1/l=a(Z -b)^2For example, the copper-Ka 1 line has a wavelength of 0.154 nm, and Z =29,
whereas for nickel the values are 0.166 nm and 28.
The absorption of X-rays must be considered, since certain elements may act
as filters for removing components of the X-ray spectrum, and also the sample
itself will absorb. The absorption of X-rays depends upon the thickness of pene-
tration into the target and a mass absorption coefficient determined by the
atomic number of the element and the wavelength of the X-rays. However, the
absorption does not follow a smooth curve, but shows a series of absorption
edgeswhich appear when the ionization energy for a K, L or M electron is
reached. This happens because more energy is absorbed in exciting the electrons
in the target. For nickel, the edge occurs at 0.148 nm, which means that a nickel
filter will absorb the copper Kblines, around 0.139 nm, strongly, but absorb the
copper Kalines at 0.154 nm very little. This is shown in Figure 1(c). In a complex
matrix, all the elements will contribute to the absorption.Instrumentation Two major types of instrumentation are used for X-ray emission spectrometry.
These are illustrated in Figures 2(a)and (b).
In a dispersive instrument, the specimen is the target for bombardment by
high energy X-rays from the source, generally an X-ray tube containing a target
such as tungsten, onto which electrons are accelerated by a 50 kV potential
difference. These primary X-rays excite the specimen to produce X-rays
E6 – X-ray emission spectrometry 215
hn or e–
- – –
- ––
- –
- –
- –
+ M'hole'KLM
KL
- – –
- ––
- –
- –
- –
e– +(a) (b) hnFig. 1. (a) Excitation of an atom. (b) Relaxation and fluorescent emission of X-rays. (c) X-ray
emission spectrum of copper (full line) plus the X-ray absorption for nickel (dashed line).Intensity0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16 0.18
Wavelength (nm)(c)