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											2017-08-02 20:43:06 +00:00
										 |  |  | A text box entitled Astronomical Data provides information needed for | 
					
						
							|  |  |  | tracking the sun or moon, compensating for EME Doppler shift, and | 
					
						
							|  |  |  | estimating EME Doppler spread and path degradation. Toggle the | 
					
						
							|  |  |  | *Astronomical data* on the *View* menu to display or hide this window. | 
					
						
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							|  |  |  | image::AstroData_2.png[align="center",alt="Astronomical Data"] | 
					
						
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							|  |  |  | Available information includes the current UTC *Date* and time; *Az* | 
					
						
							|  |  |  | and *El*, azimuth and elevation of the moon at your own location, in | 
					
						
							|  |  |  | degrees; *SelfDop*, *Width*, and *Delay*, the Doppler shift, full | 
					
						
							|  |  |  | limb-to-limb Doppler spread in Hz, and delay of your own EME echoes in | 
					
						
							|  |  |  | seconds; and *DxAz* and *DxEl*, *DxDop*, and *DxWid*, corresponding | 
					
						
							|  |  |  | parameters for a station located at the *DX Grid* entered on the main | 
					
						
							|  |  |  | window.  These numbers are followed by *Dec*, the declination of the | 
					
						
							|  |  |  | moon; *SunAz* and *SunEl*, the azimuth and elevation of the Sun; | 
					
						
							|  |  |  | *Freq*, your stated operating frequency in MHz; *Tsky*, the estimated | 
					
						
							|  |  |  | sky background temperature in the direction of the moon, scaled to the | 
					
						
							|  |  |  | operating frequency; *Dpol*, the spatial polarization offset in | 
					
						
							|  |  |  | degrees; *MNR*, the maximum non-reciprocity of the EME path in dB, | 
					
						
							|  |  |  | owing to a combination of Faraday rotation and spatial polarization; | 
					
						
							|  |  |  | and finally *Dgrd*, an estimate of the signal degradation in dB, | 
					
						
							|  |  |  | relative to the best possible time with the moon at perigee in a cold | 
					
						
							|  |  |  | part of the sky. | 
					
						
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							|  |  |  | On the higher microwave bands, where Faraday rotation is minimal and | 
					
						
							|  |  |  | linear polarization is often used, spatial offset will reduce signal | 
					
						
							|  |  |  | levels.  Some stations have implemented mechanical polarisation | 
					
						
							|  |  |  | adjustment to overcome this loss, and the amount of rotation needed is | 
					
						
							|  |  |  | predicted in real time by the value of *Dpol*.  Positive Dpol means | 
					
						
							|  |  |  | that the antenna should be rotated in a clockwise direction looking | 
					
						
							|  |  |  | from behind the antenna towards the moon.  For a dish antenna, the | 
					
						
							|  |  |  | feed should similarly be rotated clockwise looking into the mouth of | 
					
						
							|  |  |  | the feed. A negative value for Dpol means anticlockwise rotation. | 
					
						
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							|  |  |  | The state of the art for establishing three-dimensional locations of | 
					
						
							|  |  |  | the sun, moon, and planets at a specified time is embodied in a | 
					
						
							|  |  |  | numerical model of the solar system maintained at the Jet Propulsion | 
					
						
							|  |  |  | Laboratory. The model has been numerically integrated to produce | 
					
						
							|  |  |  | tabular data that can be interpolated with very high accuracy. For | 
					
						
							|  |  |  | example, the celestial coordinates of the moon or a planet can be | 
					
						
							|  |  |  | determined at a specified time to within about 0.0000003 degrees. The | 
					
						
							|  |  |  | JPL ephemeris tables and interpolation routines have been incorporated | 
					
						
							|  |  |  | into _WSJT-X_.  Further details on accuracy, especially concerning | 
					
						
							|  |  |  | calculated EME Doppler shifts, are described in {lunarEchoes} for | 
					
						
							|  |  |  | November-December, 2016. | 
					
						
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							|  |  |  | The sky background temperatures reported by _WSJT-X_ are derived from | 
					
						
							|  |  |  | the all-sky 408 MHz map of Haslam et al. (Astronomy and Astrophysics | 
					
						
							|  |  |  | Supplement Series, 47, 1, 1982), scaled by frequency to the -2.6 | 
					
						
							|  |  |  | power. This map has angular resolution of about 1 degree, and of | 
					
						
							|  |  |  | course most amateur EME antennas have much broader beamwidths than | 
					
						
							|  |  |  | this. Your antenna will therefore smooth out the hot spots | 
					
						
							|  |  |  | considerably, and the observed extremes of sky temperature will be | 
					
						
							|  |  |  | less. Unless you understand your sidelobes and ground reflections | 
					
						
							|  |  |  | extremely well, it is unlikely that more accurate sky temperatures | 
					
						
							|  |  |  | would be of much practical use. |