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81.
82.
83.
The interaction of the solar wind with non-magnetic planets has been investigated theoretically taking account of the dilution of a planet's gravity field with distance and a uniform static external pressure of the incident solar wind. This results in the termination of the ionospheric boundary at a finite distance on the nightside of the planet. Numerical results are obtained for the shape of the boundary for different values of the scale height of the ionosphere, and for ratios of static to dynamic pressure of the incident solar wind. 相似文献
84.
S. Schramm V. Dexheimer A. Mukherjee J. Steinheimer 《Journal of Astrophysics and Astronomy》2018,39(4):42
The interior of neutron stars consists of the densest, although relatively cold, matter known in the universe. Here, baryon number densities might reach values close to ten times the nuclear saturation density. These suggest that the constituents of neutron star cores not only consist of nucleons, but also of more exotic baryons like hyperons or a phase of deconfined quarks. We discuss the consequences of such exotic particles on the gross properties and phenomenology of neutron stars. In addition, we determine the general phase structure of dense and also hot matter in the chiral parity-doublet model and confront model results with the recent constraints derived from the neutron star merger observation. 相似文献
85.
Characterization of tidally influenced seasonal nutrient flux to the Bay of Bengal and its implications on the coastal ecosystem 下载免费PDF全文
Submarine groundwater discharge (SGD) introduces solute and nutrients to the global oceans, resulting in considerable nutrient cycling and dynamics in the coastal areas. We have conducted high‐resolution, spatio‐temporal, lunar tidal cycle patterns and variability of discharged solute/nutrient assessment to get an overview of seasonal nutrient flux to the Bay of Bengal in eastern parts of the Indian subcontinent. Whereas the premonsoon season SGD was found to be dominant in the marine influence (M‐SGD), the postmonsoon season was found to be predominated by the terrestrial component of SGD (T‐SGD), extending from coast to near offshore. The solute fluxes and redox transformation were found to be extensively influenced by tidal and diurnal cycles, overlapping on seasonal patterns. We have assessed the possible role of SGD‐associated solute/nutrient fluxes and their discharge mechanisms, and their associated temporal distributions have severe implications on the biological productivity of the Bay of Bengal. The estimated annual solute fluxes, using the average end‐member concentration of the SGD‐associated nutrients, were found to be 240 and 224 mM·m?2·day?1 for NO3? and Fetot, respectively. Together with huge freshwater flux from the Himalayan and Peninsular Indian rivers, the SGD has considerable influence on the bay water circulation, stratification, and solute cycling. Thus, the observation from this study implies that SGD‐associated nutrient flux to the Bay of Bengal may function as a nutrient sink, which might influence the long‐term solute/nutrient flux along the eastern coast of India. 相似文献
86.
Ria Mukherjee Sisir K. Mondal Minik T. Rosing Robert Frei 《Contributions to Mineralogy and Petrology》2010,160(6):865-885
The chromite deposits in the Archean Nuggihalli schist belt are part of a layered ultramafic–mafic sequence within the Western
Dharwar Craton of the Indian shield. The 3.1-Ga ultramafic–mafic units occur as sill-like intrusions within the volcano-sedimentary
sequences of the Nuggihalli greenstone belt that are surrounded by the tonalite–trondhjemite–granodiorite (TTG) suite of rocks.
The entire succession is exposed in the Tagdur mining district. The succession has been divided into the lower and the upper
ultramafic units, separated by a middle gabbro unit. The ultramafic units comprise of deformed massive chromitite bodies that
are hosted within chromite-bearing serpentinites. The chromitite bodies occur in the form of pods and elongated lenses (~60–500 m
by ~15 m). Detailed electron microprobe studies reveal intense compositional variability of the chromite grains in silicate-rich
chromitite (~50% modal chromite) and serpentinite (~2% modal chromite) throughout the entire ultramafic sequence. However,
the primary composition of chromite is preserved in the massive chromitites (~60–75% modal chromite) from the Byrapur and
the Bhaktarhalli mining district of the Nuggihalli schist belt. These are characterized by high Cr-ratios (Cr/(Cr + Al) = 0.78–0.86)
and moderate Mg-ratios (Mg/(Mg + Fe2+) = 0.38–0.58). The compositional variability occurs due to sub-solidus re-equilibration in the accessory chromite in the
serpentinite (Mg-ratio = 0.01–0.38; Cr-ratio = 0.02–0.99) and in silicate-rich chromitite (Mg-ratio = 0.06–0.48; Cr-ratio = 0.60–0.99).
