[Show abstract][Hide abstract] ABSTRACT: The coronal mass ejection (CME) event on April 3, 2010 is the first fast CME observed by STEREO SECCHI/HI for the full Sun-Earth line. Such an event provides us a good opportunity to study the propagation and evolution of CME from the Sun up to 1 AU. In this paper, we study the time-dependent evolution and propagation of this event from the Sun to Earth using the 3D SIP-CESE MHD model. The CME is initiated by a simple spherical plasmoid model: a spheromak magnetic structure with high speed, high pressure and high plasma density plasmoid. The simulation performs a comprehensive study on the CME by comparing the simulation results with STEREO and WIND observations. It is confirmed from the comparison with observations that the MHD model successfully reproduces many features of both the fine solar coronal structure and the typical large scale structure of the shock propagation and gives the shock arrival time at Earth with an error of sim 2 hours. Then we analyze in detail the several factors affecting the CME's geo-effectiveness: the CME's propagation trajectory, span angle and velocity.
Journal of Geophysical Research: Space Physics 11/2014; 119(12). DOI:10.1002/2014JA020347 · 3.44 Impact Factor
[Show abstract][Hide abstract] ABSTRACT: We investigate the variations in the ionosphere during a small geomagnetic
storm on June 23, 2000, using the total electron content of the Jet
Propulsion Laboratory global positioning system, and the ionospheric
critical frequency. Large and long-lasting reductions in the daytime
electron density were observed at mid-latitudes in the northern hemisphere
by ionosondes. These reductions reached 30% to 40% compared to the 27-
day median value. At the same time, a transformation from similar large
positive storm effects to negative storm effects was observed in the northern
hemisphere by the global positioning system receivers. The geomagnetic
disturbance was very weak from June 23-25, 2000, as the SYM-H index
was >−40 nT and ASY-H was <90 nT. Of note, during this case there
were neither long-lasting southward IMF Bz nor strong positive IMF By
components, where a large positive IMF By might be the main reason for
ionospheric storms during minor geomagnetic disturbances [Goncharenko
et al. 2006]. We confirm a 13-h enhanced energy input from the disturbed
solar wind by calculation of the Borovsky, Akasofu and Newell coupling
functions, the global auroral precipitation, and the Joule heating. We
suggest this enhanced energy input as the main cause of these intense
ionospheric storms, although the maximum of the energy input was not
large. In addition, we propose that the Newell coupling function might be
more suitable for reflecting the energy transfer from the disturbed solar
wind to the magnetosphere under weak geomagnetic activity.
Annals of geophysics = Annali di geofisica 06/2012; 55(5). DOI:10.4401/ag-5409 · 1.16 Impact Factor
[Show abstract][Hide abstract] ABSTRACT: 1] We study the source locations of 130 solar flare-type II radio burst events with the associated interplanetary shocks observed by L1 spacecraft (type A events) and 217 flare-type II events without such shocks observed at L1 (type B events) during February 1997–August 2002. In particular, we investigate the relative positions between the flare sources, the heliospheric current sheet (HCS), and the Earth. We found the following results: (1) Solar flares are usually distributed within [S30°, N30°] in heliographic latitude and [S30°, N30°] Â [E10°, W30°] is the predominant source region on the solar disk that includes the majority of geoeffective solar flares. (2) The shocks with the associated flares located near the HCS would have a lower probably of reaching the Earth. For the Earth-encountered shocks, their initial speeds are distinctly higher when their associated flares are located near the HCS. (3) The angular distance from the flare source to the Earth (defined as Y below) also contributes to the probability of the associated shock being observed at the Earth. The shock arrival probability decreases with the increment of Y and the mean initial shock speed increases with Y for those Earth-encountered shocks. (4) The so-called ''same-opposite side effect'' of the HCS is confirmed to exist. That is, the shocks whose associated flares are located on the same side of the HCS as the Earth (called as ''same side events'') have a greater chance of reaching the Earth than those shocks with their associated flares on the opposite side (''opposite side events''). Here for the first time, a comprehensive sample of solar transient events of both arriving and nonarriving ones (at Earth) is used to testify to the same-opposite side effect. These results would be valuable in understanding the solar-terrestrial relations, and helpful for space weather prediction.
Journal of Geophysical Research Atmospheres 01/2007; 112. DOI:10.1029/2006JA012205 · 3.44 Impact Factor
[Show abstract][Hide abstract] ABSTRACT: Using 100 CME–ICME events during 1997.01–2002.11, based on the eruptive source locations of CMEs and solar magnetic field observations at the photosphere, a current sheet magnetic coordinate (CMC) system is established in order to statistically study the characteristics of the CME–ICME events and the corresponding geomagnetic storm intensity. The transit times of CMEs from the Sun to the Earth are also investigated, by taking into account of the angle between the CME eruption normal (defined as the vector from the Sun center to the CME eruption source) and the Sun-Earth line. Our preliminary conclusions are: 1. The distribution of the CME sources in our CMC system is obviously different from that in the ordinary heliographic coordinate system. The sources of CMEs are mainly centralized near the heliospheric current sheet (HCS), and the number of events decreases with the increment of the angular distance from the CME source to the HCS on the solar surface; 2. A large portion of the total events belong to the same–side events (referring to the CME source located on the same side of the HCS as the Earth), while only a small portion belong to the opposite–side events (the CME source located on the opposite side of the HCS as the Earth). 3. The intense geomagnetic storms are usually induced by the same–side events, while the opposite side events are commonly associated with relatively weak geomagnetic storms; 4. The angle between the CME normal and the Sun–Earth line is used to estimate the transit time of the CME in order to reflect the influence of propagation characteristic of the CME along the Sun–Earth direction. With our new prediction method in context of the CMC coordinate, the averaged absolute error for these 100 events is 10.33 hours and the resulting relative error is not larger than 30% for 91% of all the events.
