The distance modulus is a way of expressing Distance that is often used in astronomy. It describes distances on a logarithmic scale based on the astronomical magnitude system.
This definition is convenient because the observed brightness of a light source is related to its distance by the inverse square law (a source twice as far away appears one quarter as bright) and because brightnesses are usually expressed not directly, but in magnitudes.
Absolute magnitude is defined as the apparent magnitude of an object when seen at a distance of 10 . If a light source has flux when observed from a distance of parsecs, and flux when observed from a distance of 10 parsecs, the inverse-square law is then written like:
The magnitudes and flux are related by:
Substituting and rearranging, we get: which means that the apparent magnitude is the absolute magnitude plus the distance modulus.
Isolating from the equation , finds that the distance (or, the luminosity distance) in parsecs is given by
The uncertainty in the distance in parsecs () can be computed from the uncertainty in the distance modulus () using which is derived using standard error analysis.
The first ones are termed visual distance moduli and are denoted by , while the second ones are called true distance moduli and denoted by .
Visual distance moduli are computed by calculating the difference between the observed apparent magnitude and some theoretical estimate of the absolute magnitude. True distance moduli require a further theoretical step; that is, the estimation of the interstellar absorption coefficient.
Using distance moduli makes computing magnitudes easy. As for instance, a solar type star (M= 5) in the Andromeda Galaxy (DM= 24.4) would have an apparent magnitude (m) of 5 + 24.4 = 29.4, so it would be barely visible for the Hubble Space Telescope which has a limiting magnitude of about 30. Since it is apparent magnitudes which are actually measured at a telescope, many discussions about distances in astronomy are really discussions about the putative or derived absolute magnitudes of the distant objects being observed.
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