A linear elastic material is a mathematical model used to analyze the deformation of solid bodies. It is useful to compute the relation between the forces applied on the object and the corresponding change in shape. In other terms, it relates the stresses and the strains in the material.

For a deformation process to be considered linear and elastic, the following conditions must be met:

The deformations, in terms of the material strains, are small.

When the loads are removed, the material naturally returns to its original, undeformed shape. In other words, the material stress level doesn’t reach the yield strength limit.

The magnitude of the deformations are proportional to the applied loads.

A linear elastic material can be seen as the generalization of Hooke’s law for a spring:

$$ F = Ku \tag{1}$$

where:

\(F\) is the tensile force applied to the spring,

\(u\) is the resulting elongation of the spring, and

\(K\) is the stiffness constant, a property of the spring dictated by the material and geometry.

In order to get rid of the geometry dependency of the stiffness, for the sake of generalization, the relation between force and deformation is expressed in terms of stress and strain:

$$ \sigma = \frac{F}{A} \tag{2}$$

$$ \varepsilon = \frac{u}{L} \tag{3}$$

where:

\(\sigma\) is the normal stress on the prismatic object under tensile load: force per unit area,

\(\varepsilon\) is the strain in the material: deformation per unit length,

\(A\) is the constant cross-section area of the object, perpendicular to the load, and

\(L\) is the length of the object in the direction of the load and deformation.

By using these terms, the one-dimensional linear elastic relation can be expressed as:

$$ \sigma = E \varepsilon \tag{4}$$

where \(E\) is the Young’s modulus of the material, the proportional relation between stress and strain:

Linear Elastic Materials in Three Dimensions

In the general case of a solid object subject to loads in multiple directions in space, the one-dimensional relation presented above is no longer sufficient to describe the deformations. In three dimensions, stress and strain are expressed as tensor quantities:

where \(\nu\) is the Poisson’s ratio, which relates normal stresses with deformations in the perpendicular directions. Here, it is assumed that the material is isotropic and homogeneous, which means that the material properties such as \(E\) and \(\nu\) are constants with respect to position and orientation.

Workbench Setup

For the application of a linear elastic material in a structural simulation, the following set of parameters must be specified:

In the Workbench, go to Materials, confirm the Material behavior to Linear Elastic, set the successive parameters and assign them to a volume:

Beyond Linear Elastic Materials

For most of the structural analysis involving metals such as steel and aluminum, if the stresses are below yield strength, linear elastic material model shall be used. However, this model is incapable of truly describing the material behaviour, if the objective of the analysis is to study plasticity. In that case, use Elasto-plastic material model for the analysis. Additionally, there are also materials such as rubbers and elastomers for which the relationship between stress and strain is nonlinear while deforming elastically. For such materials, Hyperelastic material model is the most appropriate choice.

This website uses cookies so that we can provide you with the best user experience possible. Cookie information is stored in your browser and performs functions such as recognising you when you return to our website and helping our team to understand which sections of the website you find most interesting and useful.

Strictly Necessary Cookies

Strictly Necessary Cookie should be enabled at all times so that we can save your preferences for cookie settings.

If you disable this cookie, we will not be able to save your preferences. This means that every time you visit this website you will need to enable or disable cookies again.