Flow stress

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In materials science, the flow stress, typically denoted as Y f {\displaystyle Y_{\text{f}}} (or σ f {\displaystyle \sigma _{\text{f}}} ), is defined as the instantaneous value of stress required to continue plastically deforming a material - to keep it flowing. It is most commonly, though not exclusively, used in reference to metals. On a stress-strain curve, the flow stress can be found anywhere within the plastic regime; more explicitly, a flow stress can be found for any value of strain between and including yield point ( σ y {\displaystyle \sigma _{\text{y}}} ) and excluding fracture ( σ F {\displaystyle \sigma _{\text{F}}} ): σ y ≤ Y f < σ F {\displaystyle \sigma _{\text{y}}\leq Y_{\text{f}}<\sigma _{\text{F}}} . The flow stress changes as deformation proceeds and usually increases as strain accumulates due to work hardening, although the flow stress could decrease due to any recovery process. In continuum mechanics, the flow stress for a given material will vary with changes in temperature, T {\displaystyle T} , strain, ε {\displaystyle \varepsilon } , and strain-rate, ε ˙ {\displaystyle {\dot {\varepsilon }}} ; therefore it can be written as some function of those properties: Y f = f ( ε , ε ˙ , T ) {\displaystyle Y_{\text{f}}=f(\varepsilon ,{\dot {\varepsilon }},T)} The exact equation to represent flow stress depends on the particular material and plasticity model being used. Hollomon's equation is commonly used to represent the behavior seen in a stress-strain plot during work hardening: Y f = K ε p n {\displaystyle Y_{\text{f}}=K\varepsilon _{\text{p}}^{\text{n}}} Where Y f {\displaystyle Y_{\text{f}}} is flow stress, K {\displaystyle K} is a strength coefficient, ε p {\displaystyle \varepsilon _{\text{p}}} is the plastic strain, and n {\displaystyle n} is the strain hardening exponent. Note that this is an empirical relation and does not model the relation at other temperatures...