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561.
The distributions of hydrocarbons and infauna in sediments below a permitted mixing zone for the disposal of treated ballast waters in Port Valdez, Alaska were examined annually, 1999–2001. The associations of biological measures and the abundance of selected benthic organisms to total aromatic hydrocarbons (TARO) ranged up to large-sized effects, as compared against minimum-effect criteria (|r|0.63). The apparent sensitivity of three polychaete worms to low levels of hydrocarbons makes them particularly useful as indicators of future changes in spatial distributions of hydrocarbons associated with discharged effluent. In 2001, sediment TARO concentrations decreased and the correlation values of TARO to biotic variables were generally less than in 1999 and 2000. Evidence supports a conclusion of a strong but spatially limited association of some fauna with accumulations of petroleum hydrocarbons in these sediments. 相似文献
562.
O. C. St. Cyr L. Sánchez-Duarte P. C. H. Martens J. B. Gurman E. Larduinat 《Solar physics》1995,162(1-2):39-59
We describe the ground segment, pre-launch operations concepts, and data products supporting the SOHO mission. Our goal is threefold: first, we provide a historical view of the design and development of the systems described here, as a background perspective to those who will use the system and those who may build such systems for future missions. Second, because we hope that many researchers from the solar and space physics communities will visit these facilities during the mission, we provide an overview for the benefit of the end-user. We anticipate that visitors to GSFC may plan observations for one or more of SOHO's complement of instruments, and such researchers may use the facilities to analyze data gathered by the SOHO instruments. Third, we present the working plan for investigators with groundbased or other spacebased instruments to collaborate with SOHO. 相似文献
563.
564.
Robert Howard 《Solar physics》1971,16(1):21-36
Magnetograph velocity data are studied for evidence of large-scale velocity fields. It is established that there exist on the surface of the sun regions of more or less coherent downward motion with dimensions of the order of a solar radius. Velocity amplitudes in these regions are in the range 50–75 m/sec. Downward-moving large-scale features are observed to live for at least several days in general and to rotate at least approximately with the solar rotation rate. Horizontal east-west motions appears to have lifetimes of at least many months. The extent in longitude of these horizontal features is about 25°. There is no evidence for meridional motions from these data, with an upper limit to the line-of-sight velocity of about 30 m/sec. Active regions, as reported previously, are areas of generally downward motion. Some features in the autocorrelation of the rotational velocity of the sun remain unexplained. 相似文献
565.
Howard F. Bates 《Planetary and Space Science》1974,22(6):925-937
An expression for the vertical velocity of the neutral atmosphere in the F-region is derived for Joule heating by the electric field that drives the auroral electrojet. When only vertical expansion is allowed, it is found that the vertical wind must always increase monotonically with altitude. The heating rate is proportional to the F-region ion density, so that appreciable heating, even during high electric fields, requires some production mechanism of ionization such as auroral secondary ionization or solar photoionization, in the lower F-region. Once started at night, when an ionizing source is present in the lower F-region, the expansion of the atmosphere transports ionization upward, thereby increasing the heating rate, and hence the expansion rate, i.e. positive feedback. Electric field strengths and F-region ion densities of 50 mV/m and 2 × 1011e/m3, respectively, will produce vertal neutral wind speeds of several tens of m/sec in the 300–500 km altitude range. During periods of high magnetic activity, i.e. high electric field, Joule heating can produce large increases in the relative N2 concentration in the upper F-region; computations made with a simple model suggest that tenfold increases can occur at 400 km altitude after the onset of magnetic activity, a result in agreement with satellite observations. When the Joule heating theory is applied to incoherent scatter data taken during one period of high heating, the horizontal electric field in the F-region is found to decrease markedly, possibly approaching zero as the field penetrates a weak, discrete auroral arc; the decrease began 10–20 km from the arc. 相似文献
566.
