In spectroscopy, absorbance (abbreviated as A) is a logarithmic value which describes the portion of a beam of light which does not pass through a sample. Whilst the name refers to the absorption of light, other interactions of light with a sample (reflection, scattering) may also contribute to attenuation of the beam passing through the sample. The term "internal absorbance" is sometimes used to describe beam attenuation caused by absorption, while "attenuance" or "experimental absorbance" can be used to emphasize that beam attenuation can be caused by other phenomena. separating it into a scattering coefficient <math>\mu _s</math> and an absorption coefficient obtaining

<math display="block">-\ln(T) = \ln \frac {I_0}{I_s} = (\mu_s + \mu_a) d\,.</math>

If the size of a detector is very small compared to the distance traveled by the light, any light that is scattered by a particle, either in the forward or backward direction, will not strike the detector. (Bouguer was studying astronomical phenomena, so this condition was met.) In such cases, a plot of <math>-\ln(T)</math> as a function of wavelength will yield a superposition of the effects of absorption and scattering. Because the absorption portion is more distinct and tends to ride on a background of the scatter portion, it is often used to identify and quantify the absorbing species. Consequently, this is often referred to as absorption spectroscopy, and the plotted quantity is called "absorbance", symbolized as Some disciplines by convention use decadic (base 10) absorbance rather than Napierian (natural) absorbance, resulting in <math>\Alpha_{10} = \mu_{10}d </math> (with the subscript 10 usually not shown).

Absorbance for non-scattering samples

Within a homogeneous medium such as a solution, there is no scattering. In this case, researched extensively by August Beer, the concentration of the absorbing species follows the same linear contribution to absorbance as the path-length. Additionally, the contributions of individual absorbing species are additive. This is a very favorable situation, and made absorbance an absorption metric far preferable to absorption fraction (absorptance). This is the case for which the term "absorbance" was first used.

A common expression of the Beer's law relates the attenuation of light in a material as where <math>\Alpha </math> is the absorbance; <math>\varepsilon </math> is the molar attenuation coefficient or absorptivity of the attenuating species; <math>\ell </math> is the optical path length; and <math>c </math> is the concentration of the attenuating species.

Absorbance for scattering samples

For samples which scatter light, absorbance is defined as "the negative logarithm of one minus absorptance (absorption fraction: <math>\alpha</math>) as measured on a uniform sample". For decadic absorbance, this may be symbolized as If a sample both transmits and remits light, and is not luminescent, the fraction of light absorbed remitted and transmitted add to 1: Note that and the formula may be written as For a sample which does not scatter, and yielding the formula for absorbance of a material discussed below.

Even though this absorbance function is very useful with scattering samples, the function does not have the same desirable characteristics as it does for non-scattering samples. There is, however, a property called absorbing power which may be estimated for these samples. The absorbing power of a single unit thickness of material making up a scattering sample is the same as the absorbance of the same thickness of the material in the absence of scatter.

Optics

In optics, absorbance or decadic absorbance is the common logarithm of the ratio of incident to radiant power through a material, and spectral absorbance or spectral decadic absorbance is the common logarithm of the ratio of incident to spectral radiant power through a material. Absorbance is dimensionless, and in particular is not a length, though it is a monotonically increasing function of path length, and approaches zero as the path length approaches zero.

Mathematical definitions

Absorbance of a material

The absorbance of a material, denoted , is given by

<math display="block">A = \log_{10} \frac{\Phi_\text{e}^\text{i{\Phi_\text{e}^\text{t = -\log_{10} T,</math>

where

  • <math display="inline">\Phi_\text{e}^\text{t}</math> is the radiant flux by that material,
  • <math display="inline">\Phi_\text{e}^\text{i}</math> is the radiant flux by that material, and
  • <math display="inline">T = \Phi_\text{e}^\text{t}/\Phi_\text{e}^\text{i}</math> is the transmittance of that material.

Absorbance is a dimensionless quantity. Nevertheless, the absorbance unit or AU is commonly used in ultraviolet–visible spectroscopy and its high-performance liquid chromatography applications, often in derived units such as the milli-absorbance unit (mAU) or milli-absorbance unit-minutes (mAU×min), a unit of absorbance integrated over time.

