
Plastic deformation is an irreversible process that occurs when a material undergoes a change in shape or form. Shear stress is one of the stress types that cause materials to deform or warp. It is defined as the internal forces that arise when adjacent layers of a material slide or deform relative to each other. In the case of metals, plastic deformation occurs as a result of the glide of dislocations driven by shear stress. This process, known as slip, involves the movement of atoms slipping over each other within a crystal lattice when the applied stress exceeds the critical resolved shear stress of the material. This leads to macroscopic changes without affecting the atomic arrangement. Other factors, such as grain structures and various treatments, can also influence the plastic deformation of metals.
| Characteristics | Values |
|---|---|
| Plastic deformation | An irreversible process that occurs when a shear stress exceeds a critical value and causes permanent changes in atomic positions |
| Plastic deformation in metals | Caused by the sliding of lattice planes over each other without affecting the atomic arrangement |
| Shear stress | Quantifies the internal forces that arise when adjacent layers of a material or fluid slide or deform relative to each other |
| Shear modulus | Typically assumed to be zero during plastic deformation |
| Yield stress | The stress required to initiate plastic deformation |
| Work hardening | The continued deformation of a material under an increasing level of applied stress |
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What You'll Learn
- Plastic deformation is caused by shear stress exceeding a critical value
- Shear stress causes permanent changes in atomic positions
- Dislocations, grain structures, and treatments affect metal plasticity
- Slip is a movement of atoms slipping over each other within crystal lattices
- Plastic deformation is irreversible

Plastic deformation is caused by shear stress exceeding a critical value
Plastic deformation is an irreversible process that occurs when a material is subjected to shear stress beyond its yield strength. Shear stress refers to the internal forces that cause adjacent layers of a material or fluid to slide or deform relative to each other. When the applied stress exceeds the critical resolved shear stress of the material, it can result in plastic deformation.
In metals, plastic deformation predominantly occurs through shearing, where lattice planes slide over each other, allowing macroscopic changes without altering the atomic arrangement. This is known as slip, and it is facilitated by the movement of dislocations along close-packed planes and directions, enabling atoms to slip over each other with reduced stress. The movement of dislocations is a fundamental mechanism of plastic deformation, driven by shear stresses.
The yield point, or yield stress, represents the threshold at which a material transitions from elastic behaviour to plastic deformation. Beyond this point, atomic bonds stretch and break, leading to permanent deformation. The yield stress depends on various factors, including crystal structure, grain size, composition, and prior dislocation density. Work hardening, or strain hardening, occurs as more dislocations are created and interact, leading to a decrease in mobility and an increase in the required stress for further deformation.
Plastic deformation in ceramics differs from metals due to their covalent atomic bonds, which require higher shear stresses for dislocation motion. Ceramics typically fail by the extension of flaws rather than dislocation motion. Additionally, ceramics can densify under stress at high temperatures, further distinguishing their deformation behaviour from metals.
Understanding the relationship between shear stress and plastic deformation is crucial for engineering applications. By studying the yield strength and deformation mechanisms of materials, engineers can design structures and select appropriate materials that can withstand specific stress levels without failing. This knowledge is particularly important in manufacturing processes such as wire drawing, forging, and injection moulding, where plastic deformation is intentionally induced to create desired shapes and properties.
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Shear stress causes permanent changes in atomic positions
Plastic deformation is an irreversible process that occurs when a shear stress exceeds a critical value, resulting in permanent changes in atomic positions. This phenomenon is observed in crystalline solids, polymers, and glasses, each exhibiting unique characteristics. While metals typically undergo plastic deformation at a constant volume, ceramics exhibit varying behaviour due to their as-fabricated porosity, often densifying under stress at high temperatures.
In the context of metals, plastic deformation is predominantly caused by the glide of dislocations driven by shear stresses. This occurs within a polycrystal, where individual grains undergo cooperative complex shape changes, aligning with their neighbours. The process is challenging to study in real-time, but certain situations allow for a clearer understanding. Work hardening, or strain hardening, is a notable effect of plastic deformation, where the creation and interaction of dislocations lead to reduced mobility. The work hardening rate tends to decrease with increasing strain, influenced by the formation of tangles and annihilation of dislocations through processes like climb and cross-slip.
