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971.
The water-pressure temperature stability field of yoderite,ideally Mg2Al5.6Fe3 + 0.4Si4O18(OH)2, was determined at highoxygen fugacities by high-pressure bracketing runs on eightpossible breakdown reactions involving the phases chlorite,kyanite, talc, staurolite, pyrope, enstatite, boron-free kornerupine,cordierite, quartz, and invariably an excess of hematite. Yoderitewas found to be stable over the surprisingly large PT rangefrom 6 to 25 kbar water pressure and 590 to 795 C. It is thusa high-pressure mineral covering the upper amphibolite and portionsof the eclogite facies. In the presence of quartz its upperpressure stability is reduced to some 15 kbar, and its uppertemperature stability to 715 C. Two of the yoderite-producingreactions are anomalous as they show dehydration in the directiontowards lower temperatures. Importantly, this is also true forthe reaction kyanite + talc + hematite+H2O=yoderite+quartz whichis responsible for the only yoderite occurrence in nature atMautia Hill, Tanzania. Preliminary thermodynamic calculationsindicate thatowing to this unusual dehydration behaviorthestability field for the assemblage yoderite+quartz disappearsfor water activities lower than 0.5. The rarity of yoderitein natural rocks, which is in contrast to its large PT stabilityfield, must be explained on chemical rather than on physicalgrounds. Yoderite can only occur in whiteschist-type bulk compositionsrich in MgO, Al2O3, SiO2, and containing some iron, but poorin alkalis and CaO. Oxygen fugacities must be unusually highto keep Fe trivalent, andat least for rocks with excessquartzthe water activity must be high as well. In anenvironment of this kind, yoderite formation in the Mautia Hillwhiteschist may have occurred even at constant total pressureand temperature simply by an influx of hydrous fluid duringthe late stages of metamorphism under amphibolite facies conditions. 相似文献
972.
We have obtained infrared colors and limiting magnitudes from 1.25–4.8µm for a sample of 26 of the cm continuum radio sources located in the core of the Oph molecular cloud. Their colors demonstrate that the majority of the sources appear to be heavily reddened objects surrounded by circumstellar accretion disks. In these cases the radio emission most likely diagnoses accretion driven energetic outflow phenomena: either ionized winds or possibly synchrotron emission from shocked gas associated with stellar jets. 相似文献
973.
George W. Wetherill 《Astrophysics and Space Science》1994,212(1-2):23-32
The formation of the gas giant planets Jupiter and Saturn probably required the growth of massive 15 Earth-mass cores on a time scale shorter than the 107 time scale for removal of nebular gas. Relatively minor variations in nebular parameters could preclude the growth of full-size gas giants even in systems in which the terrestrial planet region is similar to our own. Systems containing failed Jupiters, resembling Uranus and Neptune in their failure to capture much nebular gas, would be expected to contain more densely populated cometary source regions. They will also eject a smaller number of comets into interstellar space. If systems of this kind were the norm, observation of hyperbolic comets would be unexpected. Monte Carlo calculations of the orbital evolution of region of such systems (the Kuiper belt) indicate that throughout Earth history the cometary impact flux in their terrestrial planet regions would be 1000 times greater than in our Solar System. It may be speculated that this could frustrate the evolution of organisms that observe and seek to understand their planetary system. For this reason our observation of these planets in our Solar System may tell us nothing about the probability of similar gas giants occurring in other planetary systems. This situation can be corrected by observation of an unbiased sample of planetary systems.Paper presented at the Conference onPlanetary Systems: Formation, Evolution, and Detection held 7–10 December, 1992 at CalTech, Pasadena, California, U.S.A. 相似文献
974.
975.