In the massive chromitites, the sub-solidus re-equilibration for chromite is less or absent. However, the re-equilibration
is prominent in the co-existing interstitial and included olivine (Fo96–98) and pyroxene grains (Mg-numbers = 97–99). Compositional variability on the scale of a single chromite grain occurs in the
form of zoning, and it is common in the accessory chromite grains in serpentinite and in the altered grains in chromitite.
In the zoned grains, the composition of the core is modified and the rim is ferritchromit. In general, ferritchromit occurs
as irregular patches along the grain boundaries and fractures of the zoned grains. In this case, ferritchromit formation is
not very extensive. This indicates a secondary low temperature hydrothermal origin of ferritchromit during serpentinization.
In some occurrences, the ferritchromit rim is very well developed, and only a small relict core appears to remain in the chromite
grain. However, complete alteration of the chromite grains to ferritchromit without any remnant core is also present. The
regular, well-developed and continuous occurrence of ferritchromit rims around the chromite grain boundaries, the complete
alteration of the chromite grains and the modification of the core composition indicate the alteration in the Nuggihalli schist
belt to be intense, pervasive and affected by later low-grade metamorphism. The primary composition of chromite has been used
to compute the nature of the parental melt. The parental melt calculations indicate derivation from a high-Mg komatiitic basalt
that is similar to the composition of the komatiitic rocks reported from the greenstone sequences of the Western Dharwar Craton.
Tectonic discrimination diagrams using the primary composition of chromites indicate a supra-subduction zone setting (SSZ)
for the Archean chromitites of Nuggihalli and derivation from a boninitic magma. The composition of the komatiitic basalts
resembles those of boninites that occur in subduction zones and back-arc rift settings. Formation of the massive chromitites
in Nuggihalli may be due to magma mixing process involving hydrous high-Mg magmas or may be related to intrusions of chromite
crystal laden magma; however, there is little scope to test these models because the host rocks are highly altered, serpentinized
and deformed. The present configurations of the chromitite bodies are related to the multistage deformation processes that
are common in Archean greenstone belts. 相似文献
87.
Thin-section studies of the Zanskar Shear Zone (ZSZ) rocks reveal a top-to-SW and subsequent primary and secondary top-to-NE
ductile shearing; brittle–ductile and brittle extensions; top-to-SW brittle shear, steep normal faulting and fracturing. In
the proposed two-phase model of ductile extrusion of the Higher Himalayan Shear Zone (HHSZ), a top-to-SW simple shearing during
22–18 Ma was followed by a combination of top-to-SW simple shear and channel flow at 18–16 Ma. The second phase simulates
a thin ZSZ characterized by a top-to-NE shearing. The channel flow component ceased around 16 Ma, the extruding HHSZ entered
the brittle regime but the top-to-SW shearing continued until perturbed by faults and fractures. Variation in the extrusion
parameters led to variable thickness of the ZSZ. Shear strain after the extrusion is presumably maximum at the boundaries
of the HHSZ and falls towards the base of the ZSZ, which crudely matches with the existing data. The other predictions: (1)
spatially uniform shear strain after the first stage, (2) fastest extrusion rate at the base of the ZSZ, and (3) a lack of
continuation of the ZSZ along the Himalayan trend are not possible to validate due to paucity of suitable data. Non-parabolic
shear fabrics of the ZSZ indicate their heterogeneous deformation. 相似文献
88.
