Heliospheric Propagation of ICMEs: The Drag-Based Model
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Heliospheric Propagation of ICMEs: The Drag-Based Model B. Vršnak 1 , T. Žic 1 , M. Dumbović 1 , J. Čalogović 1 , A. Veronig 2 , M. Temmer 2 , C. Moestl 2 , T. Rollett 2 , L. Rodriguez 3 1 Hvar Observatory, Faculty of Geodesy, Zagreb, Croatia 2 IGAM/Institute of Physics, University of Graz, Graz, Austria 3 Royal Observatory of Belgium, Brussels, Belgium This work has received funding from the European Commission FP7 Project COMESEP (263252) ACKNOWLEDGMEN T ABSTRACT The advanced space-weather forecast-tool for predicting the arrival of Interplanetary Coronal Mass Ejections (ICMEs) is presented. The forecast-tool is based on the "Drag-Based Model" (DBM), taking into account the ICME shape using cone geometry with a semi-circular leading edge, spanning over the ICME full angular width. DBM is based on a hypothesis that the driving Lorentz force that launches CME ceases in the upper corona, and that beyond certain distance the dynamics becomes governed solely by the interaction of the ICME and the ambient solar wind. This assumption is founded on the fact that in the interplanetary space fast ICMEs decelerate, whereas slow ones accelerate, showing a tendency to adjust their velocity with the ambient solar wind. In particular, we consider the option where the drag acceleration has the quadratic dependence on the ICME relative speed, which is expected in the collisionless environment, where the drag is caused primarily by emission of MHD waves. This is the simplest version of DBM, where the equation of motion can be solved analytically, providing explicit solutions for the Sun-Earth ICME transit time and the impact speed. Basic DBM results are compared with remotely-measured interplanetary kinematics of several ICMEs, whereas forecasting abilities are tested on the statistical basis by employing in situ measurements. An example is shown for the advanced version of DBM, where geometry of ICME is taken into account. THE BASIC MODEL The basic DBM is based on the hypothesis that beyond ~20 solar radii the MHD “aerodynamic” drag caused by the interaction of ICME with solar wind, becomes the dominant force, so the equation of motion becomes: .. . . r = – g (r – w) |r – w| Running-difference images of the ICME take-off (LASCO/SOHO) and source position (AIA/SDO), providing the basic model input v 0 (R 0 ,t 0 ) and advanced model input w and a CASE STUDIES Comparison of the modeled and observed ICME kinematics (based on STEREO A&B data) Measurements taken from Liu et al. 2010, ApJ 722, 1762 200 300 400 500 600 700 0 10 20 30 40 50 60 70 v(km /s) R 250 350 450 550 650 750 0 20 40 60 80 100 120 140 v(km /s) R STATISTICAL STUDY Comparing calculated and observed transit times and speeds at 1 AU we estimated range of values for g and w. Optimal values, g = 10 -7 km -1 and w = 500 km/s, have been found also by minimizing the scatter of the difference between the observed and calculated transit times (O– C). 0 10 20 30 0 1 2 3 % g (10 -7 km -1 ) 0 20 40 60 0 500 1000 % w (km s -1 ) Samples used: Schwenn et al., 2005, AnnGeo. 26, 1033, Manoharan, 2006 , SPh 235, 345 0 5 10 15 20 25 -36 -24 -12 0 12 24 36 48 60 % O-C (h) 0 20 40 60 80 100 0 12 24 36 48 60 % abs(O-C) [h] M S* S THE ADVANCED MODEL ONLINE FORCAST TOOL - EXAMPLE CONCLUSION SLOW As a consequence fast ICMEs deccelerate, whereas slow ICMEs accelerate ( r w ) FAST w is the speed of the solar wind and g is the drag parameter. The drag parameter depends on characteristics of both ICME and solar wind – the drag is stronger for broader, low-mass ICMEs in a high-density (slow) solar wind. In the simplest form , we assume g,w = const. . AIM: prediction of ICME arrival BASIC DBM ASSUMPTION: MHD drag governs the propagation of ICME beyond ~20 solar radii ADVANCED DBM ASSUMPTION: ICME is cone-shaped with the semi-circular leading edge INPUT: v 0 (R 0 ,t 0 ) and w from the coronagraphic observations, source position from EUV observations PARAMETERS: g, w=const. and are derived empirically (in simplest form ) OUTPUT: ICME transit time and speed at some distance from the Sun correspondence: [email protected] In the advanced form DBM takes into account also the shape of ICME, where ICME is cone-shaped with the semi-circular leading edge spanning over the ICME full angular width 2w. In the advanced version we track the propagation of the element moving along the angle a (derived using EUV observations as well), assuming that the overall shape remains unchanged. w a to the spacecraf t ICME direction M9 flare N19W36 CME v 0 (R 0 ,t 0 )=1315.1 km/s HALO, w=90deg INPUT OUTPUT http://oh.geof.unizg.hr/DBM/dbm.php
description
Heliospheric Propagation of ICMEs: The Drag-Based Model. B. Vršnak 1 , T. Žic 1 , M. Dumbović 1 , J . Čalogović 1 , A. Veronig 2 , M. Temmer 2 , C. Moestl 2 , T. Rollett 2 , L . Rodriguez 3 1 Hvar Observatory, Faculty of Geodesy, Zagreb, Croatia - PowerPoint PPT Presentation