We report the first detection of interstellar nitrogen sulfide (NS) in cold dark clouds. Several components of the 2 pi 1/2, J = 3/2 --> 1/2 and J = 5/2 --> 3/2 transitions were observed in TMC-1 and L134N. The inferred column density for TMC-1 is NNS approximately 8 x 10(12)cm-2 toward the NH3 peak in that cloud, and in L134N is NNS approximately 3 x 10(12)cm-2 toward the position of peak NH3 emission. These values correspond to fractional abundances relative to molecular hydrogen of fNS approximately 8 x 10(-10) for TMC-1, and fNS approximately 6 x 10(-10) for L134N. The NS emission is extended along the TMC-1 ridge and is also extended in L134N. The measured abundances are significantly higher than those predicted by some recent gas phase ion-molecule models. 相似文献
976.
Positions of active regions estimated from observations of the whole solar disk in Caii
K
iv
during the period 1977–1989 at the Coimbra Astronomical Observatory are compared with the time-dependent latitudinal distribution of background solar magnetic fields and with the latitudinal shifts of boundaries of their polarities. We confirm that the sunspot groups are located near the zonal boundaries between the opposite polarities of the solar background magnetic field during different phases of the two recent consecutive cycles of activity. We demonstrate a probable connection between the increased number of groups and the commencement of poleward migration of zonal boundaries in both hemispheres. But the influence of the dominant convective rolls seems to he still unclear. A new problem of interrelation between the zonal and sector boundaries has also appeared. 相似文献
977.
A WKB approach, based on the method of Connor, Hastie, and Taylor (1979), is used to obtain simple estimates of the critical
conditions for the onset of ideal MHD instabilities in line-tied solar coronal loops. The method is illustrated for the constant
twist, Gold-Hoyle (1960) field, and the critical conditions are compared with previous and new numerical results. For the
force-free case, the WKB estimate for the critical loop length reduces to
. For the sufficiently non-force-free case the critical length can be expressed in the forml
0 +l
1/m. The results confirm the findings of De Bruyne and Hood (1992) that for force-free fields them = 1 mode is the first mode to become unstable but for the sufficiently strong non-force-free case this reverses with them → ∞ mode being excited first. 相似文献
978.
Definition and measurement of salinity in salt lakes 总被引:4,自引:0,他引:4
Salinity is the most important chemical attribute of athalassic salt lakes. Even so, some confusion persists of what salinity means and how to measure it. For sal lakes, salinity is best defined as the sum total of all ion concentrations, or total ion concentration. Ideally, it is recommended that salinities be expressed on a mass per mass basis and as ppt (parts per thousand). Direct measurements of salinity can only be derived from full ionic analyses. Indirect measurements can be derived by determinations of density, conductivity, freezing point depression and total dissolved solids or matter. 相似文献
979.
We discuss preliminary results of an 11.7 m imaging survey of ultracompact H II regions from the Wood and Churchwell radio survey. We find that that the morphologies of ionized gas and warm dust are often significantly different, indicating that an H II region classification scheme should be based on more than radio data. 相似文献
980.
H. A. R. De Bruin W. Kohsiek B. J. J. M. Van Den Hurk 《Boundary-Layer Meteorology》1993,63(3):231-257
A set of micro-meteorological data collected over a horizontal, uniform terrain (the plain of La Crau, France) in June 1987 is analysed. Conditions were predominantly sunny and arid, while due to the Mistral the wind speed could exceed 10 m/s. Verification of several methods to evaluate surface fluxes of heat, momentum and water vapour from the standard deviation of temperature, wind and specific humidity is presented. Also, a similar approach using the structure parameter of temperature is considered. These methods are all based on Monin-Obukhov (M-O) similarity theory. It is found that the standard deviation of temperature, vertical and horizontal wind speed as well as the structure parameter for temperature behave according to M-O similarity. It is shown that the sensible heat flux and friction velocity can be determined from a fast response thermometer and a cup anemometer. Also, it appears that the analytic solution of the set of governing equations as derived by the first author yields good results. M-O theory does not appear to work for the standard deviation of specific humidity. This may be due to the relative importance of large eddies. 相似文献