|  |  GeoAstro Applets |  Astronomy |  Chaos Game |  Java |  Miscel- laneous | 
|    Using the text fields for latitude and declination press "Apply input" after entering the values.  The
                        items "Derivative" of the Details menu are valid
                        for a single declination only.  The
                          "Draw/Write Time" button will open a diagram
                          showing the time of the prime vertical
                          passage. You also may enter the declination
                          and right ascension of a celestial body to be
                          observed. Press return key
                          after entering each value. δ=7.407° and RA=5.9195h are the coordinates of Betelgeuse (alpha Ori). The prime vertical
                      is a circle on the celestial sphere passing east
                      and west through the zenith, and intersecting the
                      horizon in its east and west points at right
                      angles. The altitude
                      and the angle of intersection when passing through
                      the prime vertical depends on the latitude of the
                      observer and on the declination of the celestial
                      body. Example:
                      eastern prime vertical (azimuth 90°): Latitude 
                      φ = 50°, declination of the body δ = 40° sin h90 = sin δ / sin
                    φ = sin 40°/sin 50° = 0.839,    h90 = 57.0° The hour angle ti when crossing the prime vertical: ti = (tan δ / tan φ)*180°/PI, ti = 270° + 40.3° = 310.3° On
                        the prime vertical the azimuth angle az
                        increases per minute by: 0.25° * sin φ = 0.192° and
                        the altitude angle h increases per minute by: 0.25° * cos φ = 0.161° The inversion
                      point of the path as a function of the hour angle
                      h=h(t)   is at
                      ti=270° at (azi=241.7° | hi=29.5°),
                      the slope (derivative dh/da) is 43.6°: sin hi
                        = sin φ * sin δ =
                        0.492,    hi
                        = 29.5° cos azi = sin δ * cos φ / cos hi = 0.475, azi = 241.7° The
                          inversion point of the path h=h(az)   is a
                          different one.  The
                          parallactic angle q ("angle at the star")
                        (*)   is zero
                          when the object crosses the meridian, and
                          largest when passing the point of inversion. On the prime vertical (az=90°, az=270°) we have the simple equation |dh/da|
                            = cot φ =
                              tan (90°-φ) The formula (*) can be derived using spherical astronomy and calculus:   The
                        body rises at an azimuth angle of az0=180°
                        (North): cos az0= - sin δ / cos φ = sin 40°/cos 50° =
                          1,    az0=180° The diurnal path crosses the horizon at an angle β: tan β = sin az0 / tan φ = 0 / tan φ = 0,    β=0°     Objects of declination δ > φ do not pass the prime vertical. Their diurnal path has a point of largest digression (LD) from the meridian where the motion is vertical (parallactic angle 90°). This happens at azimut azLD and hour angle tLD:  sin azLD = cos δ / cos φ cos tLD = tan φ / tan δ Example: φ = 50°, δ = 60°: azLD = 180°+51.1° = 231.1°, tLD = 360°-46.5° = 313.5°  This phenomenon of largest
                            digression can be used to determine the latitude
                            of the observer 
                            (W. Embacher).  51.62° N,
                                  7.96.0° E on 2011 Feb 13 at 21:50 UT:
                                  LST=119.04° Dubhe, UMa (δ=61.7°):
                              RA
                                  165.93°, alt.
h=62.1°,
                                az=229.8° t = LST - RA = -46.9° There is a (small) difference compared with tLD = arccos(tanφ/tanδ) = 47.2° azLD = arcsin(cos δ/cos φ) = 49.8° (+180° = 229.8°) As already mentioned, the angle between the tangent of the h(az) curve and the prime vertical is equal to the latitude φ of the observer. This method does not require the declination of the star or the time. Using the equation for the differential variation of the altitude h (q=parallactic angle):  and
                                        setting dδ=0 and
                                      dφ=0: dh =
                                          sin q cos δ 
                                          dt = cos φ 
                                          sin az dt On the prime
                                            vertical (sin az=1): cos  φ = dh/dtWithout a
                                            sextant or a theodolit the
                                            latitude φ can be
                                            determined by observing the
                                            shadow of a vertical gnomon
                                            (length L) pointing exactly
                                            west (or east) which happens
                                            for declination δ>=0° (March 21
                                            until September 23):   h2
                                              = arctan(L/x2),
                                          h1
                                              = arctan(L/x1), dh = h2
                                              - h1 =
                                              arctan(L/x2)
                                          - arctan(L/x1), Simulated example for the Sun: calculated by my Analemma applet, on 2011 June 1: at 7:07 x2= 1.745 m at 7:27 x1= 1.982 m dt = 20 min dh = 29,82° - 26.77° = 3.05° cos φ = dh/dt = 4min/° *
                                      3.05°/20 min = 0.610 φ = 52.4° Location
of
                                      calculation: Berlin φ =
                                        52.51° N (13.41° E)Date
                                      lines Berlin
                                  (52.51° N)  
 | 

More details:
Sun Azimuth at Rise and Set Applet
Applet: Azimuth, Latitude, Hour
              Angle, Declination 
      
|  | 
| The measurement by Prestel (using a
                  Prismenkreis) is accurate to 6''. | 
| Books, Articles | 
| Wilfried Kuhn (Hrsg.): Handbuch der
                  experimentellen Physik Sekundarbereich II, Band 11N:
                  Astronomie-Astrophysik-Kosmologie, Kapitel 2, Aulis
                  Verlag, 2011, ISBN 978-3761423967. William Chauvenet: A Manual of Spherical and
                  Practical Astronomy: Vol. I Spherical Astronomy,
                  Lippincott, Philadelphia 1891. Wilhelm Embacher: Neue Vorschläge zur
                  geographischen Ortsbestimmung, Österreichische
                  Zeitschrift für Vermessungswesen, 1952, Bd. 40, S.
                  3-88 (3 Teile). |