Therefore, we can write the steady-state creep rate $\dot{\epsilon}_{s}$ as:
\[\dot{\epsilon}_{s} = K_{2} \sigma^{n} \exp\left(-\frac{Q_{c}}{RT}\right)\]
where $K_{2}$ is a constant, $Q_{c}$ is the activation energy for creep, $R$ is the gas constant, and $T$ is
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