Abstract
The equation η =
n
.
t
r
connects the viscosity, η, with the rigidity modulus,
n
, and the time of relaxation,
t
r
. In the case of simple fluids, for which the equation was originally given by Maxwell, the dissipation of shearing stress is so rapid that neither
n
nor
t
r
has been measured, so that the relationship has only a theoretical interest. In the first paper of this series* it was shown that in flour dough stress dissipation proceeds at rates that can readily be followed experimentally. The “time of relaxation,"
t
r
, was given an extended significance, and defined in such a way as to be applicable to plastic materials like dough for which η is not a constant. A series of values for the viscosity was obtained with the aid of equation (i).
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