What two types of deformation are there in Physics

When a sufficient load is applied to a metal or other structural material, it will cause the material to change shape. This change in shape is called deformation. A temporary shape change that is self-reversing after the force is removed, so that the object returns to its original shape, is called elastic deformation. In other words, elastic deformation is a change in shape of a material at low stress that is recoverable after the stress is removed. This type of deformation involves stretching of the bonds, but the atoms do not slip past each other.

In materials science, deformation refers to modifications of the shape or size of an object due to applied forces or a change in temperature.

Deformation is usually caused by forces such as:

• Tensile (pulling)
• Compressive (pushing)
• Shear
• Bending
• Torsion (twisting)

Deformation usually appears as strain.

As deformation occurs, internal inter-molecular forces arise that oppose the applied force. If the applied force is not too high, these forces resist the applied force and allow the material to resume its original state once the load is removed. A larger applied force may cause a permanent deformation of the material, or even structural failure.

Different types of deformation may result from variations in type of material, size and the forces applied. Types of deformations include:

• Elastic deformation - This can be reversible. Elastomers and type memory metals like nitinol exhibit huge elastic deformation ranges, as does rubber.
• Plastic deformation - This may be irreversible. Soft thermoplastics have a rather large plastic deformation variance, as do ductile metals such as copper, silver and gold.
• Metal fatigue - This occurs primarily in ductile metals. Metal fatigue has been a common cause for failure, especially before the process was well understood.
• Compressive failure -This is applied to bars, columns, etc., which leads to shortening. Loading a structural object or specimen can increase the compressive stress until it reaches its compressive strength.
• Fracture - This may be irreversible. All materials eventually fracture, if enough force is applied.

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In engineering, any changes in the shape or size of an object

For usage in physics, see Deformation (physics).

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In engineering, deformation refers to the change in size or shape of an object. Displacements are the absolute change in position of a point on the object. Deflection is the relative change in external displacements on an object. Strain is the relative internal change in shape of an infinitesimally small cube of material and can be expressed as a non-dimensional change in length or angle of distortion of the cube. Strains are related to the forces acting on the cube, which are known as stress, by a stress-strain curve. The relationship between stress and strain is generally linear and reversible up until the yield point and the deformation is elastic. The linear relationship for a material is known as Young's modulus. Above the yield point, some degree of permanent distortion remains after unloading and is termed plastic deformation. The determination of the stress and strain throughout a solid object is given by the field of strength of materials and for a structure by structural analysis.

Engineering stress and engineering strain are approximations to the internal state that may be determined from the external forces and deformations of an object, provided that there is no significant change in size. When there is a significant change in size, the true stress and true strain can be derived from the instantaneous size of the object.

In the figure it can be seen that the compressive loading (indicated by the arrow) has caused deformation in the cylinder so that the original shape (dashed lines) has changed (deformed) into one with bulging sides. The sides bulge because the material, although strong enough to not crack or otherwise fail, is not strong enough to support the load without change. As a result, the material is forced out laterally. Internal forces (in this case at right angles to the deformation) resist the applied load.

The concept of a rigid body can be applied if the deformation is negligible.

Types of deformation

Depending on the type of material, size and geometry of the object, and the forces applied, various types of deformation may result. The image to the right shows the engineering stress vs. strain diagram for a typical ductile material such as steel. Different deformation modes may occur under different conditions, as can be depicted using a deformation mechanism map.

Permanent deformation is irreversible; the deformation stays even after removal of the applied forces, while the temporary deformation is recoverable as it disappears after the removal of applied forces. Temporary deformation is also called elastic deformation, while the permanent deformation is called plastic deformation.

Elastic deformation

Further information: Elasticity (physics)

The study of temporary or elastic deformation in the case of engineering strain is applied to materials used in mechanical and structural engineering, such as concrete and steel, which are subjected to very small deformations. Engineering strain is modeled by infinitesimal strain theory, also called small strain theory, small deformation theory, small displacement theory, or small displacement-gradient theory where strains and rotations are both small.

For some materials, e.g. elastomers and polymers, subjected to large deformations, the engineering definition of strain is not applicable, e.g. typical engineering strains greater than 1%,[1] thus other more complex definitions of strain are required, such as stretch, logarithmic strain, Green strain, and Almansi strain. Elastomers and shape memory metals such as Nitinol exhibit large elastic deformation ranges, as does rubber. However, elasticity is nonlinear in these materials.

Normal metals, ceramics and most crystals show linear elasticity and a smaller elastic range.

