Treatise on Materials Science and Technology, Volume 1 |
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Page 24
DISTRIBUTION POTENTIAL This potential arises as a result of the redistribution
of charged particles that are soluble in both phases at the interface between the
phases . In metals , the prime example is the redistribution of free electrons ; a ...
DISTRIBUTION POTENTIAL This potential arises as a result of the redistribution
of charged particles that are soluble in both phases at the interface between the
phases . In metals , the prime example is the redistribution of free electrons ; a ...
Page 26
ADDITIONAL DEFINITIONS As briefly discussed earlier , for each phase one may
distinguish an inner or Galvani ... The Galvani potential of a phase cannot be
measured and even the Galvani potential difference between two phases is not ...
ADDITIONAL DEFINITIONS As briefly discussed earlier , for each phase one may
distinguish an inner or Galvani ... The Galvani potential of a phase cannot be
measured and even the Galvani potential difference between two phases is not ...
Page 28
13b , we note that the surface potential ( double layer jump ) x differs in sign for
the two phases so that the Volta potential difference will be different from the
Galvani potential difference ( A0G = du + 0 . ) . From this figure , we can also note
the ...
13b , we note that the surface potential ( double layer jump ) x differs in sign for
the two phases so that the Volta potential difference will be different from the
Galvani potential difference ( A0G = du + 0 . ) . From this figure , we can also note
the ...
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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