Figure: A long-exposure image of the night sky looking toward Polaris from Ehrenbuerg, Germany
Image 1 Caption: The night sky looking toward Polaris in a long-exposure image from Ehrenbuerg, Bavaria, Germany.
Further explication:
Because it is so close to the NCP, Polaris is the Northern Hemisphere pole star of our historical period.
For Northern Hemisphere observers, it is always just hanging there at nearly the same place in the sky, but you can't see it during the daytime.
Note:
Credit and/or file tracking information follows to the divider line:
Earth rotation angular velocity = ω = 360 degrees per day
= 15 degrees per hour
= 15 arcminutes per minute ,
and therefore for δ significantly less than 90°
φ = Δt*( 15 arcminutes per minute )*cos(δ) in general.
= Δt*( 15 arcminutes per minute ) at the celestial equator.
= indeterminate by this formula for δ close to 90°.
Note, the time units are formally
sidereal times
(e.g., sidereal days, hours, minutes).
However, those are close enough to ordinary times for our purposes.
For example, one
sidereal day = 86164.0905 s
= 1 day - 4 m + 4.0905 s (on average)
and the other sidereal units scale with the sidereal day.
A sidereal day is a complete rotation relative to the
observable universe.
Images:
Local file: local link: sky_swirl_polaris_ehrenbuerg.html.
Image link: Wikipedia:
File:Sterneamwalberla2.jpg.
Image link: Itself.
Celestial sphere file:
sky_swirl_polaris_ehrenbuerg.html.