Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 18
so IT for the error in peak shift at two tilts in degrees 20 , is 360 sin e 8 ( 420 ) sp =
— A ( 16 ) RGC Rp sin ( + ) ) ? where Rp represents the distance from the sample
to the focus position ; it is given by ( Hilley et al . , 1971 ) cos [ 4s + ( 90 - 0 ) ...
so IT for the error in peak shift at two tilts in degrees 20 , is 360 sin e 8 ( 420 ) sp =
— A ( 16 ) RGC Rp sin ( + ) ) ? where Rp represents the distance from the sample
to the focus position ; it is given by ( Hilley et al . , 1971 ) cos [ 4s + ( 90 - 0 ) ...
Page 100
The xray sample was prepared with acid cut and polished single crystal
substrates , while the probe sample was ... An increase in density of high
diffusivity paths is expected in the probe sample , which is more typical of
samples used in ...
The xray sample was prepared with acid cut and polished single crystal
substrates , while the probe sample was ... An increase in density of high
diffusivity paths is expected in the probe sample , which is more typical of
samples used in ...
Page 157
much higher excitation intensities , and also provide a light beam which is much
easier to focus onto a well - defined area of the sample . Filtering of laser light
with narrow line filters is often necessary to reject background radiation from the ...
much higher excitation intensities , and also provide a light beam which is much
easier to focus onto a well - defined area of the sample . Filtering of laser light
with narrow line filters is often necessary to reject background radiation from the ...
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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