Elements of X-ray DiffractionThis is a reproduction of a book published before 1923. This book may have occasional imperfections such as missing or blurred pages, poor pictures, errant marks, etc. that were either part of the original artifact, or were introduced by the scanning process. We believe this work is culturally important, and despite the imperfections, have elected to bring it back into print as part of our continuing commitment to the preservation of printed works worldwide. We appreciate your understanding of the imperfections in the preservation process, and hope you enjoy this valuable book. |
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Page 27
... radiation and a thickness range of 0.00 to 0.02 mm . 1-5 . Graphically verify Eq . ( 1-13 ) for a lead absorber and Mo Ka , Rh Ka , and Ag Ka radiation . ( The mass absorption coefficients of lead for these radiations are 141 , 95.8 ...
... radiation and a thickness range of 0.00 to 0.02 mm . 1-5 . Graphically verify Eq . ( 1-13 ) for a lead absorber and Mo Ka , Rh Ka , and Ag Ka radiation . ( The mass absorption coefficients of lead for these radiations are 141 , 95.8 ...
Page 166
... radiation . All in all , Cu Ka radiation is generally the most useful . It cannot be employed with ferrous materials , however , since it will cause fluorescent radiation from the iron in the specimen ; instead , Co Ka , Fe Ka or Cr Ka ...
... radiation . All in all , Cu Ka radiation is generally the most useful . It cannot be employed with ferrous materials , however , since it will cause fluorescent radiation from the iron in the specimen ; instead , Co Ka , Fe Ka or Cr Ka ...
Page 407
... radiation of this wavelength by air and the counter window . This factor limits the elements detectable by fluorescence to those with atomic numbers greater than about 22 ( titanium ) . Ti Ka radiation ( λ = 2.75A ) is de- creased to ...
... radiation of this wavelength by air and the counter window . This factor limits the elements detectable by fluorescence to those with atomic numbers greater than about 22 ( titanium ) . Ti Ka radiation ( λ = 2.75A ) is de- creased to ...
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Common terms and phrases
absorption coefficient absorption edge alloy analysis angle atomic number austenite axis back-reflection Bragg angle Bragg law Bravais lattice calculated camera chart circle composition constant copper atoms cos² counter cubic curve Debye ring Debye-Scherrer decreases determined diffracted beam diffraction lines diffraction pattern diffractometer direction distance electrons elements equation error example face-centered face-centered cubic factor film fluorescent fluorescent radiation given grain hexagonal incident beam indices integrated intensity lattice parameter Laue method martensite measured metal normal obtained Orthorhombic parallel percent phase photograph pinhole plotted pole figure position powder pattern preferred orientation projection reciprocal lattice reciprocal-lattice reflecting planes relative residual stress rhombohedral rotation sample scattering shown in Fig sin² slit solid solution spacing specimen spectrometer sphere spot stereographic substance surface temperature tetragonal thickness tion transmission unit cell values vector voltage wavelength x-ray diffraction x-ray method x-ray tube zero zone