Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 45
The stresses measured with x rays include both macrostresses and
microstresses ( those averaged only over the size of the ... Thus when the entire
material is subjected to extensive plastic deformation , the x - ray method may
yield results ...
The stresses measured with x rays include both macrostresses and
microstresses ( those averaged only over the size of the ... Thus when the entire
material is subjected to extensive plastic deformation , the x - ray method may
yield results ...
Page 109
ray will be emitted with the full transition energy , the recoiless fraction , is
proportional to exp ( - ( x2 ) / 12 ) , where ( . ro ) ... In addition , normally only those
y rays may be used which arise from the decay of a low lying state to the ground
state .
ray will be emitted with the full transition energy , the recoiless fraction , is
proportional to exp ( - ( x2 ) / 12 ) , where ( . ro ) ... In addition , normally only those
y rays may be used which arise from the decay of a low lying state to the ground
state .
Page 118
4 keV y rays . Although the energy resolution ( 8E / E = 12 % ) is inferior to that of
a solid state detector such as Si ( Li ) , the proportional counter is inherently
simpler and hence easier to refurbish ; it normally has a larger sensitive area and
...
4 keV y rays . Although the energy resolution ( 8E / E = 12 % ) is inferior to that of
a solid state detector such as Si ( Li ) , the proportional counter is inherently
simpler and hence easier to refurbish ; it normally has a larger sensitive area and
...
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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