# Angular diameter distance

The **angular diameter distance** is a distance measure used in astronomy. It is defined in terms of an object's physical size, , and the angular size of the object as viewed from earth.

The angular diameter distance depends on the assumed cosmology of the universe. The angular diameter distance to an object at redshift, , is expressed in terms of the comoving distance, as:

Where is the FLRW coordinate defined as:

Where is the curvature density and is the value of the Hubble parameter today.

In the currently favoured geometric model of our Universe, the "angular diameter distance" of an object is a good approximation to the "real distance", i.e. the proper distance when the light left the object. Note that beyond a certain redshift, the angular diameter distance gets smaller with increasing redshift. In other words, an object "behind" another of the same size, beyond a certain redshift (roughly z=1.5), appears larger on the sky, and would therefore have a *smaller* "angular diameter distance".

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## Angular size redshift relationEdit

The **angular size redshift relation** describes the relation between the angular size observed on the sky of an object of given physical size, and the objects redshift from Earth (which is related to its distance, , from Earth). In a Euclidean geometry the relation between size on the sky and distance from Earth would simply be given by the equation:

where is the angular size of the object on the sky, is the size of the object and is the distance to the object. Where is small this approximates to:

.

However, in the ΛCDM model (the currently favored cosmology), the relation is more complicated. In this model, objects at redshifts greater than about 1.5 appear larger on the sky with increasing redshift.

This is related to the angular diameter distance, which is the distance an object is calculated to be at from and , assuming the Universe is Euclidean.

The actual relation between the angular-diameter distance, , and redshift is given below. is called the deceleration parameter and measures the deceleration of the expansion rate of the Universe; in the simplest models, corresponds to the case where the Universe will expand for ever, to closed models which will ultimately stop expanding and contract corresponds to the critical case – Universes which will just be able to expand to infinity without re-contracting.

The Mattig relation yields the angular-diameter distance as a function of redshift for a universe with Ω_{Λ} = 0.^{[1]}

## See alsoEdit

## ReferencesEdit

**^**An introduction to the science of cosmology, Chapter 6:2 by Derek J. Raine & Edwin George Thomas (2001)