88 research outputs found
OXYGEN ABUNDANCE AND ENERGY DEPOSITION IN THE SLOW CORONAL WIND
Observations of the extended corona obtained with the Ultraviolet Coronagraph Spectrometer (UVCS) on board the Solar and Heliospheric Observatory (SOHO) during the solar minimum years 1996 and 1997 have been analyzed to derive the oxygen abundance in the outer corona. A comparison of the absolute coronal abundance, measured in the coronal regions surrounding the quiescent solar minimum streamers, to the heliospheric values confirms that these regions are the dominant sources of the slow solar wind. However, the inferred coronal abundances are consistent with the heliospheric values only in case the ion velocity distribution is anisotropic and enhanced across the coronal magnetic field. Thus this analysis also leads to the conclusion that energy is deposited in the slow coronal wind at least up to 2.7 Râ and that the efficiency of energy deposition is likely to be related to the local coronal magnetic topology
Preliminary error budget analysis of the coronagraphic instrument metis for the solar orbiter ESA mission
METIS, the Multi Element Telescope for Imaging
and Spectroscopy, is the solar coronagraph foreseen for the ESA
Solar Orbiter mission. METIS is conceived to image the solar
corona from a near-Sun orbit in three different spectral bands: in
the HeII EUV narrow band at 30.4 nm, in the HI UV narrow
band at 121.6 nm, and in the polarized visible light band (590 â
650 nm). It also incorporates the capability of multi-slit
spectroscopy of the corona in the UV/EUV range at different
heliocentric heights.
METIS is an externally occulted coronagraph which adopts an
âinverted occultedâ configuration. The Inverted external occulter
(IEO) is a small circular aperture at the METIS entrance; the
Sun-disk light is rejected by a spherical mirror M0 through the
same aperture, while the coronal light is collected by two annular
mirrors M1-M2 realizing a Gregorian telescope. To allocate the
spectroscopic part, one portion of the M2 is covered by a grating
(i.e. approximately 1/8 of the solar corona will not be imaged).
This paper presents the error budget analysis for this newconcept
coronagraph configuration, which incorporates 3
different sub-channels: UV and EUV imaging sub-channel, in
which the UV and EUV light paths have in common the detector
and all of the optical elements but a filter, the polarimetric visible
light sub-channel which, after the telescope optics, has a
dedicated relay optics and a polarizing unit, and the
spectroscopic sub-channel, which shares the filters and the
detector with the UV-EUV imaging one, but includes a grating
instead of the secondary mirror.
The tolerance analysis of such an instrument is quite complex:
in fact not only the optical performance for the 3 sub-channels
has to be maintained simultaneously, but also the positions of M0
and of the occulters (IEO, internal occulter and Lyot stop), which
guarantee the optimal disk light suppression, have to be taken
into account as tolerancing parameters.
In the aim of assuring the scientific requirements are optimally
fulfilled for all the sub-channels, the preliminary results of
manufacturing, alignment and stability tolerance analysis for the
whole instrument will be described and discussed
PERSISTENT AND SELF-SIMILAR LARGE-SCALE DENSITY FLUCTUATIONS IN THE SOLAR CORONA
Density fluctuations of the low and midlatitude solar corona plasma are analyzed during the recent solar minimum period. Long time series of the intensity of the neutral hydrogen Lyα, 1216 A, line have been observed with the UltraViolet Coronagraph Spectrometer/Solar and Heliospheric Observatory at 1.7 R â, in low-latitude streamers and in regions where the slow solar wind is accelerated. Their frequency composition is investigated by using three different techniques, namely the Fourier, the Hurst, and the phase coherence analyses. The Fourier analysis reveals the existence of low-frequency f âα power spectra in the range from ~3 Ă 10â6 Hz to ~10â4 Hz, corresponding to periods from a few hours to a few days. The coronal density fluctuations are dominated by discontinuities separating structures with a minimum characteristic timescale of about 3 hr and a corresponding spatial scale of about 3 Ă 104 km. The nonlinear analysis technique based on the structure functions shows that for large timescales the coronal density fluctuations are statistically self-affine and give rise to an average Hurst exponent H = 0.654 ± 0.008. This indicates that the process underlying the variability of the corona and the slow wind at coronal level is a persistent mechanism, generating correlations among the plasma density fluctuations. Finally, the analysis based on the phase coherence index shows a high degree of phase synchronization of the coronal density variations for large timescales, which shows that the solar corona is dominated by phase coherent structures. The results of the analysis suggest a coupling of the variability of the solar corona and the photospheric dynamics induced by the convection at supergranular scale
STOCHASTICITY AND PERSISTENCE OF SOLAR CORONAL MASS EJECTIONS
The study of the statistical properties of coronal mass ejections (CMEs) reveals that their properties depend on the period of solar activity. In particular, when investigating the origin of the waiting time distribution between CMEs, a significant departure from a Poisson process during periods of high solar activity has been found, thus suggesting the existence of at least two physical processes underlying the origin of CMEs. One acts continuously, perhaps related to randomly occurring magnetic reconfigurations of the solar corona at large scales. The other plays a role only during the solar maximum, probably due to the photospheric emergence of magnetic flux as a statistically persistent mechanism, which generates long correlation times among CME events strong enough not to be destroyed by the former random process
STATISTICS OF DENSITY FLUCTUATIONS DURING THE TRANSITION FROM THE OUTER SOLAR CORONA TO THE INTERPLANETARY SPACE
This paper investigates the evolution of the plasma density fluctuations of the fast and slow solar wind from the solar corona into the interplanetary space. The study is performed by comparing the low-frequency spectra and the phase correlation of the proton density oscillations, measured in the inner heliosphere with the Helios 2 in situ instrumentation, with those due to the large-scale density perturbations observed with UVCS/SOHO in the outer corona. We find that the characteristics of density fluctuations of the fast solar wind are maintained in the transition from the outer corona to the inner heliosphere, thus suggesting a coronal imprint for the heliospheric large-scale 1/f 2 noise spectrum. In contrast, a quick dynamical evolution is observed in the slow wind, which, starting from large-scale fluctuations with strong phase correlations in the outer corona, gives rise to a Kolmogorov-like spectrum and an accumulation of density structures at small scales at 0.3 AU. This can be explained in the framework of nearly incompressible turbulence
Detection of Coronal Mass Ejections at L1 and Forecast of Their Geoeffectiveness
A novel tool aimed to detect solar coronal mass ejections (CMEs) at the Lagrangian point L1 and to forecast their geoeffectiveness is presented in this paper. This approach is based on the analysis of in situ magnetic field and plasma measurements to compute some important magnetohydrodynamic quantities of the solar wind (the total pressure, the magnetic helicity, and the magnetic and kinetic energy), which are used to identify the CME events, that is their arrival and transit times, and to assess their likelihood for impacting the Earths magnetosphere. The method is essentially based on the comparison of the topological properties of the CME magnetic field configuration and of the CME energetic budget with those of the quasi-steady ambient solar wind. The algorithm performances are estimated by testing the tool on solar wind data collected in situ by the Wind spacecraft from 2005 to 2016. In the scanned 12 yr time interval, it results that (i) the procedure efficiency is of 86% for the weakest magnetospheric disturbances, increasing with the level of the geomagnetic storming, up to 100% for the most intense geomagnetic events, (ii) zero false positive predictions are produced by the algorithm, and (iii) the mean delay between the potentially geoeffective CME detection and the geomagnetic storm onset if of 4 hr, with a 98% 2-8 hr confidence interval. Hence, this new technique appears to be very promising in forecasting space weather phenomena associated to CMEs
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