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Hour angle

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Coordinates used in the equatorial coordinate system
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The hour angle is indicated by an orange arrow on thecelestial equator plane. The arrow ends at thehour circle of an orange dot indicating theapparent place of anastronomical object on thecelestial sphere.

Inastronomy andcelestial navigation, thehour angle is thedihedral angle between themeridian plane (containingEarth's axis and thezenith) and thehour circle (containing Earth's axis and a given point of interest).[1]

It may be given in degrees, time, or rotations depending on the application.The angle may be expressed as negative east of the meridian plane and positive west of the meridian plane, or as positive westward from 0° to 360°. The angle may be measured in degrees or in time, with 24h = 360° exactly.Incelestial navigation, the convention is to measure in degrees westward from theprime meridian (Greenwich hour angle,GHA), from the local meridian (local hour angle,LHA) or from thefirst point of Aries (sidereal hour angle,SHA).

The hour angle is paired with thedeclination to fully specify the location of a point on thecelestial sphere in theequatorial coordinate system.[2]

Relation with right ascension

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As seen from above theEarth'snorth pole, a star's local hour angle (LHA) for an observer near New York (red dot). Also depicted are the star'sright ascension and Greenwich hour angle (GHA), thelocal mean sidereal time (LMST) andGreenwich mean sidereal time (GMST). The symbol ʏ identifies theMarch equinox direction.
Assuming in this example the day of the year is the March equinox so the sun lies in the direction of the grey arrow then this star will rise about midnight. Just after the observer reaches the green arrow dawn comes and overwhelms with light the visibility of the star about six hours before it sets on the western horizon. The Right Ascension of the star is about 18h

The local hour angle (LHA) of an object in the observer's sky isLHAobject=LSTαobject{\text{LHA}}_{\text{object}}={\text{LST}}-\alpha _{\text{object}}orLHAobject=GST+λobserverαobject{\text{LHA}}_{\text{object}}={\text{GST}}+\lambda _{\text{observer}}-\alpha _{\text{object}}where LHAobject is the local hour angle of the object, LST is thelocal sidereal time,αobject{\displaystyle \alpha _{\text{object}}} is the object'sright ascension, GST isGreenwich sidereal time andλobserver{\displaystyle \lambda _{\text{observer}}} is the observer'slongitude (positive east from theprime meridian).[3] These angles can be measured in time (24 hours to a circle) or in degrees (360 degrees to a circle)—one or the other, not both.

Negative hour angles (−180° < LHAobject < 0°) indicate the object is approaching the meridian, positive hour angles (0° < LHAobject < 180°) indicate the object is moving away from the meridian; an hour angle of zero means the object is on the meridian.

Right ascension is frequently given in sexagesimal hours-minutes-seconds format (HH:MM:SS) in astronomy, though may be given in decimal hours, sexagesimal degrees (DDD:MM:SS), or, decimal degrees.

Because the earth rotates 365.2564 times in a sidereal year whereas fixed stars appear to go around one time more, the hour angle of a fixed star increases by 366.2564/365.2564 (about 1.0027) per hour, or in other words it takes 59 minutes and 50.17 seconds for the hour angle to increase by one hour.

Solar hour angle

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See also:Sunrise equation

Observing the Sun from Earth, thesolar hour angle is an expression of time, expressed in angular measurement, usually degrees, fromsolar noon. At solar noon the hour angle is zero degrees, with the time before solar noon expressed as negative degrees, and the local time after solar noon expressed as positive degrees. For example, at 10:30 AM local apparent time the hour angle is −22.5° (15° per hour times 1.5 hours before noon).[4]

Length of solar day over the year

The solar hour angle increases on average by one hour per hour, but because of theequation of time this varies with time of year. In mid-September a solar day is about 22 seconds less than 24 hours, meaning that the solar hour angle increases by 1.00025 hours per hour, whereas in late December a solar day is about 28 seconds more than 24 hours, so the solar hour angle increases by 0.99968 hours per hour.

Thecosine of the hour angle (cos(h)) is used to calculate thesolar zenith angle. At solar noon,h = 0.000 socos(h) = 1, and before and after solar noon the cos(± h) term = the same value for morning (negative hour angle) or afternoon (positive hour angle), so that the Sun is at the same altitude in the sky at 11:00AM and 1:00PM solar time.[5]

Sidereal hour angle

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The sidereal hour angle (SHA) of a body on the celestial sphere is its angular distance west of theMarch equinox generally measured in degrees. The SHA of a star varies by less than a minute of arc per year, due toprecession, while the SHA of a planet varies significantly from night to night. SHA is often used incelestial navigation and navigational astronomy, and values are published in nauticalalmanacs.[citation needed]

See also

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Notes and references

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  1. ^U.S. Naval Observatory Nautical Almanac Office (1992). P. Kenneth Seidelmann (ed.).Explanatory Supplement to the Astronomical Almanac.Mill Valley, CA: University Science Books. p. 729.ISBN 0-935702-68-7.
  2. ^Explanatory Supplement (1992), p. 724.
  3. ^Meeus, Jean (1991).Astronomical Algorithms. Bell, Inc., Richmond, VA. p. 88.ISBN 0-943396-35-2.
  4. ^Kreider, J. F. (2007). "Solar Energy Applications".Environmentally Conscious Alternative Energy Production. pp. 13–92.doi:10.1002/9780470209738.ch2.ISBN 9780470209738.
  5. ^Schowengerdt, R. A. (2007). "Optical radiation models".Remote Sensing. pp. 45–88.doi:10.1016/B978-012369407-2/50005-X.ISBN 9780123694072.
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