Treatise on Materials Science and Technology, Volume 1 |
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Page 77
Phys . 50 , 3977 . Bolling , G . F . , and Tiller , W . A . ( 1960 ) . J . Appl . Phys . 31 ,
1345 . Bolling , G . F . , and Tiller , W . A . ( 1961 ) . J . Appl . Phys . 32 , 2587 .
Bradshaw , F . J . , Gasper , M . E . , and Pearson , S . ( 1958 ) . J . Inst . Metals 87
...
Phys . 50 , 3977 . Bolling , G . F . , and Tiller , W . A . ( 1960 ) . J . Appl . Phys . 31 ,
1345 . Bolling , G . F . , and Tiller , W . A . ( 1961 ) . J . Appl . Phys . 32 , 2587 .
Bradshaw , F . J . , Gasper , M . E . , and Pearson , S . ( 1958 ) . J . Inst . Metals 87
...
Page 114
In “ Modern Composite Materials ” ( L . J . Broutman and R . H . Krock , eds . ) , pp
. 337 - 411 . Addison - Wesley , Reading , Massachusetts . Coleman , B . D . (
1957a ) . J . Appl . Phys . 28 , 1058 . Coleman , B . D . ( 1957b ) . J . Appl . Phys .
In “ Modern Composite Materials ” ( L . J . Broutman and R . H . Krock , eds . ) , pp
. 337 - 411 . Addison - Wesley , Reading , Massachusetts . Coleman , B . D . (
1957a ) . J . Appl . Phys . 28 , 1058 . Coleman , B . D . ( 1957b ) . J . Appl . Phys .
Page 177
J . Phys . D . 1 , 1039 . Heaton , M . D . ( 1970 ) . J . Phys . D . 3 , 672 . Hill , R . (
1964 ) , J . Mech . Phys . Solids 12 , 199 . Hill , R . ( 1965 ) , J . Mech . Phys .
Solids 13 , 189 . Kothari , L . S . , and Singwi , K . S . ( 1957 ) . Phys . Rev . 106 ,
230 .
J . Phys . D . 1 , 1039 . Heaton , M . D . ( 1970 ) . J . Phys . D . 3 , 672 . Hill , R . (
1964 ) , J . Mech . Phys . Solids 12 , 199 . Hill , R . ( 1965 ) , J . Mech . Phys .
Solids 13 , 189 . Kothari , L . S . , and Singwi , K . S . ( 1957 ) . Phys . Rev . 106 ,
230 .
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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