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: http://www.eso.org/~chummel/oyster/manual/node219.html Дата изменения: Tue Apr 28 19:12:50 2015 Дата индексирования: Sun Apr 10 20:39:58 2016 Кодировка: Поисковые слова: asteroid | 
 
 
 
 
 
 
 
  
This section is partially derived from ``Basic definitions for the USNO and NRL Optical Interferometers'' by D. Buscher.
A baseline vector  is oriented from telescope 1 to
telescope 2, i.e. the baseline coordinates are the coordinates of
station 2 minus the coordinates from station 1.  In the aperture
plane, the
 is oriented from telescope 1 to
telescope 2, i.e. the baseline coordinates are the coordinates of
station 2 minus the coordinates from station 1.  In the aperture
plane, the  coordinate increases to the East, and the
 coordinate increases to the East, and the  coordinate
increases to the North. (Remember though that
 coordinate
increases to the North. (Remember though that  coverages are plotted
in
 coverages are plotted
in 
 as seen on the sky, so that the source structure and visibility
function can be easily superposed.)
as seen on the sky, so that the source structure and visibility
function can be easily superposed.)
In PEARL, a map on the sky is allocated with the  -coordinate
corresponding to RA, which increases to the left (East). The relationship
between visibility and map is then
-coordinate
corresponding to RA, which increases to the left (East). The relationship
between visibility and map is then
![\begin{displaymath}V(u,v)=\int B(\xi,\eta) exp(-j2\pi [u\xi + v\eta ]) d\xi d\eta \end{displaymath}](img61.png)