Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
From inside the book
Results 1-3 of 26
Page 5
A change in the interplanar spacing Adhki will cause a corresponding change A0
in the Bragg angle of diffraction by the planes ( Bragg ' s law : 1 = 2d sin 0 , where
1 is the wavelength of the incident x rays ) . The strain Adld can be measured ...
A change in the interplanar spacing Adhki will cause a corresponding change A0
in the Bragg angle of diffraction by the planes ( Bragg ' s law : 1 = 2d sin 0 , where
1 is the wavelength of the incident x rays ) . The strain Adld can be measured ...
Page 9
3 ) , the corresponding tilt angles are y1 = ( B – n 1 ) and V2 = ( B + m2 ) . The
diffraction ring will be asymmetric if the interplanar spacings of the diffracting
crystallites are different as a result of residual strains . From Eq . ( 6 ) , an
equation ...
3 ) , the corresponding tilt angles are y1 = ( B – n 1 ) and V2 = ( B + m2 ) . The
diffraction ring will be asymmetric if the interplanar spacings of the diffracting
crystallites are different as a result of residual strains . From Eq . ( 6 ) , an
equation ...
Page 162
... unit volume ) at the surface inside the material and a the absorption coefficient .
The corresponding excess carrier profile can then be approximated as ( Smith ,
1964 ) U 0 [ ( Lpa + vs / up ) Apix ) * ( L 2q2 – 1 ) 1 1 + us / UD : ) - exp ( - ax ) ) ] ...
... unit volume ) at the surface inside the material and a the absorption coefficient .
The corresponding excess carrier profile can then be approximated as ( Smith ,
1964 ) U 0 [ ( Lpa + vs / up ) Apix ) * ( L 2q2 – 1 ) 1 1 + us / UD : ) - exp ( - ax ) ) ] ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
R JAMES | 2 |
Principles of XRay Stress Measurement | 4 |
Control of Accuracy and Precision | 25 |
Copyright | |
15 other sections not shown
Other editions - View all
Common terms and phrases
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