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The Basic Mathematics Of The Stellar Magnitude Ranking System
Stellar magnitude 3 is fainter than magnitude 1, which may seem odd at first glance. This is because stellar brightness is generally measured in units referred to as magnitudes, which are analogous to ranks.
1st magnitude is to 3rd magnitude as 1st prize is to 3rd prize. This is why magnitude 1 is brighter than magnitude 3 and magnitude 0 is even brighter than magnitude 1 and magnitude −1 is even brighter yet!
Given a set of stellar magnitudes, the object with the greatest numerical value is always the faintest of the set and the lowest numerical value indicates the brighest object. Negative magnitudes always indicate very bright objects, for example, sun at -26.74, the full moon at -12.5, or Venus at -4.5, etc. An asteroid may have a magnitude such as +10, which is very faint and Pluto even fainter at magnitude +14, which is extremely faint. For comparison, the star Vega (alpha Lyrae) is often cited as a general example of a star of 0 (zero) magnitude.
Here, the distances to the stars can be ignored. We do not need to think about the distances when simply ranking stars by their relative apparent brightness in the sky as we see them from Earth. However, when we start to move around in space or compare stars to each other, as if side-by-side, then we will have to take into account their distances too.
The stellar magnitude system is designed mathematically so that a difference of exactly 5 magnitudes equates to an apparent brightness ratio (b) of exactly 100-fold. It is a base-10 logarithmic system of astronomical brightness scaling analogous to the Richter or decibel scales used to measure energy intensity.
The general relationship between apparent difference in magnitude vs apparent ratio in brightness may be expressed by the simple equation
Eq. 1
Apparent Magnitude With Respect to Distance
Having shown the general relationship between apparent magnitude and brightness above, we can now proceed to the next step and add distance to the problem. Using the following equations, we can mathematically move a star around in space and compute its apparent brightness at any given distance from any given known starting values.
This also allows us to mathematically compare the relative brightness of any two stars side-by-side at any common distance. For example, how bright a star would our sun appear to be if viewed from the same distance as Alpha Centauri? Or how bright would Alpha Centauri appear to be at the distance of our sun?
The relationship between apparent magnitude and distance may be expressed in terms of any of the four variables as in the following equations. Although it may not be obvious at first glance, the following equations express the inverse square law of light intensity vs. distance from the light source in a logarithmic form.
Let:
m1 = Apparent magnitude of an astronomical body at distance d1
m2 = Apparent magnitude of the same astronomical body at distance d2
Distances (d1 and d2) can be expressed in any convenient, consistent units, such as astronomical units, light years, etc.
A Randomized Numerical Example: Computing the Brightness Ratio Between Two Objects
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Eq. 1
Given the apparent magnitudes of two astronomical objects
( m1 and m2),
Equation 1 computes their comparative brightness ratio ( b).
Let:
k = 2.5118864315095801 = 5th root of 100
m1 = -3.550 = Magnitude of brighter object
and
m2 = +3.417 = Magnitude of fainter object
The brightness ratio (b) between the brighter and fainter object can be found by:
m1 = -3.550 = Brighter Object
m2 = +3.417 = Fainter Object
dm = m2 − m1
= (+3.417) − (-3.550)
= 6.967
b = k ^ dm
= 2.5118864315095801 ^ 6.967
= 612.068
This means that an object with magnitude -3.550 is about 612.1 times brighter than an object of +3.417 magnitude.
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