Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 8
then m ' ( 5b ) dy , v = o [ ( 1 + v ) / E ] Because several values of d pob are
determined , errors resulting from random ... When this holds true ( see Chapter 5
) , only two inclinations of the sample are necessary to determine the surface
stress .
then m ' ( 5b ) dy , v = o [ ( 1 + v ) / E ] Because several values of d pob are
determined , errors resulting from random ... When this holds true ( see Chapter 5
) , only two inclinations of the sample are necessary to determine the surface
stress .
Page 121
This model is frequently the sum of several Lorentzian lines whose number and
relative positions are determined by the number of phases present and by the
hyperfine interactions . The so - called best fit is that obtained by minimizing the
sum ...
This model is frequently the sum of several Lorentzian lines whose number and
relative positions are determined by the number of phases present and by the
hyperfine interactions . The so - called best fit is that obtained by minimizing the
sum ...
Page 143
A . Phase Determination As indicated in the discussion of CuFe alloys ( Section
IV , A ) , different phases are detected by their different hyperfine interactions .
The relative amount of each phase can usually be determined from the
appropriate ...
A . Phase Determination As indicated in the discussion of CuFe alloys ( Section
IV , A ) , different phases are detected by their different hyperfine interactions .
The relative amount of each phase can usually be determined from the
appropriate ...
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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