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Drucker Prager yield criterion
Encyclopedia
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The Drucker–Prager yield criterion has the form
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where
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Stress (physics)
In continuum mechanics, stress is a measure of the internal forces acting within a deformable body. Quantitatively, it is a measure of the average force per unit area of a surface within the body on which internal forces act. These internal forces are a reaction to external forces applied on the body...
and
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Stress (physics)
In continuum mechanics, stress is a measure of the internal forces acting within a deformable body. Quantitatively, it is a measure of the average force per unit area of a surface within the body on which internal forces act. These internal forces are a reaction to external forces applied on the body...
. The constants
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In terms of the equivalent stress
Von Mises stress
The von Mises yield criterion suggests that the yielding of materials begins when the second deviatoric stress invariant J_2 reaches a critical value k. For this reason, it is sometimes called the J_2-plasticity or J_2 flow theory. It is part of a plasticity theory that applies best to ductile...
(or von Mises stress
Von Mises stress
The von Mises yield criterion suggests that the yielding of materials begins when the second deviatoric stress invariant J_2 reaches a critical value k. For this reason, it is sometimes called the J_2-plasticity or J_2 flow theory. It is part of a plasticity theory that applies best to ductile...
) and the hydrostatic (or mean) stress
Hydrostatic stress
In continuum mechanics, a hydrostatic stress is an isotropic stress that is given by the weight of water above a certain point. It is often used interchangeably with "pressure" and is also known as confining stress, particularly in the field geomechanics...
, the Drucker–Prager criterion can be expressed as
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where
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The Drucker–Prager yield surface is a smooth version of the Mohr–Coulomb yield surface.
Expressions for A and B
The Drucker–Prager model can be written in terms of the principal stresses as
If
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If
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Solving these two equations gives
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Uniaxial asymmetry ratio
Different uniaxial yield stresses in tension and in compression are predicted by the Drucker–Prager model. The uniaxial asymmetry ratio for the Drucker–Prager model is
Expressions in terms of cohesion and friction angle
Since the Drucker–Prager yield surfaceYield surface
A yield surface is a five-dimensional surface in the six-dimensional space of stresses. The yield surface is usually convex and the state of stress of inside the yield surface is elastic. When the stress state lies on the surface the material is said to have reached its yield point and the...
is a smooth version of the Mohr–Coulomb yield surface
Mohr-Coulomb theory
Mohr–Coulomb theory is a mathematical model describing the response of brittle materials such as concrete, or rubble piles, to shear stress as well as normal stress. Most of the classical engineering materials somehow follow this rule in at least a portion of their shear failure envelope...
, it is often expressed in terms of the cohesion (
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Mohr-Coulomb theory
Mohr–Coulomb theory is a mathematical model describing the response of brittle materials such as concrete, or rubble piles, to shear stress as well as normal stress. Most of the classical engineering materials somehow follow this rule in at least a portion of their shear failure envelope...
. If we assume that the Drucker–Prager yield surface circumscribes the Mohr–Coulomb yield surface then the expressions for
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If the Drucker–Prager yield surface inscribes the Mohr–Coulomb yield surface then
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Derivation of expressions for ![]() ![]() |
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The expression for the Mohr–Coulomb yield criterion Mohr-Coulomb theory Mohr–Coulomb theory is a mathematical model describing the response of brittle materials such as concrete, or rubble piles, to shear stress as well as normal stress. Most of the classical engineering materials somehow follow this rule in at least a portion of their shear failure envelope... in Haigh–Westergaard space is ![]() If we assume that the Drucker–Prager yield surface circumscribes the Mohr–Coulomb yield surface such that the two surfaces coincide at ![]() ![]() or, ![]() The Drucker–Prager yield criterion expressed in Haigh–Westergaard coordinates is ![]() Comparing equations (1.1) and (1.2), we have ![]() These are the expressions for ![]() ![]() On the other hand if the Drucker–Prager surface inscribes the Mohr–Coulomb surface, then matching the two surfaces at ![]() ![]() ![]() ![]() |
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Drucker–Prager model for polymers
The Drucker–Prager model has been used to model polymers such as polyoxymethylenePolyoxymethylene
Polyoxymethylene , also known as acetal, polyacetal, and polyformaldehyde, is an engineering thermoplastic used in precision parts that require high stiffness, low friction and excellent dimensional stability....
and polypropylene
Polypropylene
Polypropylene , also known as polypropene, is a thermoplastic polymer used in a wide variety of applications including packaging, textiles , stationery, plastic parts and reusable containers of various types, laboratory equipment, loudspeakers, automotive components, and polymer banknotes...
