Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 29
002° 20 or + 0 . 002° 20 - 0 . 0088° 20 or + 0 . 0088° 20 - 0 . 0068° 20 or + 0 .
0068° 20 - axis displacement , Ax ' = + 0 . 025 mm Maximum total errors ( a ) in -
20 direction ( b ) in + 20 direction Maximum error in stress for steel - 0 . 008° 20 +
0 .
002° 20 or + 0 . 002° 20 - 0 . 0088° 20 or + 0 . 0088° 20 - 0 . 0068° 20 or + 0 .
0068° 20 - axis displacement , Ax ' = + 0 . 025 mm Maximum total errors ( a ) in -
20 direction ( b ) in + 20 direction Maximum error in stress for steel - 0 . 008° 20 +
0 .
Page 30
method yields } the error as in parafocusing in the range of 20 , appropriate for
stress measurements of steel with CrKą radiation ( 20 = 156° ) . This is another
factor favoring the stationary slit method . A defocusing error exists when using a
...
method yields } the error as in parafocusing in the range of 20 , appropriate for
stress measurements of steel with CrKą radiation ( 20 = 156° ) . This is another
factor favoring the stationary slit method . A defocusing error exists when using a
...
Page 93
Consequently , the largest potential TDS error should be associated with the (
222 ) - ( 444 ) pair , while the smallest should be for the ( 222 ) - ( 333 ) pair . Both
sets of data fit the solid ( average ) curve of Fig . 15 equally well , and one must ...
Consequently , the largest potential TDS error should be associated with the (
222 ) - ( 444 ) pair , while the smallest should be for the ( 222 ) - ( 333 ) pair . Both
sets of data fit the solid ( average ) curve of Fig . 15 equally well , and one must ...
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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