INGENIA

MAT-06

True stress from engineering

σt = σe (1+εe) at constant volume.

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PlasticityISO 6892

Governing equation

σt=σe(1+εe),εt=ln⁡(1+εe)\sigma_t=\sigma_e(1+\varepsilon_e),\quad \varepsilon_t=\ln(1+\varepsilon_e)

εe∈[0,0.8]\varepsilon_e \in \left[0, 0.8\right]

where

\sigma_e
Engineering stress (MPa)
\varepsilon_e
Engineering strain (—)
\sigma_t
True stress (MPa)
\varepsilon_t
True strain (—)

The figure, part by part

Each numbered marker wears the color of its card. Hover a card to light the marker. Tap a marker to jump to that card. The slider walks a red point along the curve; Animate drawing traces it like a pen.

MAT-06 · curve
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①

Governing law — red

σt=σe(1+εe),εt=ln⁡(1+εe)\sigma_t=\sigma_e(1+\varepsilon_e),\quad \varepsilon_t=\ln(1+\varepsilon_e)

εe∈[0,0.8]\varepsilon_e \in \left[0, 0.8\right]

εe=0\varepsilon_e = 0σt=350\sigma_t = 350

②

Domain of the variable — blue

\varepsilon_e_{\min} = 0,\quad \varepsilon_e_{\max} = 0.8

εe∈[0,0.8]\varepsilon_e \in \left[0, 0.8\right]

εe=0\varepsilon_e = 0εe=0\varepsilon_e = 0

③

Response curve — green

σt=σe(1+εe),εt=ln⁡(1+εe)\sigma_t=\sigma_e(1+\varepsilon_e),\quad \varepsilon_t=\ln(1+\varepsilon_e)

εe∈[0,0.8]\varepsilon_e \in \left[0, 0.8\right]

εe=0\varepsilon_e = 0σt=350\sigma_t = 350

④

Rate of change — amber

dσtdεe\frac{\mathrm{d}\sigma_t}{\mathrm{d}\varepsilon_e}

εe∈[0,0.8]\varepsilon_e \in \left[0, 0.8\right]

εe=0.005\varepsilon_e = 0.005σt′=350\sigma_t^{\prime} = 350

Lecture brief

Historical brief

Hooke (1678), Hall–Petch grain size, Arrhenius activation and Paris fatigue-crack growth are the spine of materials selection. The sheets relate stress, microstructure and life. This sheet (MAT-06 — True stress from engineering) is the form associated with ISO 6892. Working symbols: σe\sigma_e, εe\varepsilon_e →\rightarrow σt\sigma_t, εt\varepsilon_t. Constancy of volume in plastic flow converts instantaneous area to A0/(1+εe), hence true stress is engineering stress times (1+εe).

Purpose

Purpose: compute σt\sigma_t, εt\varepsilon_t from σe\sigma_e, εe\varepsilon_e in Materials via σt=σe(1+εe),εt=ln⁡(1+εe)\sigma_t=\sigma_e(1+\varepsilon_e),\quad \varepsilon_t=\ln(1+\varepsilon_e) σt = σe (1+εe) at constant volume. Use it when a real materials question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given σe=350.000 MPa\sigma_e = 350.000\,\mathrm{MPa}, εe=0.120 —\varepsilon_e = 0.120\,\mathrm{—}, the governing relation σt=σe(1+εe),εt=ln⁡(1+εe)\sigma_t=\sigma_e(1+\varepsilon_e),\quad \varepsilon_t=\ln(1+\varepsilon_e) yields σt=392.000 MPa\sigma_t = 392.000\,\mathrm{MPa}, εt=0.1133 —\varepsilon_t = 0.1133\,\mathrm{—}. Before necking, incompressible plasticity. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • True stress \sigma_t392.000 MPa
  • True strain \varepsilon_t0.1133 —
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MAT-06 · curve
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Narration of this film

Before necking, incompressible plasticity.

Constancy of volume in plastic flow converts instantaneous area to A0/(1+εe), hence true stress is engineering stress times (1+εe).

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Watch on YouTube