Continuum mechanics
Continuum mechanics  

Laws




Continuum mechanics is a branch of mechanics that deals with the analysis of the kinematics and the mechanical behavior of materials modeled as a continuous mass rather than as discrete particles. The French mathematician AugustinLouis Cauchy was the first to formulate such models in the 19th century. Research in the area continues today.
Contents
Explanation
Classical mechanics 

Branches

Core topics

Modeling an object as a continuum assumes that the substance of the object completely fills the space it occupies. Modeling objects in this way ignores the fact that matter is made of atoms, and so is not continuous; however, on length scales much greater than that of interatomic distances, such models are highly accurate. Fundamental physical laws such as the conservation of mass, the conservation of momentum, and the conservation of energy may be applied to such models to derive differential equations describing the behavior of such objects, and some information about the particular material studied is added through constitutive relations.
Continuum mechanics deals with physical properties of solids and fluids which are independent of any particular coordinate system in which they are observed. These physical properties are then represented by tensors, which are mathematical objects that have the required property of being independent of coordinate system. These tensors can be expressed in coordinate systems for computational convenience.
Concept of a continuum
Materials, such as solids, liquids and gases, are composed of molecules separated by "empty" space. On a microscopic scale, materials have cracks and discontinuities. However, certain physical phenomena can be modeled assuming the materials exist as a continuum, meaning the matter in the body is continuously distributed and fills the entire region of space it occupies. A continuum is a body that can be continually subdivided into infinitesimal elements with properties being those of the bulk material.
The validity of the continuum assumption may be verified by a theoretical analysis, in which either some clear periodicity is identified or statistical homogeneity and ergodicity of the microstructure exists. More specifically, the continuum hypothesis/assumption hinges on the concepts of a representative volume element (RVE) (sometimes called "representative elementary volume") and separation of scales based on the Hill–Mandel condition. This condition provides a link between an experimentalist's and a theoretician's viewpoint on constitutive equations (linear and nonlinear elastic/inelastic or coupled fields) as well as a way of spatial and statistical averaging of the microstructure.^{[1]}
When the separation of scales does not hold, or when one wants to establish a continuum of a finer resolution than that of the RVE size, one employs a statistical volume element (SVE), which, in turn, leads to random continuum fields. The latter then provide a micromechanics basis for stochastic finite elements (SFE). The levels of SVE and RVE link continuum mechanics to statistical mechanics. The RVE may be assessed only in a limited way via experimental testing: when the constitutive response becomes spatially homogeneous.
Specifically for fluids, the Knudsen number is used to assess to what extent the approximation of continuity can be made.
Car traffic is an introductory example
Consider car traffic on a highwaywith just one lane for simplicity. Somewhat surprisingly, and in a tribute to its effectiveness, continuum mechanics effectively models the movement of cars via a partial differential equation (PDE) for the density of cars. The familiarity of this situation empowers us to understand a little of the continuumdiscrete dichotomy underlying continuum modelling in general.
To start modelling define that: measure distance (in km) along the highway; is time (in minutes); is the density of cars on the highway (in cars/km in the lane); and is the flow velocity (average velocity) of those cars 'at' position .
Conservation derives a PDE
Cars do not appear and disappear. Consider any group of cars: from the particular car at the back of the group located at to the particular car at the front located at . The total number of cars in this group . Since cars are conserved (if there is overtaking, then the `car at the front \ back' may become a different car) . But via the fundamental theorem of calculus
This integral being zero holds for all groups, that is, for all intervals . The only way an integral can be zero for all intervals is if the integrand is zero for all . Consequently, conservation derives the first order nonlinear conservation PDE
for all positions on the highway.
This conservation PDE applies not only to car traffic but also to fluids, solids, crowds, animals, plants, bushfires, financial traders, and so on.
Observation closes the problem
This PDE is one equation with two unknowns, so we need another equation to form a well posed problem. Such an extra equation is typically needed in continuum mechanics and typically comes from experiments. For car traffic it is well established that cars typically travel at a speed depending upon density, for some experimentally determined function that is a decreasing function of density. For example, experiments in the Lincoln Tunnel, New York, found that a good fit (except at low density) is obtained by (km/hr for density in cars/km).^{[2]}
Thus the basic continuum model for car traffic is the PDE
for the car density on the highway.
Major areas of continuum mechanics
Continuum mechanics The study of the physics of continuous materials 
Solid mechanics The study of the physics of continuous materials with a defined rest shape. 
Elasticity Describes materials that return to their rest shape after applied stresses are removed. 

