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Powder diffraction cone

Figure 2.31. The origin of the powder diffraction eone as the result of the infinite number of the completely randomly oriented identical reciprocal lattice vectors, d hki, forming a circle with their ends placed on the surface of the Ewald s sphere, thus producing the powder diffraction cone and the corresponding Debye ring on the flat screen (film or area detector). The detector is perpendicular to both the direction of the incident beam and cone axis, and the radius of the Debye ring in this geometry is proportional to tan20. Figure 2.31. The origin of the powder diffraction eone as the result of the infinite number of the completely randomly oriented identical reciprocal lattice vectors, d hki, forming a circle with their ends placed on the surface of the Ewald s sphere, thus producing the powder diffraction cone and the corresponding Debye ring on the flat screen (film or area detector). The detector is perpendicular to both the direction of the incident beam and cone axis, and the radius of the Debye ring in this geometry is proportional to tan20.
Figure 2.32. The schematic of the powder diffraction cones produced by a polycrystalline copper sample using Cu Ktti radiation. The differences in the relative intensities of various Bragg peaks (diffraction cones) are not discriminated, and they may be found in Table 2.6. Each cone is marked with the corresponding triplet of Miller indices. Figure 2.32. The schematic of the powder diffraction cones produced by a polycrystalline copper sample using Cu Ktti radiation. The differences in the relative intensities of various Bragg peaks (diffraction cones) are not discriminated, and they may be found in Table 2.6. Each cone is marked with the corresponding triplet of Miller indices.
FIGURE 2.4 (a) Cones produced by a powder diffraction experiment (b) experimental arrangement for a Debye-Scherrer photograph. [Pg.96]

Assuming that the diffracted intensity is distributed evenly around the base of each cone (see the postulations made above), there is usually no need to measure the intensity of the entire Debye ring. Hence, in a conventional powder diffraction experiment, the measurements are performed only along a narrow rectangle centered at the circumference of the equatorial plane of the Ewald s sphere, as shown in Figure 2.32 and indicated by the arc with an... [Pg.154]

Fig. 3-11 Formation of a diffracted cone of radiation in the powder method. Fig. 3-11 Formation of a diffracted cone of radiation in the powder method.
Datasqueeze Datasqueeze Program for analyzing 2D diffraction data, especially small angle and powder diffraction. Paul Heiney, pheiney datasqueezesoftware.com, PMB 252, 303 West Lancaster Ave., Wayne, PA 19087 3938 U.S.A. Available at http // WWW.datasqueezesoftware.com/. First release 2002, last update February 2005 Can integrate full 2D cones of diffraction... [Pg.504]

Figure 14.15. Typical x-ray powder diffraction pattern. The numbers represent opposite arcs of the same cone. A The instrumental arrangement. B The developed film strip. The radius of the film is r the S s are the distances between the arcs of a given cone. [Pg.414]

Figure 12. Diffraction cones in the crystalline powder method... Figure 12. Diffraction cones in the crystalline powder method...
XRD on battery materials can be classified as powder dififaction, a technique developed by Peter Debye and Paul Scherrer. In powder dififaction the material consists of microscopic crystals oriented at random in all directions. If one passes a monochromatic beam of X-rays through a fiat thin powder electrode, a fraction of the particles will be oriented to satisfy the Bragg relation for a given set of planes. Another group will be oriented so that the Bragg relationship is satisfied for another set of planes, and so on. In this method, cones of reflected and transmitted radiation are produced (Fig. 27.2). X-ray diffraction patterns can be recorded by intercepting a... [Pg.471]

Figure 8.28 Schematic diagram showing (a) diffraction from a single crystal, (b) from four crystals at different orientations with respect to the incident beam and (c) from a polycrystalline powder giving rise to a pattern of concentric cones of diffraction, often presented as a one-dimensional plot of intensity vs diffraction angle (reproduced by permission of The Royal Society of Chemistry). Figure 8.28 Schematic diagram showing (a) diffraction from a single crystal, (b) from four crystals at different orientations with respect to the incident beam and (c) from a polycrystalline powder giving rise to a pattern of concentric cones of diffraction, often presented as a one-dimensional plot of intensity vs diffraction angle (reproduced by permission of The Royal Society of Chemistry).
Figure 12.3 Illustration of the cones of diffraction produced by an X-ray beam striking a crystalline powder sample (reproduced with permission). Figure 12.3 Illustration of the cones of diffraction produced by an X-ray beam striking a crystalline powder sample (reproduced with permission).
Figure 7 (a) Bragg reflection from a set of lattice planes, (b) The cone of diffracted X-rays from a powder specimen. The cone contains all X-rays reflected from one particular family of lattice planes in all crystals which are correctly oriented, (c) The form of a powder pattern (asymmetric film mounting)... [Pg.6412]


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See also in sourсe #XX -- [ Pg.153 , Pg.155 ]




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Powder diffraction

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