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... W 0.2 V ( 16 ) 0.28 ( 3 ) Voids : The most significant hardening equation for voids is due to Coulomb ( 17 ) , and this can again be expressed as Δι = α , μόν nd where n and d are the density and diameter of void , respectively .
... W 0.2 V ( 16 ) 0.28 ( 3 ) Voids : The most significant hardening equation for voids is due to Coulomb ( 17 ) , and this can again be expressed as Δι = α , μόν nd where n and d are the density and diameter of void , respectively .
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The number density of the radiators is very much smaller than that of the perturbers so that the interaction between the radiators is negligible . The gas is regarded as being divided into a very large number of noninteracting cells .
The number density of the radiators is very much smaller than that of the perturbers so that the interaction between the radiators is negligible . The gas is regarded as being divided into a very large number of noninteracting cells .
Seite
The number density of the radiators is very much smaller than that of the perturbers so that the interaction between the radiators is negligible . The gas is regarded as being divided into a very large number of noninteracting cells .
The number density of the radiators is very much smaller than that of the perturbers so that the interaction between the radiators is negligible . The gas is regarded as being divided into a very large number of noninteracting cells .
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