The critical resolved shear stress (CRSS) required to initiate deformation varies between theoretical predictions and experimental observations. Theoretically, metals have a CRSS range of 1000 to 3000 N/mm² (1 to 3 GPa), while experimental values are significantly lower, falling between 1 and 30 N/mm². This discrepancy highlights that deformation commences at much lower shear stress levels than theoretically calculated.
The deformation process is influenced by factors such as crystal structure, grain size, crystallographic texture, composition, and grain boundary structure. These factors contribute to the complexity of plasticity, and external factors like thermal or mechanical treatments can further modify these characteristics. Additionally, the ductility of metals plays a crucial role in their ability to withstand plastic deformation. A metal with high ductility possesses numerous slip planes, allowing for simultaneous deformation in multiple directions without irreparably rupturing the atomic structure.
Shear stress, denoted by τ or tau, is a component of stress coplanar with a material cross-section. It arises from shear force, which is parallel to the material cross-section. The shear force induces the slipping of atomic planes, leading to deformation. This slipping occurs when the force per bond or force per area exceeds a critical value, causing the lattice planes to slip and triggering a deformation process.
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Dislocations, grain structures, and treatments affect metal plasticity
Plastic deformation of metals is primarily caused by the glide of dislocations driven by shear stress. Dislocations are the primary drivers of plastic deformation, and their interactions with each other and with other microstructural features such as
Grain boundaries are insurmountable borders for dislocations, and the number of dislocations within a grain influences how stress builds up in the adjacent grain, eventually activating dislocation sources and enabling deformation in the neighbouring grain as well. This is known as grain-boundary strengthening or Hall-Petch strengthening. The smaller the grain size, the higher the strength, and this phenomenon arises from the blocking of dislocation motion by grain boundaries.
Grain boundary engineering involves manipulating the grain boundary structure and energy to enhance mechanical properties. By controlling the interfacial energy, it is possible to engineer materials with desirable grain boundary characteristics, such as increased interfacial area or higher grain boundary density. Introducing alloying elements into the material can alter the interfacial energy of grain boundaries. Alloying can result in segregation of solute atoms at the grain boundaries, modifying the atomic arrangements and bonding, and thereby influencing the interfacial energy.
Thermal treatments can also be employed to modify the interfacial energy of grain boundaries. Annealing at specific temperatures and durations can induce atomic rearrangements, diffusion, and stress relaxation at the grain boundaries, leading to changes in the interfacial energy. Severe plastic deformation techniques, such as equal-channel angular pressing (ECAP) or high-pressure torsion (HPT), can lead to grain refinement and the creation of new grain boundaries with tailored characteristics.
The plasticity of metals can also be affected by various treatments. For example, work hardening or strain hardening arises as more dislocations are created and interact with each other, becoming less mobile. Mechanical treatments and exposure to different environments can also dramatically change the plasticity characteristics of a material.
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Slip is a movement of atoms slipping over each other within crystal lattices
Plastic deformation is an irreversible process that occurs when a shear stress exceeds a critical value, causing permanent changes in atomic positions. This phenomenon is observed in crystalline solids, polymers, and glasses, with metals being the most common example. It is important to note that while the crystalline nature remains unchanged during plastic deformation, the process results in non-recoverable alterations.
Slip, a fundamental mechanism in plastic deformation, is the movement of atoms slipping over each other within crystal lattices. In crystalline solids, atoms are arranged in a regular pattern called a lattice. However, imperfections called dislocations can disrupt this ordered arrangement. Dislocations are linear crystallographic defects or irregularities within a crystal structure, causing an abrupt change in the arrangement of atoms. These dislocations act as line defects, making it easier for atoms to move past one another under stress.
