BRAGG DIFFRACTION FROM A MATERIAL OF CIRCULAR CROSS SECTIONdifference between Laue-case and Bragg-case diffraction. Rays affected by the Bragg surface give rise to a high-intensity region on dark-field profiles. The profiles of this peak are not well predicted by an approximate Green-function method based on truncated planar Bragg surfaces. As d increases so as to be much greater than about ~1, the Bragg peak begins to consist of several narrowly-spaced fringes contained within a broad envelope.There is some experimental evidence for the presence of such Bragg peaks on X-ray topographs of cylindrical crystals (see e.g. Saldin & Buckley-Golder, 1977). In the instance cited above the diameter was of the order of a hundred extinction distances. The narrow Bragg fringes expected were smeared out to form a wide highintensity region near FI on the photographs in this case since they were projection (or traverse) topographs. One method of computing the form of such peaks would be by means of an extension of our calculations and the use of the reciprocity theorem (Kato, 1968