concerning CMEs
  • origin, evolution, structure/extent in the
    interplanetary space
  • ? Largest phenomenon associated with the
    dissipation of
  • magnetic flux at and above the surface of
    the Sun
  • ? Travel outward at range of speeds, 10 -- 2500
    km/s
  • ? Mass involved in each ejection is 1014
    1015 g
  • ? Main cause of large geo-magnetic storms
  • ? CMEs appear to be an important factor of
    space weather,
  • which has multiple geospheric, biospheric,
    and technological
  • effects.
  • ? A great interest in understanding the
    propagation and arrival
  • of Earth-directed CMEs, which cause major
    storms at the
  • Earths magnetosphere.
  • ? However, there are many open questions
    concerning CMEs
  • origin, evolution, structure/extent in the
    interplanetary space

31
IPS Imaging of interplanetary disturbances (CIRs
and CMEs)
Shock
32
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33
Continuous acceleration? energy source?
IPS
Height-Time Plot
LASCO
Speed-Distance Plot
34
CME Propagation Speed (from Sun to Earth)
Height Time plot
Radial Evolution of Speed
K.E. lost/dissipated within lt100Rsun 1032 erg
VCME R-0.08 at R lt 100 Rsun VCME R-0.72 at
R gt 100 Rsun
35
  • VCME(R) of 30 CMEs
  • IPS LASCO provide sky-plane speeds
  • Include constant speed, accelerating and
  • decelerating events
  • VCME(R) can be represented by power-law
  • forms
  • VCME(R) R-ß R lt 50 R?
  • VCME(R) R-a R 100 - 200 R?
  • 2-step effective acceleration
  • Transition around 70 80 R?
  • at R lt 70 R? -0.3 lt ß lt 0.06

Speed Profiles VCME(R)
deceleration
constant speed
acceleration
36
CME Initial Speed vs Acceleration Slope at R gt
70 R?
deceleration zone
V 380 km/s
a 0.2-6.410-4V1.110-7V2
Aerodynamic drag force Interaction between CME
cloud and ambient solar wind plays an important
role in controlling the propagation of CME K.E.
utilized/gained times a against the drag force
imposed by the ambient solar wind (VCME
VAMB)2 shows good linear correlation (97)
acceleration zone
zero acceleration line
37
59 Events CME Initial Speed (LASCO field of view)
CME at 100 R? (Ooty IPS)
ICME Speed (at 1 AU)
Shock Speed (at 1 AU)
38
Geometry of magnetic flux rope IPS, cosmic ray,
and Spacecraft measurements
from Cosmic Ray data
from ACE IMF data
39
Current 3D Ooty Density Reconstruction
The left movie shows an ecliptic cut through the
3D Ooty IPS density reconstruction and the right
movie show a meridional cut (from East of the
Sun-Earth line) of the same both with the Earth
on the right-hand side and its orbit shown in
each case
40
Speed Comparisons with Wind in situ Data
41
CME internal energy
Summary
Ooty IPS measurements can provide the 3-D view of
solar wind transients, their dynamics, and nature
of interaction at the near-earth environment.
  • Near-Earth Manifestations required dynamic
    pressure and kinetic energy density depend on the
    energy exerted/deposited by the CME in the sheath
    portion of the shock
  • compression energy available from the CME
    expansion
  • Ooty images will be useful in understanding the
    reconnection processes associated with the
    earth-directed CMEs.
  • Space Weather Forecast Ooty data will play a
    crucial role

42
Thank You
43
Radial Evolution of CIRs
75 solar radii
100 solar radii
expansion
150 solar radii
44
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45
Initial Speed Arrival Time at 1 AU
TCME 109 - 0.5 10-1 VCME 1.1 10-5 V2CME
hours VCME 400 km/s, TCME 90 hours
(considerable assistance by CME expansion) VCME
2000 km/s, TCME dominated by interaction
Includes energy provided by CME Expansion SW
interaction
46
Bastille Day EventCoronal Mass Ejection July
14, 2000
TRACE Image of magnetic flux rope
236-MHz radio contour on Ha image
47
CME in the interplanetary medium
LASCO Images lt30 Rsun
Waves Radio Spectrum
Ooty Scintillation Images 50 - 250 Rsun
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