Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 67
( a ) Cu Nicu - ( 200 ) ( 220 ) As - Plated 2 MIN 4 MIN RELATIVE INTENSITY - 10
MIN 45 MIN 66 67 68 69 78 79 80 81 82 27 128 129 130 131 132 133 134 135
28 , DEGREES ( b ) cu Ni Cu Nicu Ni | ( II ) | | ( 200 ) | . . ( 220 ) AS - PLATED - 4 ...
( a ) Cu Nicu - ( 200 ) ( 220 ) As - Plated 2 MIN 4 MIN RELATIVE INTENSITY - 10
MIN 45 MIN 66 67 68 69 78 79 80 81 82 27 128 129 130 131 132 133 134 135
28 , DEGREES ( b ) cu Ni Cu Nicu Ni | ( II ) | | ( 200 ) | . . ( 220 ) AS - PLATED - 4 ...
Page 133
It is possible to measure the nitride layer thickness layer accurately up to
thicknesses of about 30 um in this way , by initially determining the relative nitride
, austenite , and ferrite contributions for standard nitride layers of known thickness
...
It is possible to measure the nitride layer thickness layer accurately up to
thicknesses of about 30 um in this way , by initially determining the relative nitride
, austenite , and ferrite contributions for standard nitride layers of known thickness
...
Page 143
The relative amount of each phase can usually be determined from the
appropriate relative area . For thin absorbers the relative area due to a given
phase is proportional to the product of the areal density of Mössbauer atoms in
that phase ...
The relative amount of each phase can usually be determined from the
appropriate relative area . For thin absorbers the relative area due to a given
phase is proportional to the product of the areal density of Mössbauer atoms in
that phase ...
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Contents
R JAMES | 2 |
Principles of XRay Stress Measurement | 4 |
Control of Accuracy and Precision | 25 |
Copyright | |
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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