|
|
GeoAstro Applets |
Astronomy |
Chaos Game |
Java |
Miscel- laneous |
Physics Quiz |
Who is Who ? |
|
Large version ![]() ![]() Using the text fields for latitude and declination press return key after entering each value. ![]() 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/dt
Without
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). |