Transcript of Heliospheric Propagation of ICMEs: The Drag-Based Model
Heliospheric Propagation of ICMEs: The Drag-Based Model
B. Vršnak1, T. Žic1, M. Dumbović1, J. Čalogović1, A. Veronig2, M. Temmer2,C. Moestl2, T. Rollett2, L. Rodriguez3
1 Hvar Observatory, Faculty of Geodesy, Zagreb, Croatia2 IGAM/Institute of Physics, University of Graz, Graz, Austria
3 Royal Observatory of Belgium, Brussels, Belgium
This work has received funding
from the European Commission FP7
Project COMESEP (263252)
ACKNOWLEDGMENT
ABSTRACT
The advanced space-weather forecast-tool for predicting the arrival of Interplanetary Coronal Mass Ejections (ICMEs) is presented. The forecast-tool is based on the "Drag-Based Model" (DBM), taking into account the ICME shape using cone geometry with a semi-circular leading edge, spanning over the ICME full angular width. DBM is based on a hypothesis that the driving Lorentz force that launches CME ceases in the upper corona, and that beyond certain distance the dynamics becomes governed solely by the interaction of the ICME and the ambient solar wind. This assumption is founded on the fact that in the interplanetary space fast ICMEs decelerate, whereas slow ones accelerate, showing a tendency to adjust their velocity with the ambient solar wind. In particular, we consider the option where the drag acceleration has the quadratic dependence on the ICME relative speed, which is expected in the collisionless environment, where the drag is caused primarily by emission of MHD waves. This is the simplest version of DBM, where the equation of motion can be solved analytically, providing explicit solutions for the Sun-Earth ICME transit time and the impact speed. Basic DBM results are compared with remotely-measured interplanetary kinematics of several ICMEs, whereas forecasting abilities are tested on the statistical basis by employing in situ measurements. An example is shown for the advanced version of DBM, where geometry of ICME is taken into account.
THE BASIC MODELThe basic DBM is based on the hypothesis that beyond ~20 solar radii the MHD “aerodynamic” drag caused by the interaction of ICME with solar wind, becomes the dominant force, so the equation of motion becomes:.. . .r = – g (r – w) |r – w|
Running-difference images of the ICME take-off (LASCO/SOHO) and source position (AIA/SDO), providing the basic model
input v0(R0,t0) and advanced model input w and a
CASE STUDIES
Comparison of the modeled and observed ICME kinematics (based on STEREO A&B data)
Measurements taken from Liu et al. 2010, ApJ 722, 1762
200
300
400
500
600
700
0 10 20 30 40 50 60 70
v (k
m/s
)
R
250
350
450
550
650
750
0 20 40 60 80 100 120 140
v (k
m/s
)
R
STATISTICAL STUDY
Comparing calculated and observed transit times and speeds at 1 AU we estimated range of values for g and w.
Optimal values, g = 10-7 km-1 and w = 500 km/s, have been found also by minimizing the scatter of the difference between
the observed and calculated transit times (O– C).
0
10
20
30
0 1 2 3
%
g(10-7 km-1)
0
20
40
60
0 500 1000
%
w ( km s-1)
Samples used: Schwenn et al., 2005, AnnGeo. 26, 1033, Manoharan, 2006 , SPh 235, 345
0
5
10
15
20
25
-36 -24 -12 0 12 24 36 48 60
%
O-C (h)
0
20
40
60
80
100
0 12 24 36 48 60
%
abs(O-C) [h]
M S*
S
THE ADVANCED MODEL ONLINE FORCAST TOOL - EXAMPLE
CONCLUSION
SLOWAs a consequence fast
ICMEs deccelerate, whereas slow ICMEs accelerate ( r w )
FAST
w is the speed of the solar wind and g is the drag parameter. The drag parameter depends on characteristics of both ICME and solar wind – the drag is stronger for broader, low-mass ICMEs in a high-density (slow) solar wind.In the simplest form , we assume g,w = const.
.
AIM: prediction of ICME arrivalBASIC DBM ASSUMPTION: MHD drag governs the propagation of ICME beyond ~20 solar radii ADVANCED DBM ASSUMPTION: ICME is cone-shaped with the semi-circular leading edgeINPUT: v0(R0,t0) and w from the coronagraphic observations, source position from EUV observationsPARAMETERS: g, w=const. and are derived empirically (in simplest form )OUTPUT: ICME transit time and speed at some distance from the Sun (e.g. 1 AU)ADVANTAGES: easy handling, straightforward application in the real-time space-weather forecastingDRAWBACKS: does not predict arrival of shock, typical error for forecast models (~10 h)
correspondence:[email protected]
In the advanced form DBM takes into account also the shape of ICME, where ICME is cone-shaped with the semi-circular leading edge spanning over the ICME full angular width 2w.
In the advanced version we track the propagation of the element moving along the angle a (derived using EUV observations as well), assuming that the overall shape remains unchanged.
wa
to the spacecraft
ICME direction
M9 flareN19W36 CME v0(R0,t0)=1315.1km/s HALO, w=90deg
INPUT
OUTPUT
http://oh.geof.unizg.hr/DBM/dbm.php