Linear elastic deformation is governed by Hooke's law, which states:

σ = E ε {\displaystyle \sigma =E\varepsilon }

Where σ {\displaystyle \sigma }

E {\displaystyle E}

Note that not all elastic materials undergo linear elastic deformation; some, such as concrete, gray cast iron, and many polymers, respond in a nonlinear fashion. For these materials Hooke's law is inapplicable.[2]

True stress and strain

Since we disregard the change of area during deformation above, the true stress and strain curve should be re-derived. For deriving the stress strain curve, we can assume that the volume change is 0 even if we deformed the materials. We can assume that:

A i × ε i = A f × ε f {\displaystyle A_{i}\times \varepsilon _{i}=A_{f}\times \varepsilon _{f}}

Then, the true stress can be expressed as below:

σ T = F / A f = F / A i × A i / A f = σ e × l f / l i = σ E × l i + δ l l i = σ E ( 1 + ε E ) {\displaystyle \sigma _{T}=F/A_{f}=F/A_{i}\times A_{i}/A_{f}=\sigma _{e}\times l_{f}/l_{i}=\sigma _{E}\times {\frac {l_{i}+\delta l}{l_{i}}}=\sigma _{E}(1+\varepsilon _{E})}

Additionally, the true strain εT can be express as below:

ε T = d l l 0 + d l l 1 + d l l 2 + ⋯ = ∑ i d l l i {\displaystyle \varepsilon _{T}={\frac {dl}{l_{0}}}+{\frac {dl}{l_{1}}}+{\frac {dl}{l_{2}}}+\cdots =\sum _{i}{\frac {dl}{l_{i}}}}

Then, we can express the value as

∫ l 0 l i d l l d x = ln ⁡ ( l i l 0 ) = ln ⁡ ( 1 + ε E ) {\displaystyle \int _{l_{0}}^{l_{i}}{\frac {dl}{l}}\,dx=\ln \left({\frac {l_{i}}{l_{0}}}\right)=\ln(1+\varepsilon _{E})}

Thus, we can induce the plot in terms of σ T {\displaystyle \sigma _{T}}

ε E {\displaystyle \varepsilon _{E}}

Additionally, based on the true stress-strain curve, we can estimate the region where necking starts to happen. Since necking starts to appear after ultimate tensile stress where the maximum force applied, we can express this situation as below:

d F = 0 = σ T d A i + A i d σ T {\displaystyle dF=0=\sigma _{T}dA_{i}+A_{i}d\sigma _{T}}

so this form can be expressed as below:

d σ T σ T = − d A i A i {\displaystyle {\frac {d\sigma _{T}}{\sigma _{T}}}=-{\frac {dA_{i}}{A_{i}}}}

It indicates that the necking starts to appear where reduction of area becomes much significant compared to the stress change. Then the stress will be localized to specific area where the necking appears.

Additionally, we can induce various relation based on true stress-strain curve.

1) True strain and stress curve can be expressed by the approximate linear relationship by taking a log on true stress and strain. The relation can be expressed as below:

σ T = K × ( ε T ) n {\displaystyle \sigma _{T}=K\times (\varepsilon _{T})^{n}}

Where K {\displaystyle K}

n {\displaystyle n}

2) In reality, stress is also highly dependent on the rate of strain variation. Thus, we can induce the empirical equation based on the strain rate variation.

σ T = K ′ × ( ε T ˙ ) m {\displaystyle \sigma _{T}=K'\times ({\dot {\varepsilon _{T}}})^{m}}

Where K ′ {\displaystyle K'}

ε T ˙ {\displaystyle {\dot {\varepsilon _{T}}}}

m {\displaystyle m}

By combining the 1) and 2), we can create the ultimate relation as below:

σ T = K ″ × ( ε T ) n ( ε T ˙ ) m {\displaystyle \sigma _{T}=K''\times (\varepsilon _{T})^{n}({\dot {\varepsilon _{T}}})^{m}}

Where K ″ {\displaystyle K''}

3) Based on the true stress-strain curve and its derivative form, we can estimate the strain necessary to start necking. This can be calculated based on the intersection between true stress-strain curve as shown in right.

This figure also shows the dependency of the necking strain at different temperature. In case of FCC metals, both of the stress-strain curve at its derivative are highly dependent on temperature. Therefore, at higher temperature, necking starts to appear even under lower strain value.

All of these properties indicate the importance of calculating the true stress-strain curve for further analyzing the behavior of materials in sudden environment.

