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Law with Effective Time

Recall from Chapter 6 that the constitutive law describing the stress and strain relation of a viscoelastic material can be written as [Pg.254]

one can consider the modulus at temperature T and time t to be the same as the modulus at a reference temperature To at a reduced time At a small time increment later, dt, the modulus at temperature T has changed to a new value correspondingly later in reduced time at the reference temperature [Pg.254]

Physically, this expression represents that all relaxation times in a time increment at temperature T are 1/a times slower/faster than those occurring in the reduced time increment at the reference temperature. Integrating one obtains an expression for reduced time, or ejfective time as it is often called, as [Pg.254]

Note that the shift factor is a function of time according to the temperature history as the temperature changes, so does the shift factor. To account for a temperature history, the constitutive law can thus be written in effective time space as [Pg.254]

Mapping this constitutive law to the real time domain results in [Pg.255]


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