Plasticity

Science — James William Steven Parker

Plasticity is the branch of mechanics and materials science concerned with irreversible deformation that remains after unloading when a material is subjected to stresses beyond its elastic range. Plastic deformation changes the material's shape or internal state without requiring the load to remain present. The concept is particularly important in metals, where dislocation motion within crystalline structures provides a microscopic mechanism for permanent deformation, but plastic behaviour also occurs in polymers, soils, rocks, ceramics under certain conditions and many other materials.

Plasticity differs from elasticity because elastic deformation is recoverable, while plastic strain remains after the load is removed. It also differs from fracture because a material can undergo substantial plastic deformation without immediately separating into distinct pieces. Engineering plasticity theory provides mathematical models for predicting yielding, plastic strain accumulation, hardening and the load carrying capacity of structures.

Yielding is the transition into significant plastic deformation under a specified constitutive model. For metals, yield criteria such as von Mises and Tresca are widely used to represent the onset of yielding under multiaxial stress states. The von Mises criterion is based on distortional or deviatoric stress and is closely connected to the idea that yielding begins when a critical level of distortional energy or equivalent stress is reached. The Tresca criterion is associated with maximum shear stress.

These criteria give different predictions in some stress states but often produce similar engineering results for ductile metals. Yield stress can depend on temperature, strain rate, microstructure, prior deformation and loading history. Consequently, a tabulated yield strength is meaningful only within the conditions under which it was measured.

Plastic deformation in crystalline materials is strongly associated with dislocations, which are line defects in crystal lattices. Plastic strain can occur when dislocations move through a crystal under suitable resolved shear stresses. Slip systems, crystal structure, temperature and obstacles to dislocation motion influence plastic behaviour. Grain boundaries, precipitates, solute atoms and other microstructural features can impede dislocation motion and increase strength. Cold working increases the density of dislocations and can produce strain hardening, making further plastic deformation more difficult. Annealing can alter the microstructure and reduce some effects of prior deformation. This connection between microscopic structure and macroscopic constitutive behaviour is a central reason why Plasticity belongs simultaneously to mechanics and materials science.

Hardening describes the change in material resistance as plastic deformation accumulates. In strain hardening, continued plastic deformation generally requires increasing stress over a specified range. Isotropic hardening models represent expansion of the yield surface in stress space, while kinematic hardening represents translation of the yield surface and can describe aspects of the Bauschinger effect, in which prior plastic deformation in one direction changes subsequent yielding in the reverse direction. Combined hardening models can represent both effects. The choice of hardening law influences predictions of cyclic loading, forming processes and structural response. Perfect plasticity provides a simpler idealisation in which plastic flow occurs without further increase in yield stress, while more realistic models incorporate evolving material strength.

Plastic flow rules describe the direction in stress space associated with incremental plastic strain. In associated plasticity, the plastic potential is taken to coincide with the yield function, producing a mathematically convenient relationship between yielding and flow. Non associated plasticity uses a separate plastic potential and is particularly important for some pressure sensitive materials such as soils and rocks. The distinction matters because the direction of plastic strain increments affects predicted deformation and volume change. Classical metal plasticity often assumes approximately incompressible plastic flow, whereas geological and granular materials can undergo significant plastic volume changes. Constitutive modelling must therefore reflect the material's actual mechanisms rather than treating all plastic solids as equivalent.

Plasticity is essential in manufacturing processes such as rolling, forging, extrusion, stamping and metal forming because permanent deformation is deliberately produced to obtain a desired shape. Accurate plastic models allow engineers to estimate forming forces, material flow, thickness changes, springback and potential defects. Plasticity also matters in accidental overload because a structure can redistribute stresses after local yielding. In some structural systems, controlled plastic deformation provides energy absorption during impacts or extreme loads. However, excessive yielding can cause permanent distortion, loss of dimensional accuracy, instability or eventual fracture. Engineering design therefore distinguishes between allowable local yielding, which may be acceptable under defined circumstances, and uncontrolled plastic collapse or damage.

Plasticity interacts with other failure mechanisms and time dependent effects. Repeated loading can produce cyclic plasticity, where the material accumulates or redistributes plastic strain over cycles. Ratcheting can cause progressive permanent deformation under certain combinations of cyclic and sustained loads. Creep is a time dependent inelastic process that becomes particularly important at elevated temperatures, and viscoplastic models combine plastic type behaviour with rate dependence.

Damage and fracture can develop after plastic deformation through mechanisms such as void nucleation, growth and coalescence in ductile metals. The history dependence of these processes means that the current response cannot always be determined from the instantaneous stress alone. Internal variables representing accumulated plastic strain, hardening state or damage are therefore commonly used in constitutive models.

Plasticity theory is implemented extensively in computational Solid Mechanics, especially finite element analysis of structures subjected to large loads or forming processes. Numerical algorithms must determine whether an increment of loading remains elastic or crosses the yield surface, then calculate the corresponding plastic correction and update internal material variables. The accuracy of the simulation depends on the constitutive model, material parameters, mesh, loading history and numerical integration method.

Plasticity models can be highly sophisticated, but greater complexity does not guarantee greater accuracy if the underlying material assumptions are inappropriate. Experimental testing is therefore required to identify yield behaviour, hardening characteristics and rate or temperature dependence. Plasticity provides a powerful bridge between microscopic mechanisms and macroscopic structural response, enabling engineers to predict permanent deformation and assess the behaviour of materials under loads that exceed purely elastic limits.