
By comparing two photographs taken exactly six months apart the angle of parallax (p) can be determined in arc-seconds. Hence the distance to the star can be found as d in parsec.
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The apparent magnitude of any star (m) can be related to its apparent brightness (B) by Pogson’s equation, where k is an experimental benchmark.

Brightness reduces with distance as an inverse square of distance. Thus brightness of an object as observed from two distances r1 & r2 is as shown in the formula.

Absolute magnitude is defined as the magnitude of the object when it is observed from a distance of 10 parsec. Using the 1/r2 relationship we get the above. Absolute magnitude can also be determined by measuring the parallax of the object.

The LHS is called as the distance modulus. If m is measured and M is determined by astrophysical reasoning, then distance D can be found in parsec.

The earth’s atmosphere as well as the intervening medium between stars or galaxies (usually called the Inter-stellar medium), dim the starlight by absorbing it. Hence the magnitude measurements have to be corrected by a certain factor A for each absorption. AISM is determined experimentally by observing many stars with similar M (judged on the basis of their physical properties) and correlating their magnitudes. Aatmosphere can be determined by measuring the magnitude of the same star at various points in the sky, since the density of the layers of the atmosphere and the distance through which starlight travels in the atmosphere, play a role here. a is the extinction coefficient for the medium which makes up the atmosphere.

Luminosity of a star can be obtained by measuring the bolometric absolute magnitudes (measured by using instruments equally sensitive to all wavelengths) of the star and the sun. It is convenient to express luminosities with respect to solar luminosity (3.79 x 1026 J/s). By Stefan’s law the energy density of a star having effective spectral temperature Teff is given as
. Thus Luminosity, which is the net energy given by the entire surface is
. The energy density received from the star at a distance r is
,
where
is the angular diameter of the star as viewed at a distance D. The energy density as measured above for the sun from the earth is called the solar constant. If we know the bolometric apparent magnitude of the star, its angular diameter and its effective temperature, we can use Pogson’s equation to obtain


Apparent brightness of a system of stars such as a cluster or a galaxy can be found by adding up the intrinsic brightness (luminosities) of the various components (stars). Hence, using Pogson’s equation one can calculate the magnitudes. It is often easier to express the brightness in terms of solar brightness.

HIP | Common name | mvis | Mvis | D (pc) | Spectral Type |
53020 | EE Leo or Wolf 358 | ??? | 12.89 | 5.6351 | M4: |
25878 | Wolf 1453 | 7.97 | ??? | 5.6909 | M1V |
26857 | Ross 47 | 11.56 | 12.75 | ??? | M5 |
86990 | 10.75 | 11.93 | 5.8113 | M5 |
Civilization | Planet | Star | mvis | Mvis | p (mas) |
Bellaris | Bellar | Bellatrix | 1.64 | -2.72 | |
Arcturamans | 3-Arcturi | Arcturus | -0.05 | 88.89 | |
429/25 | 429 | Fomalhaut | 1.17 | 1.74 | 130.03 |
Vegnolans | Vegnola | Vega | 0.03 | 0.58 |
Common Name | mvis | Mvis | D |
Shaula | 1.62 | -5.05 | 215.52 |
El Nath | 1.65 | -1.37 | 40.18 |
Alnilam | 1.69 | -6.38 | 411.52 |
Al Nair | 1.73 | -0.73 | 31.09 |
Alnitak | 1.74 | -5.26 | 250.63 |
Alsuhail | 1.75 | -5.31 | 257.73 |