Plasticity Describes materials that permanently deform after a sufficient applied stress. 
Rheology The study of materials with both solid and fluid characteristics. 

Fluid mechanics The study of the physics of continuous materials which deform when subjected to a force. 
NonNewtonian fluids do not undergo strain rates proportional to the applied shear stress.  
Newtonian fluids undergo strain rates proportional to the applied shear stress. 
An additional area of continuum mechanics comprises elastomeric foams, which exhibit a curious hyperbolic stressstrain relationship. The elastomer is a true continuum, but a homogeneous distribution of voids gives it unusual properties.^{[3]}
Formulation of models
Continuum mechanics models begin by assigning a region in threedimensional Euclidean space to the material body being modeled. The points within this region are called particles or material points. Different configurations or states of the body correspond to different regions in Euclidean space. The region corresponding to the body's configuration at time is labeled .
A particular particle within the body in a particular configuration is characterized by a position vector
where are the coordinate vectors in some frame of reference chosen for the problem (See figure 1). This vector can be expressed as a function of the particle position in some reference configuration, for example the configuration at the initial time, so that
This function needs to have various properties so that the model makes physical sense. needs to be:
 continuous in time, so that the body changes in a way which is realistic,
 globally invertible at all times, so that the body cannot intersect itself,
 orientationpreserving, as transformations which produce mirror reflections are not possible in nature.
For the mathematical formulation of the model, is also assumed to be twice continuously differentiable, so that differential equations describing the motion may be formulated.
Forces in a continuum
Continuum mechanics deals with deformable bodies, as opposed to rigid bodies. A solid is a deformable body that possesses shear strength, sc. a solid can support shear forces (forces parallel to the material surface on which they act). Fluids, on the other hand, do not sustain shear forces. For the study of the mechanical behavior of solids and fluids these are assumed to be continuous bodies, which means that the matter fills the entire region of space it occupies, despite the fact that matter is made of atoms, has voids, and is discrete. Therefore, when continuum mechanics refers to a point or particle in a continuous body it does not describe a point in the interatomic space or an atomic particle, rather an idealized part of the body occupying that point.
Following the classical dynamics of Newton and Euler, the motion of a material body is produced by the action of externally applied forces which are assumed to be of two kinds: surface forces and body forces .^{[4]} Thus, the total force applied to a body or to a portion of the body can be expressed as:
Surface forces or contact forces, expressed as force per unit area, can act either on the bounding surface of the body, as a result of mechanical contact with other bodies, or on imaginary internal surfaces that bound portions of the body, as a result of the mechanical interaction between the parts of the body to either side of the surface (EulerCauchy's stress principle). When a body is acted upon by external contact forces, internal contact forces are then transmitted from point to point inside the body to balance their action, according to Newton's second law of motion of conservation of linear momentum and angular momentum (for continuous bodies these laws are called the Euler's equations of motion). The internal contact forces are related to the body's deformation through constitutive equations. The internal contact forces may be mathematically described by how they relate to the motion of the body, independent of the body's material makeup.^{[5]}
The distribution of internal contact forces throughout the volume of the body is assumed to be continuous. Therefore, there exists a contact force density or Cauchy traction field ^{[4]} that represents this distribution in a particular configuration of the body at a given time . It is not a vector field because it depends not only on the position of a particular material point, but also on the local orientation of the surface element as defined by its normal vector .^{[6]}
Any differential area with normal vector of a given internal surface area , bounding a portion of the body, experiences a contact force arising from the contact between both portions of the body on each side of , and it is given by
where is the surface traction,^{[7]} also called stress vector,^{[8]} traction,^{[9]} or traction vector.^{[10]} The stress vector is a frameindifferent vector (see EulerCauchy's stress principle).
The total contact force on the particular internal surface is then expressed as the sum (surface integral) of the contact forces on all differential surfaces :
