Random layer lattice structures are considered which consist of layers arranged parallel and equidistant, but random in translation parallel to the layer, and rotation about the normal. We call a and b the axes in the layer, and c the axis normal to the layer. In this notation there will be crystalline reflections of type ($00l$), two-dimensional lattice reflections of type (hk), and no general reflections (hkl). Equations are developed for the intensity distribution in a two-dimensional powder reflection, and for the integrated intensity. Equations are also de-developed for the particle size in terms of the peak breadth, and for the displacement of the peak. The powder pattern of a heat treated carbon black is presented as an illustration of two-dimensional lattice reflections.
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Β. E. Warren (1941) studied this question.
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