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Bragg’s relation

This definition is associated with Bragg s relation A = 2b sin 6 where t> is the distance between crystalline planes. In what follows, we shall always adopt the convention (6.4.3), though certain experimentalists choose to express their results as the crystallographers do. [Pg.214]

From the wave-length A of X-rays measured with a ruled grating and the observed angles 6 at whidbi these same X-rays are reflected from a ciystal one can calculate by Bragg s relation A = 2 i sin 0 the value of d the grating space of the aystal. For caldte at 20 °C it is found that... [Pg.50]

Mandelshtam, 1926 Fabelinski, 1965 Kerker, 1969 Vuks, 1977). Then, Bragg s relation for the first diffreiction maximum (the second one is negligible due to the blurred... [Pg.153]

Of these five variables, only three do influence light scattering along a given direction 9 (say, z) since the two transversal components V (V and V,) do not comply with Bragg s relation (Equation 17) (see Figure 2.30). [Pg.162]

The key question regarding the structure of a thermoset/clay nanocomposite system is whether a true nanocomposite has formed or not. If not, the material is comparable to a conventional filled microcomposite. Generally, wide angle X-ray diffraction (WAXD) analysis and transmission electron microscopy (TEM) are used to elucidate the structure of a nanocomposite. Due to its easiness and availability, WAXD is most commonly used to establish the nanocomposite structure [30, 31]. By monitoring the position, shape, and intensity of the basal reflections from the distributed silicate layers, the nanocomposite structure (intercalated or exfoliated) may be identified. The X-ray technique is often applied to identify nanocomposite structures through Bragg s relation, which is given below ... [Pg.330]

But we have assumed that the X-ray has already satisfied the diffraction condition, i.e., Bragg s relation which is... [Pg.51]

The technique is based on Bragg s law, which describes the diffraction of a monochromatic x-ray beam impinging on a plane of atoms [38]. Parallel incident rays strike the crystal planes and are then diffracted at angles that are related to the spacings between planes of molecules in the lattice. [Pg.15]

Fig. 1.6 (a) Arrangement of X-ray source, sample, and detector, used in X-ray direction from powders, (b) Typical diffraction pattern, showing the X-ray scattering as a function of angle. (The notation 20 is conventionally used for the scattering angle, as this relates to the theoretical interpretation given in Fig. 1.7.) The different peaks in (b) come from crystals oriented at different angles, so as to satisfy Bragg s Law (eqn 1.10) for an appropriate set of atomic planes. Fig. 1.6 (a) Arrangement of X-ray source, sample, and detector, used in X-ray direction from powders, (b) Typical diffraction pattern, showing the X-ray scattering as a function of angle. (The notation 20 is conventionally used for the scattering angle, as this relates to the theoretical interpretation given in Fig. 1.7.) The different peaks in (b) come from crystals oriented at different angles, so as to satisfy Bragg s Law (eqn 1.10) for an appropriate set of atomic planes.
Bragg s law relates the diffraction angle 4 in a crystal with planes a distance d apart to the wavelength X and a... [Pg.124]

Unit cell dimensions are obtained from measurements of 29 values of several Bragg reflections for which the indices h, k, and I are known. Values of 26 are measured as accurately as possible, and, since the wavelength A. of the radiation used is known, a value of dhu may be found by Bragg s Law, Equation 3.2 (Chapter 3). The value of is related to the unit cell dimensions and, if 26 values are measured for several reflections, values of the unit cell dimensions may be derived. The selected group of reflections chosen to do these calculations should contain a distribution of Miller indices and they should have relatively high 29 values ... [Pg.258]

Equation 2.114 represents the algebraic formulation of the FriedeTs law, which states that the absolute values of structure amplitudes and intensities are identical but the phase angles have opposite signs for Bragg reflections related to one another by the center of inversion. In another formulation, it states that the reciprocal space is always centrosymmetric in the absence of the anomalous scattering because lF(h) = lF(h). Friedel s law is illustrated in Figure 2.57, left. [Pg.220]


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