The large-scale upwelling influence on the coastal urbanized area waters' quality according to hydro-optical observations

2021 ◽  
Author(s):  
Pavel D. Lomakin ◽  
Alexey I. Chepyzhenko ◽  
Anna A. Chepyzhenko
1978 ◽  
Vol 79 ◽  
pp. 253-262
Author(s):  
G. O. Abell

Holmberg's (1937) analysis of the distribution of double and multiple galaxies provided what may have been the first hint of a local inhomogeneity of greater scale than that of the Local Group. the idea of a Local Supercluster was subsequently revived by de Vaucouleurs (1953, 1956, 1958). the analyses of others, as well as the continuing study of de Vaucouleurs himself (1976 and references cited therein) have now effectively established the reality of the Local Supercluster. Several other more remote inhomogeneities, or “clouds” of galaxies, were described by Shane and Wirtanen (1954). the writer (Abell 1958) found the distribution of rich clusters to be clumpy, and published a finding list of several apparent superclusters (Abell 1961).


1974 ◽  
Vol 60 ◽  
pp. 249-256
Author(s):  
G. Monnet

This paper reviews recent optical results on the large scale distribution of ionized gas in spiral galaxies, including our own. There is a diffuse, inhomogeneous emission in the arm region in spirals, including our Galaxy, and in gas-rich galaxies a fainter diffuse emission between the arms.


2012 ◽  
Vol 52 (2) ◽  
pp. 197-203 ◽  
Author(s):  
D. G. Baishev ◽  
E. S. Barkova ◽  
K. Yumoto

2016 ◽  
Vol 7 (47) ◽  
pp. 7211-7215 ◽  
Author(s):  
Jan K. Szymański ◽  
Juan Pérez-Mercader

In this report, we employ a photo-controlled polymerization protocol featuring a fluorescent initiator to follow the evolution of the generated self-assembled microscopic structures in a phase-separating dispersion polymerization medium.


1994 ◽  
Vol 140 ◽  
pp. 370-371
Author(s):  
R. L. Hurt ◽  
J. L. Turner ◽  
D. Levine ◽  
K. M. Merrill ◽  
I. Gatley

Near infrared imaging can be a powerful tool in tracing the densest molecular structures in galaxies. The observable molecular emission originates in large molecular cloud complexes which are also subject to significant extinctions caused by the associated dust. It can be difficult to distinguish between regions of moderate and large molecular density with optical observations as both will appear optically thick. Since extinction in the near infrared is only about a tenth of the corresponding visual extinction, multi-band near infrared imaging will trace the regions of the highest optical depths much more effectively. With the advent of large format infrared imaging arrays it is now possible to use infrared extinction maps as a probe of the large scale distribution of molecular emission in extragalactic sources.


2012 ◽  
Vol 30 (2) ◽  
pp. 283-302 ◽  
Author(s):  
R. Maggiolo ◽  
M. Echim ◽  
C. Simon Wedlund ◽  
Y. Zhang ◽  
D. Fontaine ◽  
...  

Abstract. On 1 April 2004 the GUVI imager onboard the TIMED spacecraft spots an isolated and elongated polar cap arc. About 20 min later, the Cluster satellites detect an isolated upflowing ion beam above the polar cap. Cluster observations show that the ions are accelerated upward by a quasi-stationary electric field. The field-aligned potential drop is estimated to about 700 V and the upflowing ions are accompanied by a tenuous population of isotropic protons with a temperature of about 500 eV. The magnetic footpoints of the ion outflows observed by Cluster are situated in the prolongation of the polar cap arc observed by TIMED GUVI. The upflowing ion beam and the polar cap arc may be different signatures of the same phenomenon, as suggested by a recent statistical study of polar cap ion beams using Cluster data. We use Cluster observations at high altitude as input to a quasi-stationary magnetosphere-ionosphere (MI) coupling model. Using a Knight-type current-voltage relationship and the current continuity at the topside ionosphere, the model computes the energy spectrum of precipitating electrons at the top of the ionosphere corresponding to the generator electric field observed by Cluster. The MI coupling model provides a field-aligned potential drop in agreement with Cluster observations of upflowing ions and a spatial scale of the polar cap arc consistent with the optical observations by TIMED. The computed energy spectrum of the precipitating electrons is used as input to the Trans4 ionospheric transport code. This 1-D model, based on Boltzmann's kinetic formalism, takes into account ionospheric processes such as photoionization and electron/proton precipitation, and computes the optical and UV emissions due to precipitating electrons. The emission rates provided by the Trans4 code are compared to the optical observations by TIMED. They are similar in size and intensity. Data and modelling results are consistent with the scenario of quasi-static acceleration of electrons that generate a polar cap arc as they precipitate in the ionosphere. The detailed observations of the acceleration region by Cluster and the large scale image of the polar cap arc provided by TIMED are two different features of the same phenomenon. Combined together, they bring new light on the configuration of the high-latitude magnetosphere during prolonged periods of Northward IMF. Possible implications of the modelling results for optical observations of polar cap arcs are also discussed.


1981 ◽  
Vol 64 (2) ◽  
pp. 367-382
Author(s):  
G. Debney ◽  
D. Farnsworth

1970 ◽  
Vol 38 ◽  
pp. 107-121
Author(s):  
P. G. Mezger

The distribution of optically observed H II regions and OB stars with galactic longitude indicates that it is primarily determined by extinction by interstellar dust. Thus optical observations can, at the best, reveal the local structure in the vicinity of the sun. Radio observations, on the other hand, are not affected by dust. Thus the distribution of galactic radio sources, which peaks in the northern part at about lII = 17°.5, must be related to the large-scale structure of our Galaxy. Two radio recombination line surveys of the northern and southern sky yield kinematic distances. If only the ‘giant H II regions’ are retained, the following distribution is obtained: (1) Only 5 giant H II regions are found within the 4 kpc arm. (2) The bulk of the giant H II regions is concentrated in a ring between 4 and 6 kpc from the galactic center. (3) There are other concentrations of giant H II regions indicating the existence of the Sagittarius and Perseus arm. (4) The three features revealed by optical observations of H II regions in the vicinity of the sun cannot be matched with the large-scale distribution outlined by giant H II regions. This is particularly true for the so-called Orion arm. (5) At distances beyond 13 kpc from the galactic center virtually no giant H II regions are found. (6) The surface density of giant H II regions attains its maximum between 4 and 8 kpc; the surface density of neutral hydrogen (H I) attains its maximum between 11 and 15 kpc, but the actual space density of H I in the region 4 to 8 kpc may still be rather high.


Sign in / Sign up

Export Citation Format

Share Document