Absorbance is related to optical depth by

<math display="block">A = \frac{\tau}{\ln 10} = \tau \log_{10} e \,,</math>

where is the optical depth.

Spectral absorbance

Spectral absorbance in frequency and spectral absorbance in wavelength of a material, denoted and respectively, are given by

Relationship with attenuation

Attenuance

Absorbance is a number that measures the attenuation of the transmitted radiant power in a material. Attenuation can be caused by the physical process of "absorption", but also reflection, scattering, and other physical processes. Absorbance of a material is approximately equal to its attenuance when both the absorbance is much less than 1 and the emittance of that material (not to be confused with radiant exitance or emissivity) is much less than the absorbance. Indeed,

<math display="block">\Phi_\mathrm{e}^\mathrm{t} + \Phi_\mathrm{e}^\mathrm{att} = \Phi_\mathrm{e}^\mathrm{i} + \Phi_\mathrm{e}^\mathrm{e}\,,</math>

where

  • <math display="inline">\Phi_\mathrm{e}^\mathrm{t}</math> is the radiant power transmitted by that material,
  • <math display="inline">\Phi_\mathrm{e}^\mathrm{att}</math> is the radiant power attenuated by that material,
  • <math display="inline">\Phi_\mathrm{e}^\mathrm{i}</math> is the radiant power received by that material, and
  • <math display="inline">\Phi_\mathrm{e}^\mathrm{e}</math> is the radiant power emitted by that material.

This is equivalent to

<math display="block">T + \mathrm{ATT} = 1 + E\,,</math>

where

  • <math display="inline">T = \Phi_\mathrm{e}^\mathrm{t} / \Phi_\mathrm{e}^\mathrm{i}</math> is the transmittance of that material,
  • <math display="inline">\mathrm{ATT} = \Phi_\mathrm{e}^\mathrm{att} / \Phi_\mathrm{e}^\mathrm{i}</math> is the of that material,
  • <math display="inline">E = \Phi_\mathrm{e}^\mathrm{e} / \Phi_\mathrm{e}^\mathrm{i}</math> is the emittance of that material.

According to the Beer's law, , so

  • <math>\mathrm{ATT} = 1 - 10^{-A} + E \approx A \ln 10 + E, \quad \text{if}\ A \ll 1,</math>

and finally

  • <math>\mathrm{ATT} \approx A \ln 10, \quad \text{if}\ E \ll A.</math>

Attenuation coefficient

Absorbance of a material is also related to its decadic attenuation coefficient by

<math display="block">A = \int_0^l a(z)\, \mathrm{d}z\,,</math>

where

  • is the thickness of that material through which the light travels, and
  • is the decadic attenuation coefficient of that material at .

If a(z) is uniform along the path, the attenuation is said to be a linear attenuation, and the relation becomes

<math display="block">A = al.</math>

Sometimes the relation is given using the molar attenuation coefficient of the material, that is its attenuation coefficient divided by its molar concentration:

<math display="block">A = \int_0^l \varepsilon c(z)\, \mathrm{d}z\,,</math>

where

  • is the molar attenuation coefficient of that material, and
  • is the molar concentration of that material at .

If is uniform along the path, the relation becomes

<math display="block">A = \varepsilon cl\,.</math>

The use of the term "molar absorptivity" for molar attenuation coefficient is discouraged.

For quantitative purposes, absorbance is often measured on a sample solution held in a cuvette, where the solution is sufficiently dilute that the linear relationship of the Beer's law holds. The cuvette provides a known and consistent path length for the light beam passing through the sample.

Shade number

Some filters, notably welding glass, are rated by shade number (SN), which is 7/3 times the absorbance plus one:

<math display="block">\begin{align}

\mathrm{SN} &= \frac{7}{3} A + 1 \\

&= \frac{7}{3}(-\log_{10} T) + 1\,.

\end{align}</math>

For example, if the filter has 0.1% transmittance (0.001 transmittance, which is 3 absorbance units), its shade number would be 8.

See also

  • Absorptance
  • Tunable Diode Laser Absorption Spectroscopy (TDLAS)
  • Densitometry
  • Neutral density filter
  • Mathematical descriptions of opacity

References