Robert F. Howard 《Solar physics》1991,132(2):257-270
Magnetogram data are analyzed to study east-west magnetic flux differences interpreted as the component of magnetic field line inclination at the photospheric level in a plane parallel to the solar equator. This component is determined by comparing average east-west pairs of flux values at equal distances from the central meridian. The average inclination of a whole region is such as to trail the rotation (incline toward the east) by about 1.9 deg. Leading and following polarities tilt toward each other by about 16 deg. Growing regions are strongly inclined to the west (to lead the rotation) with large differences between leading and following portions. Decaying regions are slightly inclined to the east with more normal differences between leading and following portions. These results concerning growing and decaying regions are seen with greater amplitude for reversed polarity regions. As the activity cycle progresses, the average inclination of the field lines of the following portions of regions varies from about 10 to about 3 deg (leading the rotation), and the average difference in inclination of the leading and following portions of regions decreases monotonically during the cycle from nearly 20 to about 11 deg. A slight difference is seen between the average east-west inclination angles of regions that are rotating faster than average and those that are rotating slower than average in the sense that slower regions are slightly inclined toward the east and faster regions toward the west. Some of these results may be related to the location or nature of the subsurface flux tubes to which the active regions fields are connected and also, perhaps, to the nature of this connection.Operated by the Association of Universities for Research in Astronomy, Inc., under Cooperative Agreement with the National Science Foundation. 相似文献
567.
S. T. Wu W. P. Guo M. D. Andrews G. E. Brueckner R. A. Howard M. J. Koomen C. M. Korendyke D. J. Michels J. D. Moses D. G. Socker K. P. Dere P. L. Lamy A. Llebaria M. V. Bout R. Schwenn G. M. Simnett D. K. Bedford C. J. Eyles 《Solar physics》1997,175(2):719-735
We present a qualitative and quantitative comparison of a single coronal mass ejection (CME) as observed by LASCO (July 28–29,
1996) with the results of a three-dimensional axisymmetric time-dependent magnetohydrodynamic model of a flux rope interacting
with a helmet streamer. The particular CME considered was selected based on the appearance of a distinct ‘tear-drop’ shape
visible in animations generated from both the data and the model.
The CME event begins with the brightening of a pre-existing coronal streamer which evolves into a ‘tear-drop’ shaped loop
followed by a Y-shaped structure. The brightening moves slowly outward with significant acceleration reaching velocities of
∼450 km s-1 at 30 R⊙.
The observed CME characteristics are compared with the model results. On the basis of this comparison, we suggested that the
observed features were caused by the evacuation of a flux rope in the closed field region of the helmet streamer (i.e., helmet
dome). The flux rope manifests itself as the cavity of the quasi-static helmet streamer and the whole system becomes unstable
when the flux rope reaches a threshold strength. The observed ‘tear-drop’ structure is due to the deformed flux rope. The
leading edge of the flux rope interacts with the helmet dome to form the typical loop-like CME. The trailing edge of this
flux rope interacts with the local bi-polar field to form the observed Y-shaped structure. The model results for the evolution
of the magnetic-field configurations, velocity, and polarization brightness are directly compared with observations.
Animations have been generated from both the actual data and the model to illustrate the good agreement between the observation
and the model. These animations can be found on the CD-ROM which accompanies this volume.
Supplementary material to this paper is available in electronic form at http://dx.doi.org/10.1023/A:1004923016322 相似文献
568.
M. R. Kundu T. E. Gergely E. J. Schmahl A. Szabo R. Loiacono Z. Wang R. A. Howard 《Solar physics》1987,108(1):113-129
We present meterwave maps of the solar corona made with the Clark Lake Radioheliograph at 30.9, 50, and 73.8 MHz for one solar rotation. We compare and contrast them with optical data: 10830 Å maps, white-light coronagraph images (SOLWIND and Mauna Loa K coronameter) and forbidden line scans. Most of the sources in the radio maps persist for two days or more, and appear to rotate approximately with the solar rate. A coronal hole seen against the disk at all three frequencies shows interesting similarities and significant differences with the optical signatures of the hole. Elongated features of the 50 MHz corona correspond rather well to the azimuthal position of white light streamers seen in SOLWIND images. Synoptic charts made from the radio maps show overall similarities to synoptic charts constructed from (limb) coronagraph data. Some of the differences may result from the different weightings given by the radio and optical data to density and temperature, or by the different sensitivities to non-radial geometries. We show that the combined use of meter wave and optical images provide considerable new insights into the three-dimensional structure of the low to middle corona. 相似文献
569.