Astrophysics and Space Science 11/2006; 305(1):37-47. DOI:10.1007/s10509-006-9039-6 · 2.40 Impact Factor
[Show abstract][Hide abstract] ABSTRACT: Solar transient activities such as solar flares, disappearing filaments, and coronal mass ejections (CMEs) are solar manifestations
of interplanetary (IP) disturbances. Forecasting the arrival time at the near Earth space of the associated interplanetary
shocks following these solar disturbances is an important aspect in space weather forecasting because the shock arrival usually
marks the geomagnetic storm sudden commencement (SSC) when the IMF Bz component is appropriately southward and/or the solar wind dynamic pressure behind the shock is sufficiently large. Combining
the analytical study for the propagation of the blast wave from a point source in a moving, steady-state, medium with variable
density (wei, 1982; wei and dryer 1991) with the energy estimation method in the ISPM model (smith and dryer 1990, 1995),
we present a new shock propagation model (called SPM below) for predicting the arrival time of interplanetary shocks at Earth.
The duration of the X-ray flare, the initial shock speed and the total energy of the transient event are used for predicting
the arrival of the associated shocks in our model. Especially, the background speed, i.e., the convection effect of the solar
wind is considered in this model. Applying this model to 165 solar events during the periods of January 1979 to October 1989
and February 1997 to August 2002, we found that our model could be practically equivalent to the prevalent models of STOA,
ISPM and HAFv.2 in forecasting the shock arrival time. The absolute error in the transit time in our model is not larger than
those of the other three models for the same sample events. Also, the prediction test shows that the relative error of our
model is ≤10% for 27.88% of all events, ≤30% for 71.52%, and ≤50% for 85.46%, which is comparable to the relative errors of
the other models. These results might demonstrate a potential capability of our model in terms of real-time forecasting.
Solar Physics 10/2006; 238(1):167-186. DOI:10.1007/s11207-006-0185-3 · 3.81 Impact Factor
[Show abstract][Hide abstract] ABSTRACT: 1] Solar flares and metric type II radio bursts are one kind of preliminary manifestations of solar disturbances and they are fundamental for predicting the arrival of associated interplanetary (IP) shocks at Earth. We statistically studied 347 solar flare type II radio burst events during 1997.2–2002.8 and found (1) only 37.5% of them were followed by the IP shocks at L1 (in other words, at Earth), the others without such IP shocks account for 62.5%; (2) the IP shocks associated with intense flares have large probability to arrive at Earth; (3) the IP shocks associated with central flares are more likely to arrive at Earth than those associated with the limb flares, and the most probable location for flares associated with IP shocks at Earth is W20°; and (4) there exists a east-west asymmetry in the distribution of geoeffectiveness of flare-associated IP shocks along the flare longitude. Most severe geomagnetic storms (Dst min À100 nT) are usually caused by flare-associated shocks originating from western hemisphere or middle regions near central meridian, and the most probable location for strong flares associated with more intense geomagnetic storms is W20° as well. These results could provide some criteria to estimate whether the associated shock would arrive at Earth and corresponding geomagnetic storm intensity.
Journal of Geophysical Research Atmospheres 01/2006; 111. DOI:10.1029/2006JA011784 · 3.44 Impact Factor
[Show abstract][Hide abstract] ABSTRACT: Using 80 CME-ICME events during 1997.1–2002.9, based on the eruptive source locations of CMEs and solar magnetic field observation
at the photosphere, a current sheet magnetic coordinate (CMC) system is established in order to study the propagation of CME
and its geoeffectiveness. In context of this coordinate system, the effect of the eruptive source location and the form of
heliospheric current sheet (HCS) at the eruptive time of CME on the geomagnetic storm intensity caused by CME and the CME’s
transit time at the Earth is investigated in detail. Our preliminary conclusions are: 1) The geomagnetic disturbances caused
by CMEs tend to have the so-called “same side-opposite side effect”, i.e. CMEs erupt from the same side of the HCS as the
earth would be more likely to arrive at the earth and the geomagnetic disturbances associated with them tend to be of larger
magnitude, while CMEs erupting from the opposite side would arrive at the earth with less probability and the corresponding
geomagnetic disturbance magnitudes would be relatively weaker. 2) The angular separation between the earth and the HCS affect
the corresponding disturbance intensity. That is, when our earth is located near the HCS, adverse space weather events occur
most probably. 3) The erupting location of the CME and its nearby form of HCS will also affect its arrival time at the earth.
According to these conclusions, in this context of CMC coordinate we arrive at new prediction method for estimating the geomagnetic
storm intensity (Dst
min) caused by CMEs and their transit times. The application of the empirical model for 80 CME-ICME events shows that the relative
error of Dst is within 30% for 59% events with Dst
min≤−50 nT, while the averaged absolute error of transit time is lower than 10 h for all events.
Keywordscoronal mass ejections-current sheet magnetic coordinate system-geomagnetic storm intensity-transit time-prediction method
Science in China Series E Technological Sciences 01/2005; 48(6):648-668. DOI:10.1360/03ye0240 · 1.02 Impact Factor