Glass, Volume 1 |
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Page 142
+ n22 where E , is the uniform field in the absence of the minor phase particle . In
the derivation of this equation , it is assumed that the polarization of one particle
is not influenced by the polarization of other particles . In reality , the polarization
...
+ n22 where E , is the uniform field in the absence of the minor phase particle . In
the derivation of this equation , it is assumed that the polarization of one particle
is not influenced by the polarization of other particles . In reality , the polarization
...
Page 148
In spite of the broad distribution of particle sizes in one sample , the elongation
ratio of silver particles was found fairly ... of different interfacial energies on
elongated particles of different size ( Seward , 1974 ) is small in this particular
case .
In spite of the broad distribution of particle sizes in one sample , the elongation
ratio of silver particles was found fairly ... of different interfacial energies on
elongated particles of different size ( Seward , 1974 ) is small in this particular
case .
Page 312
Quantitatively , the theory by Charles starts with the orientation polarization
theory by Frölich ( 1949 ) who postulated that a particle with charge e can take
one of two equivalent sites 1 and 2 separated by a distance b and an energy of
height H ...
Quantitatively , the theory by Charles starts with the orientation polarization
theory by Frölich ( 1949 ) who postulated that a particle with charge e can take
one of two equivalent sites 1 and 2 separated by a distance b and an energy of
height H ...
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