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Page 134
The agreement obtained here between observed and calculated intensities is
satisfactory . For example , lines 1 and 2 are observed to be of strong and
medium intensity , their respective calculated intensities being 10 and 4 . 6 .
Similar ...
The agreement obtained here between observed and calculated intensities is
satisfactory . For example , lines 1 and 2 are observed to be of strong and
medium intensity , their respective calculated intensities being 10 and 4 . 6 .
Similar ...
Page 322
Bernard Dennis Cullity. TABLE 10 - 6 2 5 Calculated intensity hkl Observed
intensity Na Cl structure ZnS structure 200 0 . 05 13 . 2 10 . 0 0 . 02 12 . 4 0 . 03
10 . 0 6 . 2 220 311 2 3 3 { ás 2 .0 . 007 1 . 7 222 400 331 420 3 . 5 1 . 7 0 . 01 4 .
6 2 .
Bernard Dennis Cullity. TABLE 10 - 6 2 5 Calculated intensity hkl Observed
intensity Na Cl structure ZnS structure 200 0 . 05 13 . 2 10 . 0 0 . 02 12 . 4 0 . 03
10 . 0 6 . 2 220 311 2 3 3 { ás 2 .0 . 007 1 . 7 222 400 331 420 3 . 5 1 . 7 0 . 01 4 .
6 2 .
Page 394
Calculated powder patterns of austenite and martensite , each containing 1 . 0
percent carbon . Co Ka radiation . In calculating the value of R for a particular
diffraction line , various factors should be kept in mind . The unit cell volume v is ...
Calculated powder patterns of austenite and martensite , each containing 1 . 0
percent carbon . Co Ka radiation . In calculating the value of R for a particular
diffraction line , various factors should be kept in mind . The unit cell volume v is ...
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User Review - ron_benson - LibraryThingExcellent reference book. Needs some updating in terms of advances in detector technology. Read full review
Contents
CHAPTER | 1 |
CHAPTER 2 | 29 |
THE DIRECTIONS OF DIFFRACTED BEAMS | 78 |
Copyright | |
16 other sections not shown
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Elements of X-ray Diffraction Bernard Dennis Cullity,Stuart R. Stock,Stuart R.. Stock Snippet view - 2001 |
Common terms and phrases
absorption alloy angle applied atoms axis Bragg calculated called camera cause circle composition consider constant contains copper corresponding counter counting crystal cubic curve decreases depends described determined diffracted beam diffraction lines diffractometer direction distance effect electrons elements energy equal equation error example factor Figure film fluorescent given gives grain hexagonal incident beam increases indices intensity involved kind known lattice Laue length located material means measured metal method normal observed obtained occur orientation origin parallel parameter particular pattern percent phase photograph planes pole position possible powder produced projection proportional radiation rays reciprocal reference reflection relation relative result rotation sample scattering shown in Fig shows simple single slit solid solution spacing specimen sphere strain stress structure substance surface temperature tion tube twin unit cell usually vector voltage wave wavelength x-ray zone