Logo Introduction

Course Material Index  Section Index  Next Page

Introduction

Quantitative Analysis versus Structure Analysis

In an earlier section, Diffraction II (as well as Assignment 3), a simplified formula was given, relating the intensity of a powder diffraction peak to a number of instrumental and crystallographic parameters:

Ihkl = c jPLA Fhkl2
On that occasion the intention was to obtain for each peak a value for the structure factor Fhkl, the ultimate goal being the determination of the atomic structure of the diffracting sample. It was a working assumption that only one diffracting phase was present. In quantitative analysis there is a marked change of emphasis, since in general the sample will contain more than one diffracting phase, but we are no longer interested in crystallographic structure determination. The relative concentrations of the phases present are usually denoted as wi (termed the weight fraction for phase i ), and the diffracted intensity equation must now be written as:
Ihkl = (wi / ρi ) c jPLA Fhkl2
where ρi is the density of phase i. The aim is now the elimination of all terms except wi. This is the essence of quantitative analysis - to be presented with an unknown powder sample, to collect its powder diffraction pattern, to identify the phases present, and to determine the weight fractions of each phase (i.e. wi, i = 1 to i = N) present. Historically this has been one of the most important applications of powder diffraction. For example, in the industrial context it can give information on the efficiency of a process or the purity of the product; in exploration industry it can give valuable information on mineral composition; in investigative science it provide an effective "fingerprint" enabling the source of material to be identified. However, it is true to say that in its fullness the literature on the subject has become complicated, even messy. This situation has arisen because the technique has been developed independently down many routes. The result is that the there are only a few enlightening reviews covering the whole field ("X-ray Powder Diffractometry" by Jenkins & Snyder comes closer than most). It would be beyond the scope of this section to rectify this defect; an introductory look at some typical problems and solutions is all that is promised!

It has been a common practice to use only one peak (or perhaps just a few peaks) of a powder pattern to represent the quantity of any one phase present. The main problem entailed by this approach is that with a heavy reliance on just one peak, effects such as preferred orientation can strongly distort the result. The method of whole pattern fitting is therefore preferable, though computationally more demanding. These considerations are the subject of the next three sub-sections.


Course Material Index  Section Index  Next Page
© Copyright 1997-2006.  Birkbeck College, University of London.
 
Author(s): Paul Barnes
Martin Vickers