Treatise on Materials Science and Technology, Volume 1 |
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Page 105
Dependence of minimum length of bundle on flaw distribution exponent m for
condition of equal strength for composite and bundle . would be a certain length ,
however , where the strength of the bundle is equal to the strength of the ...
Dependence of minimum length of bundle on flaw distribution exponent m for
condition of equal strength for composite and bundle . would be a certain length ,
however , where the strength of the bundle is equal to the strength of the ...
Page 286
A . Local Displacement Equations Consider the element of length of aaß triple
line shown in Fig . B - 1 . When the triple line moves along the ad boundary , this
element ( a ) sweeps through an area 8 ( DS ) ; and ( b ) changes its length S ( DL
) ...
A . Local Displacement Equations Consider the element of length of aaß triple
line shown in Fig . B - 1 . When the triple line moves along the ad boundary , this
element ( a ) sweeps through an area 8 ( DS ) ; and ( b ) changes its length S ( DL
) ...
Page 287
THE CHANGE IN LINE LENGTH The length of the element dL before its
displacement may be expressed in terms of its local curvature and the angle
subtended by its normals , see Fig . B - 1b : dL = rdo After displacement , its
length is dL + 8 ...
THE CHANGE IN LINE LENGTH The length of the element dL before its
displacement may be expressed in terms of its local curvature and the angle
subtended by its normals , see Fig . B - 1b : dL = rdo After displacement , its
length is dL + 8 ...
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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