Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 3
... Macroscopic over the sample over several grains 2nd ( um ) Microscopic over
grains Peak shift and peak broadening ... screw dislocation within ( 1 - 1 000 Å )
within grains 3rd Peak broadening а grain a Adapted from Buck and Thompson ...
... Macroscopic over the sample over several grains 2nd ( um ) Microscopic over
grains Peak shift and peak broadening ... screw dislocation within ( 1 - 1 000 Å )
within grains 3rd Peak broadening а grain a Adapted from Buck and Thompson ...
Page 245
PURE METALS Both pure Cu and pure Ni formed highly twinned , columnar
grain structures when deposited at low temperatures ( Dahlgren , 1974 ; Wang
and Dahlgren , 1975 ; Dahlgren et al . , 1977 ) . Grain sizes were so fine ( < 1000
Å ) ...
PURE METALS Both pure Cu and pure Ni formed highly twinned , columnar
grain structures when deposited at low temperatures ( Dahlgren , 1974 ; Wang
and Dahlgren , 1975 ; Dahlgren et al . , 1977 ) . Grain sizes were so fine ( < 1000
Å ) ...
Page 246
Heat treated amorphous Sm - Co alloys consisted of a magnetic compound
having exceptionally high coercivity due to its extremely small grain size . Finally ,
A - 15 phase superconducting compounds had high critical current capacities
due to ...
Heat treated amorphous Sm - Co alloys consisted of a magnetic compound
having exceptionally high coercivity due to its extremely small grain size . Finally ,
A - 15 phase superconducting compounds had high critical current capacities
due to ...
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Contents
R JAMES | 2 |
Principles of XRay Stress Measurement | 4 |
Control of Accuracy and Precision | 25 |
Copyright | |
15 other sections not shown
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absorption additional allows alloy angle Appl applications atoms bandgap beam broadening cause coefficients components composition composition profile concentration constant containing cooling crystal curve defects dependent deposits depth determined developed diffraction diffusion direction discussed dislocation distance distribution effect electron elements employed energy error et al example excitation experimental factor field function give given grain heat important included increasing intensity intensity bands iron laser lattice layer less magnetic material measurements Metals method Mössbauer observed obtained occur optical parameter peak phase Phys plane position possible powder problem produce range rays recent region relative residual stress sample semiconductors shift shown single Society solid spacing specimen spectra spectrum sputtering steel structure studies substrate surface target technique temperature term thickness values variation volume x-ray