Treatise on Materials Science and Technology, Volume 1 |
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Page 153
Once Fn are known , the distribution function F ( 0 ) can be constructed from Eq . (
99 ) . Thus we see that a measurement of E ( 0 ) can be used to derive the exact
distribution function of the fibers in the composite . As the Fourier coefficients ...
Once Fn are known , the distribution function F ( 0 ) can be constructed from Eq . (
99 ) . Thus we see that a measurement of E ( 0 ) can be used to derive the exact
distribution function of the fibers in the composite . As the Fourier coefficients ...
Page 267
THE FUNDAMENTAL RELATION GOVERNING SIZE DISTRIBUTION
EVOLUTION Let the size distribution of particles at any time t be expressed in
terms of the fractional frequency function f ( R , 1 ) , such that f ( R , t ) dR is the
fraction of ...
THE FUNDAMENTAL RELATION GOVERNING SIZE DISTRIBUTION
EVOLUTION Let the size distribution of particles at any time t be expressed in
terms of the fractional frequency function f ( R , 1 ) , such that f ( R , t ) dR is the
fraction of ...
Page 269
The size distribution may be reported as a fractional or number frequency
function , or as a cumulative distribution function . In the present application it will
be found most useful to plot the size distribution in terms of the Ny > ( R , t )
function ...
The size distribution may be reported as a fractional or number frequency
function , or as a cumulative distribution function . In the present application it will
be found most useful to plot the size distribution in terms of the Ny > ( R , t )
function ...
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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