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 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 ...
Page 116
This is then compared with the reference waveform , and the difference , the error
signal , is amplified and applied to the drive coil . This system is therefore a single
negative feedback loop in which the error signal not only corrects for ...
This is then compared with the reference waveform , and the difference , the error
signal , is amplified and applied to the drive coil . This system is therefore a single
negative feedback loop in which the error signal not only corrects for ...
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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