Atomic ratio

Atomic ratio

The atomic ratio is a measure of the ratio of atoms of one kind (i) to another kind (j). A closely related concept is the atomic percent (or at.%), which gives the percentage of one kind of atom relative to the total number of atoms. The molecular equivalents of these concepts are the molar fraction, or molar percent.

Contents

Atoms

Mathematically, the atomic percent is (There is a problem here - there is no 100, therefore this is a fraction and not a percent. TT)

 \mathrm{atomic \ percent} \ (\mathrm{i}) = \frac{N_\mathrm{i}}{N_\mathrm{tot}} \ ,

where Ni are the number of atoms of interest and Ntot are the total number of atoms, while the atomic ratio is

 \mathrm{atomic \ ratio} \ (\mathrm{i:j}) = \mathrm{atomic \ percent} \ (\mathrm{i}) : \mathrm{atomic \ percent} \ (\mathrm{j}) \ .

For example, the atomic percent of hydrogen in water (H2O) is at.%H2O = 2/3 ≈ 66.67%, while the atomic ratio of hydrogen to oxygen is AH:O = 2:1.

Isotopes

Another application is in radiochemistry, where this may refer to isotopic ratios or isotopic abundances. Mathematically, the atomic percent is (see comment above)

 \mathrm{isotopic \ abundance} \ (\mathrm{i}) = \frac{N_\mathrm{i}}{N_\mathrm{tot}} \ ,

where Ni are the number of atoms of the isotope of interest and Ntot is the total number of atoms, while the atomic ratio is

 \mathrm{isotopic \ ratio} \ (\mathrm{i:j}) = \mathrm{isotopic \ percent} \ (\mathrm{i}) : \mathrm{isotopic \ percent} \ (\mathrm{j}) \ .

For example, the isotopic ratio of deuterium (D) to hydrogen in Heavy water is roughly D:H = 1:7000 (corresponding to an isotopic abundance of 0.00014%).

Doping in laser physics

In laser physics however, the atomic ratio may refer to the doping ratio or the doping fraction.

\mathrm{doping \ fraction} = \frac{N_\mathrm{atoms \ of \ dopant}}{N_\mathrm{atoms \ of \ solution \ which \  can \ be \ substituted \ with \ the \ dopant}}

For example, a 100% doped Yb:Y3Al5O12 is pure Yb3Al5O12. The ambiguity of this term can lead to confusion.

See also


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