Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 228
First , however , there will be a brief analysis of the heat flow through a target . a .
Target Heat Flow . The flow of heat through a solid body is given by : Q = KAAT /
L , where Q is the amount of heat flow per unit time , A the cross sectional area of
...
First , however , there will be a brief analysis of the heat flow through a target . a .
Target Heat Flow . The flow of heat through a solid body is given by : Q = KAAT /
L , where Q is the amount of heat flow per unit time , A the cross sectional area of
...
Page 232
B . Substrates A significant heat load was experienced by the substrate during
high rate sputter deposition so that substrate cooling was required for all low
temperature deposits . The heat load did permit deposition at elevated
temperatures ...
B . Substrates A significant heat load was experienced by the substrate during
high rate sputter deposition so that substrate cooling was required for all low
temperature deposits . The heat load did permit deposition at elevated
temperatures ...
Page 246
Heat treated amorphous Sm - Co alloys consisted of a magnetic compound
having exceptionally high coercivity due to its extremely small grain size . Finally ,
A - 15 phase superconducting compounds had high critical current capacities
due to ...
Heat treated amorphous Sm - Co alloys consisted of a magnetic compound
having exceptionally high coercivity due to its extremely small grain size . Finally ,
A - 15 phase superconducting compounds had high critical current capacities
due to ...
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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