. For polyoxymethylene
Polyoxymethylene
Polyoxymethylene , also known as acetal, polyacetal, and polyformaldehyde, is an engineering thermoplastic used in precision parts that require high stiffness, low friction and excellent dimensional stability....
the yield stress is a linear function of the pressure. However, polypropylene
Polypropylene
Polypropylene , also known as polypropene, is a thermoplastic polymer used in a wide variety of applications including packaging, textiles , stationery, plastic parts and reusable containers of various types, laboratory equipment, loudspeakers, automotive components, and polymer banknotes...
shows a quadratic pressure-dependence of the yield stress.
Drucker–Prager model for foams
For foams, the GAZT model uses
where
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Extensions of the isotropic Drucker–Prager model
The Drucker–Prager criterion can also be expressed in the alternative form
Deshpande–Fleck yield criterion
The Deshpande–Fleck yield criterion for foams has the form given in above equation. The parameters
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where
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Anisotropic Drucker–Prager yield criterion
An anisotropic form of the Drucker–Prager yield criterion is the Liu–Huang–Stout yield criterion . This yield criterion is an extension of the generalized Hill yield criterionHill yield criteria
Rodney Hill has developed several yield criteria for anisotropic plastic deformations. The earliest version was a straightforward extension of the von Mises yield criterion and had a quadratic form. This model was later generalized by allowing for an exponent m...
and has the form
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The coefficients
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where
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and
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The Drucker yield criterion
The Drucker–Prager criterion should not be confused with the earlier Drucker criterion which is independent of the pressure (
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where
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Anisotropic Drucker Criterion
An anisotropic version of the Drucker yield criterion is the Cazacu–Barlat (CZ) yield criterion which has the form
where
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Cazacu–Barlat yield criterion for plane stress
For thin sheet metals, the state of stress can be approximated as plane stress. In that case the Cazacu–Barlat yield criterion reduces to its two-dimensional version with
For thin sheets of metals and alloys, the parameters of the Cazacu–Barlat yield criterion are
Material | ![]() | ![]() | ![]() | ![]() | ![]() | ![]() | ![]() | ![]() | ![]() | ![]() | ![]() |
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6016-T4 Aluminum Alloy | 0.815 | 0.815 | 0.334 | 0.42 | 0.04 | -1.205 | -0.958 | 0.306 | 0.153 | -0.02 | 1.4 |
2090-T3 Aluminum Alloy | 1.05 | 0.823 | 0.586 | 0.96 | 1.44 | 0.061 | -1.302 | -0.281 | -0.375 | 0.445 | 1.285 |
See also
- Yield surfaceYield surfaceA yield surface is a five-dimensional surface in the six-dimensional space of stresses. The yield surface is usually convex and the state of stress of inside the yield surface is elastic. When the stress state lies on the surface the material is said to have reached its yield point and the...
- Yield (engineering)Yield (engineering)The yield strength or yield point of a material is defined in engineering and materials science as the stress at which a material begins to deform plastically. Prior to the yield point the material will deform elastically and will return to its original shape when the applied stress is removed...
- Plasticity (physics)Plasticity (physics)In physics and materials science, plasticity describes the deformation of a material undergoing non-reversible changes of shape in response to applied forces. For example, a solid piece of metal being bent or pounded into a new shape displays plasticity as permanent changes occur within the...
- Failure theory (material)Failure theory (material)Failure theory is the science of predicting the conditions under which solid materials fail under the action of external loads. The failure of a material is usually classified into brittle failure or ductile failure . Depending on the conditions most materials can fail in a brittle or ductile...