RADIATION FIELD OF X-RAY TUBES IS SUBJECT OF NEW WORLD STANDARD

1985 ◽  
Vol 15 (2) ◽  
pp. 12
2006 ◽  
Vol 21 (2) ◽  
pp. 170-170
Author(s):  
T. McNulty ◽  
S. Bird ◽  
A. Martin ◽  
L. Daniels
Keyword(s):  

2004 ◽  
Vol 15 (4) ◽  
pp. 419-439 ◽  
Author(s):  
Dennis E. Ogburn

Abstract Ethnohistorical and archaeological data suggest that a collection of more than 450 finely worked Inka building stones found near Saraguro in the southern highlands of Ecuador originated outside that region. The origin of those andesite blocks was investigated via geochemical analysis. Wavelength-dispersive X-ray fluorescence determined the concentrations of nine elements in samples from stones in the Saraguro region and in samples from known Inka andesite quarries at Cojitambo in the southern sierra of Ecuador, and at the Rumiqolqa and Huaccoto quarries near the Inka capital of Cuzco in Peru. The results show that the geochemical composition of the Saraguro stones closely matches that of the Rumiqolqa material, indicating that the Inka had these large andesite blocks moved over a distance of more than 1,600 km, the greatest known distance for the transport of large objects in the precolumbian New World. This endeavor had many implications, including reinforcing state power and ideology, and is also perceived to reflect an imperial “made-work” policy that consumed excess labor through non-utilitarian assignments. These “made-work” projects are best explained as a strategy for reinforcing state control over subject provinces, in contrast to current models of Inka economic organization that focus on efficiency in the use of labor.


1995 ◽  
Vol 163 ◽  
pp. 522-522
Author(s):  
Ian R. Stevens ◽  
Andrew M.T. Pollock

The low X-ray temperatures and luminosities of colliding wind binaries compared to theoretical expectations has been a long standing problem. As a potential solution to this problem we present quantitative calculations of the radiation hydrodynamics in colliding wind binary systems, accounting for the effect of two radiation fields on the dynamics of both winds, using a formulation similar to that of Castor et al. (1975, ApJ 195, 157). A more detailed description of this work can be found in Stevens & Pollock (1994, MNRAS in press). Consider only the WR wind being driven under the influence of the WR and O-star radiation fields and motion only on the line-of-centers. Near the WR-star, its own radiation field dominates, and the mass-loss rate will be largely unaffected by the presence of the companion. However, moving towards the O-star, the O-star radiation field becomes a significant fraction of the total flux. As the O-star radiation field is opposed to the WR radiation field the radiative line-force will be diminished and the wind acceleration diminished. This will lead to the WR star wind colliding with the O-star wind at a lower velocity than would be expected from single star models. This mechanism will only be at work in close binary systems. In wide binaries both winds will be at terminal velocity before the other radiation field makes a difference. Results for a sample calculation are shown in Fig 1, using parameters for V444 Cyg from Schmutz et al. (1989, A&A 210, 236). In the absence of any deceleration effects the WR wind velocity at the shock would be ∼ 1300 km s−1, corresponding to kT ∼ 2 keV. The reduction in the WR star velocity at the shock interface caused by the O-star radiation field is predicted to be ∼ x2 leading to kTx ∼ 0.5 keV, in line with X-ray observations.


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