Understanding Creep and Creep Rate

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The discussion focuses on understanding the significance of the graph plotting ln(dεss/dt) against ln(σ) in the context of creep behavior. It highlights that this relationship indicates a strain rate effect, which can involve strain hardening, as expressed in the equation σ = K εn \dot{ε}^m. The use of natural logarithms allows for a linear representation of the relationship between stress and steady-state creep rate, facilitating analysis of material behavior under different loading conditions. The conversation also touches on the elastic range, where stress is proportional to strain through Young's modulus. Overall, the analysis aims to clarify the implications of these logarithmic relationships in material science.
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So I'm looking through some material on creep for one of my courses. There is a graph of strain ε vs Time, t. Consisting of Primary creep, steady-state creep, and tertiary creep. I pretty much can follow that and understand why the graph looks the way it does.

However there is another graph under it that is ln(dεss/dt) vs ln(σ). I am trying to understand what the significance is of taking the natural log of stress and the steady state creep rate. What would a graph containing these things be telling us, and why the natural log?

Thanks for any help.
 
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In the elastic range, σ = Eε, where E is the elastic (Young's) modulus, i.e., it's linear as in 'linear elastic'. In most systems, the service domain is in the elastic range.

Secondary or steady-state creep involves inelastic or plastic deformation in which,

σ = Kεn, or ln σ = ln K + n ln ε.

and there is also cases where,

σ = K εn \dot{\epsilon}^m.

In the case of ln(dεss/dt) vs ln(σ), this implies a strain rate effect, i.e., strain hardening or strain rate (hardening) effect, e.g., σ = K \dot{\epsilon}^m.
 
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