When an external force is applied to a material, it generates stress, and the presence of dislocations allows planes of atoms to slide over each other along specific planes known as slip planes. These slip planes are the most densely packed planes in the lattice, and the slip directions are the most closely packed directions in the crystal. Together, they form the crystal's slip system, which enables materials to undergo plastic deformation without breaking. The slip mechanism is crucial in applications where ductility, or the ability to deform without fracturing, is essential, such as in the manufacturing of metal products.
The slip process can be observed when a metal rod is pulled. As the force increases, dislocations within the metal lattice move, allowing layers of atoms to slide past each other, causing the rod to stretch without breaking. Similarly, during the bending of a metal sheet, slip allows the metal to deform while remaining intact. The movement of dislocations, or glide, allows atoms to slide over each other at low stress levels. This results in a change in the material's geometry without altering its crystalline nature.
The magnitude and direction of slip are represented by the Burgers vector, which also defines the distance and direction of movement caused by a dislocation. There are two types of dislocations that can induce slip: edge dislocations and screw dislocations. Edge dislocations have a Burgers vector perpendicular to the dislocation line, while screw dislocations have a parallel Burgers vector. Screw dislocations can easily cross slip between planes if the adjacent plane contains the direction of the Burgers vector. The formation of slip bands indicates concentrated unidirectional slip, leading to surface roughness and potential crack nucleation sites.
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Plastic deformation is irreversible
Plastic deformation is an irreversible process that occurs when a material is subjected to stress beyond its yield strength. This typically happens when a shear stress exceeds a critical value, resulting in permanent changes to the atomic positions within the material. While the crystalline nature remains unchanged, the atomic bonds stretch and break, causing planes to shear over each other and leading to irreversible deformation.
In metals, plastic deformation commonly occurs due to the glide of dislocations driven by shear stresses. Dislocations are defects in the crystal lattice, where an extra half plane is inserted, resulting in two types of movements: glide and climb. During glide, dislocations move along a surface defined by their burgers vector, while during climb, they move outward from the glide plane. This dislocation motion allows for the generation and movement of dislocations, which is the principal mechanism of plastic deformation in metals.
The irreversible nature of plastic deformation is attributed to the fact that even after the load is removed, the stretched bonds may recover, but the shear planes remain. This indicates that the material has undergone a permanent change. Additionally, plastic deformation is characterized by phenomena such as yielding, strain hardening, and necking, which contribute to its irreversible nature.
Furthermore, the stress components can continue to increase even after yielding, and the work hardening rate tends to decrease progressively with increasing strain. This complexity in the behavior of materials under stress highlights the difficulty in studying plastic deformation, especially in metals. However, it is important to note that the plasticity characteristics can be altered by various treatments or exposure to different environments, demonstrating the dynamic nature of material behavior under stress.
While plastic deformation is typically associated with metals, it can also occur in other materials such as ceramics, polymers, and glasses. In ceramics, dislocation motion requires high shear stresses due to the presence of covalent atomic bonds. On the other hand, polymers and glasses undergo a time-dependent process called viscous deformation, where atomic and molecular bonds are permanently rearranged. This highlights the diverse nature of plastic deformation and the importance of understanding the specific characteristics of different materials under stress.
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Frequently asked questions
Plastic deformation is an irreversible process that occurs when a material undergoes a change in atomic positions due to stress exceeding a critical value. It is often assumed to occur at a constant volume, which is usually the case for metals.
Shear stress quantifies the internal forces that arise when adjacent layers of a material slide or deform relative to each other. When shear stress exceeds a critical value, it can cause plastic deformation by allowing planes to shear over each other, leading to permanent deformation.
The stress required for plastic deformation can be influenced by various factors, such as the type of material, crystal structure, grain size, temperature, and the presence of defects or dislocations. Additionally, the yield strength of the material plays a crucial role, as plastic deformation occurs when the applied stress exceeds the yield point.









































