Treatise on Materials Science and Technology, Volume 1 |
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Page 90
( 8 ) At an applied stress o or less the probability Q ( o ) of fracture of an element
of length d , and width w , having a flaw density distribution & ( o ) = Com per unit
surface area is Qo ) = 1 – exp ( - woč ( o ) ) = 1 – exp ( - s ) where s has been ...
( 8 ) At an applied stress o or less the probability Q ( o ) of fracture of an element
of length d , and width w , having a flaw density distribution & ( o ) = Com per unit
surface area is Qo ) = 1 – exp ( - woč ( o ) ) = 1 – exp ( - s ) where s has been ...
Page 172
The distribution function for the other two waves is more or less constant with
respect to 0 ; the P2 waves do show a little accumulation near 0 = 0 . For most
angles of incidence the p , wave is polarized in a direction close to the fiber axis (
Figs .
The distribution function for the other two waves is more or less constant with
respect to 0 ; the P2 waves do show a little accumulation near 0 = 0 . For most
angles of incidence the p , wave is polarized in a direction close to the fiber axis (
Figs .
Page 208
7 kcal / mole which is less than the value of 20 . 8 kcal / mole for the Fe - C peak .
This result is explained in terms of a contraction of the lattice ( Wert , 1950 )
caused by the silicon atoms . As a result , the combination of a carbon atom with
a ...
7 kcal / mole which is less than the value of 20 . 8 kcal / mole for the Fe - C peak .
This result is explained in terms of a contraction of the lattice ( Wert , 1950 )
caused by the silicon atoms . As a result , the combination of a carbon atom with
a ...
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addition alloys analysis angle applied approach associated assumed atoms average becomes bond boundary calculated complex composite concentration consider constants contribution crystal curvature curve decrease defined dependence deposition determined developed direction discussed displacement distance distribution dynamical effect elastic electron elements energy equal equation exist experimental fibers force fracture function given gives grain grain boundaries Group growth growth path illustrated increase indicate interaction interface internal friction interstitial iron laminate lattice layer length material matrix measured mechanism metal microstructural molecules nitrogen normal nucleation observed obtained occur oxygen particles peak phase plane position possible potential present produce properties region reinforcing relaxation respectively shown in Fig shows single Snoek peak solid solution strain strength stress structure substitutional surface Table temperature tungsten unit values volume waves