quantity

column density

The number of particles in a column of unit area along the line of sight, measuring gas abundance.
6 related articles · 2 formulas

Description

Column density is a measure of how many particles are present in a column of unit cross-sectional area along a given line of sight. It is typically expressed in units of particles per square centimeter (cm⁻²) and is a fundamental quantity in astrophysics, where it quantifies the amount of gas or dust between an observer and a distant source. For example, the column density of hydrogen in the interstellar medium tells astronomers how much material lies along the path to a star, affecting the star's observed brightness and spectrum. Column density is distinct from volume density (particles per cubic centimeter) because it integrates along the line of sight, making it directly relevant to observations of absorption and emission.

History

The concept of column density has been used in astronomy since the early 20th century, particularly in studies of stellar atmospheres and interstellar absorption lines. It became a standard tool with the development of radio astronomy and ultraviolet spectroscopy in the mid-1900s.

How it works

To obtain column density, one integrates the volume density n(r) along the line of sight from the observer to the source: N = ∫ n(r) dr. In practice, astronomers infer column density from spectral line measurements—the strength of absorption or emission lines depends on the number of absorbing or emitting particles along the path. For instance, the hydrogen column density is often derived from the Lyman-alpha absorption line, and dust column density from infrared extinction maps.

In practice

Column density is used to map the distribution of gas in galaxies, to correct for extinction in astronomical observations, and to assess the shielding of molecular clouds from ultraviolet radiation, which affects star formation.

Fun fact

The column density of the Earth's atmosphere at sea level is about 10²⁵ molecules per square centimeter, which is why the sky is blue—Rayleigh scattering is efficient because the column is so thick.

Concept graph →

Formulas

$$N = \frac{4\pi S_\nu \Delta\nu Q(T_{\rm rot})}{A_{ul} \Omega h c g_u e^{-E_u/kT_{\rm rot}}}$$
Column density derived from rotational molecular line emission.
What is in the formula
Nvariablecolumn density — column density per square metre
S_νvariableline flux density — spectral flux density joule per square metre per second per he
Δνvariableline width — frequency interval hertz
Qvariablerotational partition function — partition function
T_rotvariablerotational temperature — temperature kelvin
A_ulvariableEinstein A coefficient — einstein a coefficient per second
Ωvariablesolid angle of source — solid angle steradian
hvariablePlanck constant — planck constant joule second
cvariablespeed of light — speed of light metre per second
g_uvariabledegeneracy of upper level — degeneracy
E_uvariableenergy of upper level — energy joule
kvariableBoltzmann constant — boltzmann constant joule per kelvin
$$N = \frac{EW}{f \lambda^2}$$
Column density relates to equivalent width in optically thin limit.
What is in the formula
Nvariablecolumn density — column density per square metre
EWvariableequivalent width — equivalent width metre
fvariableoscillator strength — oscillator strength
λvariablewavelength — wavelength metre

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