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train:lectures:positionalastro [2024/03/18 12:49] – Roy Prouty | train:lectures:positionalastro [2024/03/18 16:10] (current) – Roy Prouty | ||
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- | The March Equinox is chosen to be the zero-point for the Equatorial Coordinate analogous to latitude -- the Right Ascension or RA. RA is measured eastward along the Celestial Equator starting at the March Equinox. | + | The March Equinox is chosen to be the zero-point for the Equatorial Coordinate analogous to latitude -- the Right Ascension or RA. RA($\alpha$) |
==Milankovitch Cycles== | ==Milankovitch Cycles== | ||
The specific location of the CNP/CSP/CEq do change over time in cycles known as {{https:// | The specific location of the CNP/CSP/CEq do change over time in cycles known as {{https:// | ||
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- | Declination is measured in degrees, minutes of arc and seconds of arc with $360^\circ$ if traversing any Great Circle containing the CNP and CSP. Right Ascension is measured in hours, minutes, and seconds with $24^h$ if traversing the full Celestial Equator. As we shall see, changes in RA correspond to different angular rotations of the Earth -- or different times of day! These units can be confusing. Minutes of arc (or arcminutes) are NOT the same as minutes of RA. Furthermore, | + | Declination is measured in degrees, minutes of arc and seconds of arc with $360^\circ$ if traversing any Great Circle containing the CNP and CSP. Right Ascension is measured in hours, minutes, and seconds with $24^h$ if traversing the full Celestial Equator. As we shall see, changes in $\alpha$ |
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- | ==== Reconciling | + | ==== Reconciling |
With this Equatorial Coordinate System, an observer | With this Equatorial Coordinate System, an observer | ||
[{{: | [{{: | ||
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+ | For an observer at a positive latitude, $\lambda$, r ($\lambda=~39^\circ$ for MD): | ||
+ | - the CNP will be located at $(ALT=\lambda^\circ, | ||
+ | - the CSP will never be above the local horizon (Why?) | ||
+ | - the CEq will intersect the local meridian at $(ALT=90^\circ - \lambda, AZ=180^\circ)$ | ||
+ | - Zenith will see changing RA, depending on the local time, but the $\delta$ will always be $\lambda^\circ$ | ||
+ | =====Stellarium Exercises===== | ||
+ | Using Stellarium, let’s all do the following together … | ||
+ | - Set location to Baltimore. Note the (lat, lon) | ||
+ | - Identify the Ecliptic | ||
+ | - Set the date to your birthday and tell me your “Sun sign” – ugh | ||
+ | - Explore Local Horizon Grid | ||
+ | - Find the Pole Star and find its (alt, az) – what should it be? | ||
+ | - Enable the Local Meridian | ||
+ | - Play time forward and watch star paths | ||
+ | - Explore Equatorial Grid | ||
+ | - Enable CEq | ||
+ | - Play time forward and watch star paths | ||
+ | - Set location to North Pole, South Pole, Equator, etc | ||
+ | - Determine (alt, az) of a star in Orion, determine (RA, DEC) | ||
+ | - Determine exact time (ET) of March Equinox | ||
+ | - Back in Baltimore, identify the set of stars that never set | ||
+ | - These stars comprise the Circumpolar Region of our Local Horizon | ||
+ | - How does this region change with latitude? | ||
+ | - With Local Meridian on over Equatorial Grid: Define Transits & Sidereal Time | ||
+ | - Look up current Sidereal Time: https:// | ||
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+ | ---- | ||
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+ | Written by Roy Prouty 20240318\\ | ||
+ | Reviewed by | ||