A Kelvin–Voigt material, also called a Voigt material, is a viscoelastic material having the properties both of elasticity and viscosity. It is named after the British physicist and engineer William Thomson, 1st Baron Kelvin and after German physicist Woldemar Voigt.
The Kelvin–Voigt model, also called the Voigt model, can be represented by a purely viscous damper and purely elastic spring connected in parallel as shown in the picture.
If we connect these two elements in series we get a model of a Maxwell material.
Since the two components of the model are arranged in parallel, the strains in each component are identical:
Similarly, the total stress will be the sum of the stress in each component:
Effect of a sudden stress
If we suddenly apply some constant stress to Kelvin–Voigt material, then the deformations would approach the deformation for the pure elastic material with the difference decaying exponentially:
where t is time and the rate of relaxation .
If we would free the material at time , then the elastic element would retard the material back until the deformation becomes zero. The retardation obeys the following equation:
The picture shows the dependence of the dimensionless deformation on dimensionless time . In the picture the stress on the material is loaded at time , and released at the later dimensionless time .
Since all the deformation is reversible (though not suddenly) the Kelvin–Voigt material is a solid.
The Voigt model predicts creep more realistically than the Maxwell model, because in the infinite time limit the strain approaches a constant:
while a Maxwell model predicts a linear relationship between strain and time, which is most often not the case. Although the Kelvin–Voigt model is effective for predicting creep, it is not good at describing the relaxation behavior after the stress load is removed.
The complex dynamic modulus of the Kelvin–Voigt material is given by:
Thus, the real and imaginary components of the dynamic modulus are:
Note that is constant, while is directly proportional to frequency (where the apparent viscosity, , is the constant of proportionality).
- Meyers and Chawla (1999): Section 13.10 of Mechanical Behaviors of Materials, Mechanical behavior of Materials, 570–580. Prentice Hall, Inc.