X-Ray Diffraction: A Practical ApproachIn this, the only book available to combine both theoretical and practical aspects of x-ray diffraction, the authors emphasize a "hands on" approach through experiments and examples based on actual laboratory data. Part I presents the basics of x-ray diffraction and explains its use in obtaining structural and chemical information. In Part II, eight experimental modules enable the students to gain an appreciation for what information can be obtained by x-ray diffraction and how to interpret it. Examples from all classes of materials -- metals, ceramics, semiconductors, and polymers -- are included. Diffraction patterns and Bragg angles are provided for students without diffractometers. 192 illustrations. |
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... . The Structure Factor . . 50 52 60 200 2.9 . Diffraction from Amorphous Materials Chapter 3. Practical Aspects of X - Ray Diffraction 3.1 . Geometry of an X - Ray Diffractometer • 63 3.2 . Components of an X - Ray Diffractometer 65 xi.
... . The Structure Factor . . 50 52 60 200 2.9 . Diffraction from Amorphous Materials Chapter 3. Practical Aspects of X - Ray Diffraction 3.1 . Geometry of an X - Ray Diffractometer • 63 3.2 . Components of an X - Ray Diffractometer 65 xi.
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A Practical Approach C. Suryanarayana, M. Grant Norton. 3.2 . Components of an X - Ray Diffractometer 65 3.2.1 . The X - Ray Source · 65 3.2.2 . The Specimen 66 3.2.3 . The Optics 68 3.2.4 . The Detector 72 3.3 . Examination of a ...
A Practical Approach C. Suryanarayana, M. Grant Norton. 3.2 . Components of an X - Ray Diffractometer 65 3.2.1 . The X - Ray Source · 65 3.2.2 . The Specimen 66 3.2.3 . The Optics 68 3.2.4 . The Detector 72 3.3 . Examination of a ...
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... components of a modern x - ray tube . Beryllium is used for the window because it is highly transparent to x - rays . duced . We don't normally use the continuous part of the x - ray spectrum unless we require a number of different ...
... components of a modern x - ray tube . Beryllium is used for the window because it is highly transparent to x - rays . duced . We don't normally use the continuous part of the x - ray spectrum unless we require a number of different ...
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... components . To determine the weighted average , we need to know not only the wavelengths of the resolved lines but also their relative intensities . The Ka , line is twice as strong ( intense ) as the Ka2 line , so it is given twice ...
... components . To determine the weighted average , we need to know not only the wavelengths of the resolved lines but also their relative intensities . The Ka , line is twice as strong ( intense ) as the Ka2 line , so it is given twice ...
Page 12
... components of the spectrum . The absorption edge , or , as it is also known , critical absorption wavelength represents an abrupt change in the absorption characteristics of x - rays of a particular wavelength by a material . For ...
... components of the spectrum . The absorption edge , or , as it is also known , critical absorption wavelength represents an abrupt change in the absorption characteristics of x - rays of a particular wavelength by a material . For ...
Contents
3 | |
21 | |
Practical Aspects of XRay Diffraction | 63 |
Cubic Structures | 94 |
Hexagonal Structures | 125 |
Precise Lattice Parameter Measurements | 153 |
Phase Diagram Determination | 167 |
Quantitative Analysis of Powder Mixtures | 223 |
Identification of an Unknown Specimen | 237 |
Appendixes | 251 |
Atomic and lonic Scattering Factors of Some Selected | 255 |
Physical Constants and Conversion Factors | 261 |
Index | 271 |
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Common terms and phrases
20 values absorption alloy aluminum amplitude ångstrom atomic scattering factor atoms per cell atoms per unit body-centered cubic Bragg angle Bragg's law Bravais lattice broadening close-packed components composition copper cos² crystal structure crystal systems crystallite CsCl cubic Bravais lattice detector determine diamond cubic diamond cubic structure diffracted beam electron energy equation example Experimental Module face-centered cubic face-centered cubic Bravais face-centering translations fcc structure grain hexagonal hkl a nm integrated intensity lattice parameter lattice parameter(s lattice point lattice strain metal Miller indices mixture NaCl structure obtained orthorhombic phase diagram point lattice polycrystalline powder quantum number radiation relative intensities shell shown in Fig silicon simple cubic sin² sin² 0 sin² sin² 0 values slits solid solution spacing structure factor Table Theta FIG Titanium unit cell unknown specimen wavelength x-ray diffraction pattern x-ray photon zinc blende