Eit Observations of the Extreme Ultraviolet Sun 总被引:3,自引:0,他引:3
D. Moses F. Clette J.-P. Delaboudinière G. E. Artzner M. Bougnet J. Brunaud C. Carabetian A. H. Gabriel J. F. Hochedez F. Millier X. Y. Song B. Au K. P. Dere R. A. Howard R. Kreplin D. J. Michels J. M. Defise C. Jamar P. Rochus J. P. Chauvineau J. P. Marioge R. C. Catura J. R. Lemen L. Shing R. A. Stern J. B. Gurman W. M. Neupert J. Newmark B. Thompson A. Maucherat F. Portier-Fozzani D. Berghmans P. Cugnon E. L. Van Dessel J. R. Gabryl 《Solar physics》1997,175(2):571-599
The Extreme Ultraviolet Imaging Telescope (EIT) on board the SOHO spacecraft has been operational since 2 January 1996. EIT
observes the Sun over a 45 x 45 arc min field of view in four emission line groups: Feix, x, Fexii, Fexv, and Heii. A post-launch
determination of the instrument flatfield, the instrument scattering function, and the instrument aging were necessary for
the reduction and analysis of the data. The observed structures and their evolution in each of the four EUV bandpasses are
characteristic of the peak emission temperature of the line(s) chosen for that bandpass. Reports on the initial results of
a variety of analysis projects demonstrate the range of investigations now underway: EIT provides new observations of the
corona in the temperature range of 1 to 2 MK. Temperature studies of the large-scale coronal features extend previous coronagraph
work with low-noise temperature maps. Temperatures of radial, extended, plume-like structures in both the polar coronal hole
and in a low latitude decaying active region were found to be cooler than the surrounding material. Active region loops were
investigated in detail and found to be isothermal for the low loops but hottest at the loop tops for the large loops.
Variability of solar EUV structures, as observed in the EIT time sequences, is pervasive and leads to a re-evaluation of the
meaning of the term ‘quiet Sun’. Intensity fluctuations in a high cadence sequence of coronal and chromospheric images correspond
to a Kolmogorov turbulence spectrum. This can be interpreted in terms of a mixed stochastic or periodic driving of the transition
region and the base of the corona. No signature of the photospheric and chromospheric waves is found in spatially averaged
power spectra, indicating that these waves do not propagate to the upper atmosphere or are channeled through narrow local
magnetic structures covering a small fraction of the solar surface. Polar coronal hole observing campaigns have identified
an outflow process with the discovery of transient Fexii jets. Coronal mass ejection observing campaigns have identified the
beginning of a CME in an Fexii sequence with a near simultaneous filament eruption (seen in absorption), formation of a coronal
void and the initiation of a bright outward-moving shell as well as the coronal manifestation of a ‘Moreton wave’.
Supplementary material to this paper is available in electronic form at http://dx.doi.org/10.1023/A:1004902913117 相似文献
570.
Howard F. Bates 《Planetary and Space Science》1974,22(12):1625-1636
In the first few tens of minutes after the onset of widespread Joule heating, the motion of the ionospheric atmosphere can be approximated by the one-dimensional motion of a gas in a gravity field—a problem that is easily solved because the motion takes place at constant pressure. The solution provides an estimate of time for which the model is applicable to the physical situation. Seasonal variations of the early effects are examined by using ion profiles appropriate to each season. The results show that the atmosphere above 100 km is strongly modified within a few tens of minutes after the onset of widespread heating: the density can double, the temperature can increase several hundred degrees, and the molecular nitrogen concentration can quadruple. Vertical winds exceeding 100 m/sec at 400km altitude are possible for a brief period after the onset of electric fields of 100 mV/m—rare but observed events. In the first few tens of minutes after the onset of a given electric field, the greatest power is deposited in the thermosphere around summer solstice, while the greatest winds occur at 200 km altitude in the summer and at 400km in the winter. These differing seasonal effects show primarily that a given level of change occurs sooner for one season than another, not that long term seasonal differences exist. Once a magnetic storm is in progress, the quiet-day ion profiles change to the non-seasonal storm profile ; for this ion distribution, F-region effects are minimum regardless of season. Joule heating effects in the upper thermosphere are therefore concluded to be self-limiting. 相似文献