The Higher Himalayan Shear Zone (HHSZ) in the Sutlej section reveals (1) top-to-SW ductile shearing, (2) top-to-NE ductile shearing in the upper- and the lower strands of the South Tibetan Detachment System (STDSU, STDSL), and (3) top-to-SW brittle shearing corroborated by trapezoid-shaped minerals in micro-scale. In the proposed extrusion model of the HHSZ, the E1-phase during 25–19 Ma is marked by simple shearing of the upper sub-channel defined by the upper strand of the Main Central Thrust (MCTU) and the top of STDSU as the lower- and the upper boundaries, respectively. Subsequently, the E2a-pulse during 15–14 Ma was characterized by simple shear, pure shear, and channel flow of the entire HHSZ. Finally, the E2b-pulse during 14–12 Ma observed simple shearing and channel flow of the lower sub-channel defined by the lower strand of the Main Central Thrust (MCTL) and the top of the STDSL as the lower- and the upper boundaries, respectively. The model explains the constraints of thicknesses of the STDSU and the STDSL along with spatially variable extrusion rate and the inverted metamorphism of the HHSZ. The model predicts (1) shear strain after ductile extrusion to be maximum at the boundaries of the HHSZ, which crudely matches with the existing data. The other speculations that cannot be checked are (2) uniform shear strain from the MCTU to the top of the HHSZ in the E1-phase; (3) fastest rates of extrusion of the lower boundaries of the STDSU and the STDSL during the E2a- and E2b-pulses, respectively; and (4) variable thickness of the STDSL and rare absence of the STDSU. Non-parabolic shear fabrics of the HHSZ possibly indicate heterogeneous strain. The top-to-SW brittle shearing around 12 Ma augmented the ductile extruded rocks to arrive a shallower depth. The brittle–ductile extension leading to boudinage possibly did not enhance the extrusion. 相似文献
89.
Kalyan Kumar Bagchi Sukla Mukherjee Lokenath Debnath 《Pure and Applied Geophysics》1973,111(1):2255-2263
Summary With the aid of the generalized function method, a study is made of the linearized theory of transient development of capillary-gravity waves in an inviscid, incompressible and homogeneous liquid of finite and infinite depth due to an arbitrary oscillating source situated at a finite depth below the undisturbed free surface of the liquid. The initial value problem is solved by using Laplace-Fourier transforms combined with asymptotic methods. The asymptotic solution is found to consist of the steady state and the transient components which are independently modified by surface tension. The latter decays more rapidly as timet due to the presence of surface tension than in the case where surface tension is neglected. It is predicted that the principal effect of surface tension is to increase both the phase and group velocity of the waves and make the energy more readily available among the rapidly travelling progressive surface waves. In addition to the effects of surface tension on the physical properties of the wave motions, our method of solution provides an interesting illustration of the applicability of generalized functions in water wave phenomena. 相似文献
90.
The rocketsonde data obtained from the launchings made at Thumba (8°3215N, 76°5148E) during the winter period 1970–71, as already reported, have indicated that warmings of noticeable magnitude occurred at high levels (upper stratosphere and mesosphere) over this tropical station during the period mentioned. The mean monthly radiosonde temperatures of 50, 100 and 300 mb levels at Thumba (Trivandrum) and Delhi (28°35N, 77°12E) during the same period have also pointed out certain anomalies consistent with the warmings referred to above at Thumba. The radiosonde temperatures of the two stations, Thumba (Trivandrum) and Delhi, have now been examined, along with the values of total ozone, for the ten winter periods commencing from 1961–1962. The analysis has pointed out the possibility of high-level warmings also having occurred in the past over the Indian region during the winters of 1963–1964 and 1967–1968, which are also the periods when prominent warmings are definitely known to have occurred at higher latitudes. The behaviour of total ozone has been found to be different in the different years of the warmings. The features noticed have been presented and discussed. 相似文献