4) A graphical method, so-called "Considere construction", can help determine the behavior of stress-strain curve whether necking or drawing happens on the sample. By setting λ = L / L 0 {\displaystyle \lambda =L/L_{0}}

σ T = σ e × λ , ε T = ln ⁡ λ . {\displaystyle \sigma _{T}=\sigma _{e}\times \lambda ,\qquad \varepsilon _{T}=\ln \lambda .}

Therefore, the value of engineering stress can be expressed by the secant line from made by true stress and λ {\displaystyle \lambda }

λ = 0 {\displaystyle \lambda =0}

λ = 1 {\displaystyle \lambda =1}

σ T − λ {\displaystyle \sigma _{T}-\lambda }

On the figure (a), there is only concave upward Considere plot. It indicates that there is no yield drop so the material will be suffered from fracture before it yields. On the figure (b), there is specific point where the tangent matches with secant line at point where λ = λ Y {\displaystyle \lambda =\lambda _{Y}}

λ = λ d {\displaystyle \lambda =\lambda _{d}}

λ Y {\displaystyle \lambda _{Y}}

λ d {\displaystyle \lambda _{d}}

Plastic deformation

See also: Plasticity (physics)

This type of deformation is not undone simply by removing the applied force. An object in the plastic deformation range, however, will first have undergone elastic deformation, which is undone simply be removing the applied force, so the object will return part way to its original shape. Soft thermoplastics have a rather large plastic deformation range as do ductile metals such as copper, silver, and gold. Steel does, too, but not cast iron. Hard thermosetting plastics, rubber, crystals, and ceramics have minimal plastic deformation ranges. An example of a material with a large plastic deformation range is wet chewing gum, which can be stretched to dozens of times its original length.

Under tensile stress, plastic deformation is characterized by a strain hardening region and a necking region and finally, fracture (also called rupture). During strain hardening the material becomes stronger through the movement of atomic dislocations. The necking phase is indicated by a reduction in cross-sectional area of the specimen. Necking begins after the ultimate strength is reached. During necking, the material can no longer withstand the maximum stress and the strain in the specimen rapidly increases. Plastic deformation ends with the fracture of the material.

Compressive failure

Usually, compressive stress applied to bars, columns, etc. leads to shortening.

Loading a structural element or specimen will increase the compressive stress until it reaches its compressive strength. According to the properties of the material, failure modes are yielding for materials with ductile behavior (most metals, some soils and plastics) or rupturing for brittle behavior (geomaterials, cast iron, glass, etc.).

In long, slender structural elements — such as columns or truss bars — an increase of compressive force F leads to structural failure due to buckling at lower stress than the compressive strength.

Fracture

See also: Concrete fracture analysis and Fracture mechanics

This type of deformation is also irreversible. A break occurs after the material has reached the end of the elastic, and then plastic, deformation ranges. At this point forces accumulate until they are sufficient to cause a fracture. All materials will eventually fracture, if sufficient forces are applied.

Misconceptions

A popular misconception is that all materials that bend are "weak" and those that don't are "strong". In reality, many materials that undergo large elastic and plastic deformations, such as steel, are able to absorb stresses that would cause brittle materials, such as glass, with minimal plastic deformation ranges, to break.[6]

See also

• Artificial cranial deformation
• Buff strength
• Creep (deformation)
• Deflection (engineering)
• Deformation (mechanics)
• Deformation mechanism maps
• Deformation monitoring
• Deformation retract
• Deformation theory
• Elasticity
• Malleability
• Planar deformation features
• Plasticity (physics)
• Poisson's ratio
• Strain tensor
• Strength of materials
• Wood warping

References

1. ^ Rees, David (2006). Basic Engineering Plasticity: An Introduction with Engineering and Manufacturing Applications. Butterworth-Heinemann. p. 41. ISBN 0-7506-8025-3. Archived from the original on 2017-12-22.
2. ^ Callister, William D. (2004) Fundamentals of Materials Science and Engineering, John Wiley and Sons, 2nd ed. p. 184. ISBN 0-471-66081-7.
3. ^ a b Courtney, Thomas (2000). Mechanical Behavior of Materials. Illinois: Waveland Press. p. 165. ISBN 9780073228242.
4. ^ "True Stress and Strain" (PDF).
5. ^ Roland, David. "STRESS-STRAIN CURVES" (PDF). MIT.
6. ^ Rice, Peter and Dutton, Hugh (1995). Structural glass. Taylor & Francis. p. 33. ISBN 0-419-19940-3.{{cite book}}: CS1 maint: multiple names: authors list (link)

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