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MISCELLANEOUS FORMULAE
HOUR ANGLE
H = Theta - Delta
where H is the hour angle
Theta is sidereal time
Delta is right ascension
The Hour Angle is negative east of and positive west of the meridian (as
right ascension increases eastward).
BODE'S LAW
(4 + 3(2^n))/10 in AU at aphelion
where n is the serial order of the planets from the sun (Mercury's 2n =1,
Venus's n = 0, Earth's n = 1, asteroid belt = 3)
APPARENT ANGULAR SIZE OF AN OBJECT
Theta = (h/D)*k
where Theta is the object's apparent angular size in units corresponding to k
h is the linear height of the object in units corresponding to D
D is the distance of the object in units corresponding to h
Theta is the object's angular height (angle of view) in units
corresponding to k
k is a constant with a value of 57.3 for Theta in degrees, 3438 in
minutes of arc, 206265 for seconds of arc (the number of the
respective units in a radian)
A degree is the apparent size of an object whose distance is 57.3 times its
diameter. The formula holds for celestial or terrestrial objects. E.g.,
for the width of a quarter at arm's length: (57.3*25 mm)/700 mm = 2o.
Under ideal conditions, the human eye can resolve anything subtending more
than a 1' angle, i.e., see an object as an extended object or see a double
star as two stars rather than a single point of light, provided that the two
components are of nearly equal brightness. A more practical value would be
4'; 8' is an even more practical value for comfortable viewing. The best
earthbound telescopes are usually limited by atmospheric effects to objects
1" or larger (0.25" with excellent seeing) in apparent size (before
magnification). In theory, a telescope could see everything with a
magnification of 60x (1" magnified to 1').
LENGTH OF A METEOR TRAIL
h = (Theta*D)/57.3
where h is the linear height of the meteor in km
Theta is the object's apparent angular size in degrees
D is the distance of the object in km
GEOGRAPHIC DISTANCE
Geographic distance of one second of arc = 30 m * cos of the latitude
where cos(Latitude)=1 on lines of constant longitude
ESTIMATING ANGULAR DISTANCE
Penny, 4 km distant ....................................... 1"
Sun, Moon ................................................. 30'
(The Moon is approximately 400 times smaller in angular
diameter than the Sun, but is approximately 400 times
closer.)
Width of little finger at arm's length .................... 1o
Dime at arm's length ...................................... 1o
Quarter at arm's length ................................... 2.5o
Width of Orion's belt ..................................... 3o
Alpha Ursae Majoris (Dubhe) to Beta Ursae Majoris (Merak) 5o
(Height of Big Dipper's cup. These are the "pointer
stars" to Polaris.)
Alpha Geminorum (Castor) to Beta Geminorum (Pollux) ....... 5o
Width of fist at arm's length ............................. 10o
Alpha Ursae Majoris (Dubhe) to Delta Ursae Majoris (Megrez) 10o
(Width of Big Dipper's cup.)
Height of Orion ........................................... 16o
Length of palm at arm's length ............................ 18o
Width of thumb to little finger at arm's length ........... 20o
Alpha Ursae Majoris (Dubhe) to Eta Ursae Majoris (Alkaid) . 25o
(Length of Big Dipper.)
Alpha Ursae Majoris (Dubhe) to Alpha Ursae Minoris
(Polaris) ............................................. 27o
ESTIMATING MAGNITUDES
Big Dipper, from cup to handle
Alpha (Dubhe) 1.8
Beta (Merak) 2.4
Gamma (Phecda) 2.5
Delta (Megrez) 3.4
Epsilon (Alioth) 1.8
Zeta (Mizar) 2.2
Eta (Alkaid) 1.9
Little Dipper, from cup to handle
Beta (Kochab) 2.0
Gamma (Pherkad) 3.1
Eta 5.0
Zeta 4.3
Epsilon 4.4
Delta (Pherkard) 4.4
Alpha (Polaris) 2.0
RANGE OF USEFUL MAGNIFICATION OF A TELESCOPE
D = diameter of aperture in mm
Minimum useful magnification ............................... 0.13*D 0.2*D for better contrast
Best visual acuity ................................................. 0.25*D
Wide views ............................................................ 0.4*D
Lowest power to see all detail
(resolution of eye matches resolution of telescope) .....0.5*D
Planets, Messier objects, general viewing ................. 0.8*D
Normal high power, double stars .................. 1.2*D to 1.6*D
Maximum useful magnification ................................. 2.0*D
Close doubles ....................................................... 2.35*D
Sometimes useful for double stars ............................ 4.0*D
Limit imposed by atmospheric turbulance ..................... 500
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