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Von Mises yield criterion

In continuum mechanics, the maximum distortion energy criterion (also von Mises yield criterion[1]) states that yielding of a ductile material begins when the second invariant of deviatoric stress reaches a critical value.[2] It is a part of plasticity theory that mostly applies to ductile materials, such as some metals. Prior to yield, material response can be assumed to be of a linear elastic, nonlinear elastic, or viscoelastic behavior.

In materials science and engineering, the von Mises yield criterion is also formulated in terms of the von Mises stress or equivalent tensile stress, . This is a scalar value of stress that can be computed from the Cauchy stress tensor. In this case, a material is said to start yielding when the von Mises stress reaches a value known as yield strength, . The von Mises stress is used to predict yielding of materials under complex loading from the results of uniaxial tensile tests. The von Mises stress satisfies the property where two stress states with equal distortion energy have an equal von Mises stress.

Because the von Mises yield criterion is independent of the first stress invariant, , it is applicable for the analysis of plastic deformation for ductile materials such as metals, as onset of yield for these materials does not depend on the hydrostatic component of the stress tensor.

Although it has been believed it was formulated by James Clerk Maxwell in 1865, Maxwell only described the general conditions in a letter to William Thomson (Lord Kelvin).[3] Richard Edler von Mises rigorously formulated it in 1913.[2][4] Tytus Maksymilian Huber (1904), in a paper written in Polish, anticipated to some extent this criterion by properly relying on the distortion strain energy, not on the total strain energy as his predecessors.[5][6][7] Heinrich Hencky formulated the same criterion as von Mises independently in 1924.[8] For the above reasons this criterion is also referred to as the "Maxwell–Huber–Hencky–von Mises theory".

  1. ^ "Von Mises Criterion (Maximum Distortion Energy Criterion)". Engineer's edge. Retrieved 8 February 2018.
  2. ^ a b von Mises, R. (1913). "Mechanik der festen Körper im plastisch-deformablen Zustand". Nachrichten von der Gesellschaft der Wissenschaften zu Göttingen. Mathematisch-Physikalische Klasse. 1913 (1): 582–592.
  3. ^ Jones, Robert Millard (2009). Deformation Theory of Plasticity, p. 151, Section 4.5.6. Bull Ridge Corporation. ISBN 9780978722319. Retrieved 2017-06-11.
  4. ^ Ford (1963). Advanced Mechanics of Materials. London: Longmans.
  5. ^ Huber, M. T. (1904). "Właściwa praca odkształcenia jako miara wytezenia materiału". Czasopismo Techniczne. 22. Lwów. Translated as "Specific Work of Strain as a Measure of Material Effort". Archives of Mechanics. 56: 173–190. 2004.
  6. ^ Hill, R. (1950). The Mathematical Theory of Plasticity. Oxford: Clarendon Press.
  7. ^ Timoshenko, S. (1953). History of strength of materials. New York: McGraw-Hill.
  8. ^ Hencky, H. (1924). "Zur Theorie plastischer Deformationen und der hierdurch im Material hervorgerufenen Nachspannngen". Z. Angew. Math. Mech. 4 (4): 323–334. Bibcode:1924ZaMM....4..323H. doi:10.1002/zamm.19240040405.

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