In continuum mechanics a body is considered stressfree if the only forces present are those interatomic forces (ionic, metallic, and van der Waals forces) required to hold the body together and to keep its shape in the absence of all external influences, including gravitational attraction.^{[10]}^{[11]} Stresses generated during manufacture of the body to a specific configuration are also excluded when considering stresses in a body. Therefore, the stresses considered in continuum mechanics are only those produced by deformation of the body, sc. only relative changes in stress are considered, not the absolute values of stress.
Body forces are forces originating from sources outside of the body^{[12]} that act on the volume (or mass) of the body. Saying that body forces are due to outside sources implies that the interaction between different parts of the body (internal forces) are manifested through the contact forces alone.^{[7]} These forces arise from the presence of the body in force fields, e.g. gravitational field (gravitational forces) or electromagnetic field (electromagnetic forces), or from inertial forces when bodies are in motion. As the mass of a continuous body is assumed to be continuously distributed, any force originating from the mass is also continuously distributed. Thus, body forces are specified by vector fields which are assumed to be continuous over the entire volume of the body,^{[13]} i.e. acting on every point in it. Body forces are represented by a body force density (per unit of mass), which is a frameindifferent vector field.
In the case of gravitational forces, the intensity of the force depends on, or is proportional to, the mass density of the material, and it is specified in terms of force per unit mass () or per unit volume (). These two specifications are related through the material density by the equation . Similarly, the intensity of electromagnetic forces depends upon the strength (electric charge) of the electromagnetic field.
The total body force applied to a continuous body is expressed as
Body forces and contact forces acting on the body lead to corresponding moments of force (torques) relative to a given point. Thus, the total applied torque about the origin is given by
In certain situations, not commonly considered in the analysis of the mechanical behavior of materials, it becomes necessary to include two other types of forces: these are body moments and couple stresses^{[14]}^{[15]} (surface couples,^{[12]} contact torques^{[13]}). Body moments, or body couples, are moments per unit volume or per unit mass applied to the volume of the body. Couple stresses are moments per unit area applied on a surface. Both are important in the analysis of stress for a polarized dielectric solid under the action of an electric field, materials where the molecular structure is taken into consideration (e.g. bones), solids under the action of an external magnetic field, and the dislocation theory of metals.^{[8]}^{[9]}^{[12]}
Materials that exhibit body couples and couple stresses in addition to moments produced exclusively by forces are called polar materials.^{[9]}^{[13]} Nonpolar materials are then those materials with only moments of forces. In the classical branches of continuum mechanics the development of the theory of stresses is based on nonpolar materials.
Thus, the sum of all applied forces and torques (with respect to the origin of the coordinate system) in the body can be given by
Kinematics: deformation and motion
A change in the configuration of a continuum body results in a displacement. The displacement of a body has two components: a rigidbody displacement and a deformation. A rigidbody displacement consists of a simultaneous translation and rotation of the body without changing its shape or size. Deformation implies the change in shape and/or size of the body from an initial or undeformed configuration to a current or deformed configuration (Figure 2).
The motion of a continuum body is a continuous time sequence of displacements. Thus, the material body will occupy different configurations at different times so that a particle occupies a series of points in space which describe a pathline.
There is continuity during deformation or motion of a continuum body in the sense that:
 The material points forming a closed curve at any instant will always form a closed curve at any subsequent time.
 The material points forming a closed surface at any instant will always form a closed surface at any subsequent time and the matter within the closed surface will always remain within.
It is convenient to identify a reference configuration or initial condition which all subsequent configurations are referenced from. The reference configuration need not be one that the body will ever occupy. Often, the configuration at is considered the reference configuration, . The components of the position vector of a particle, taken with respect to the reference configuration, are called the material or reference coordinates.
When analyzing the deformation or motion of solids, or the flow of fluids, it is necessary to describe the sequence or evolution of configurations throughout time. One description for motion is made in terms of the material or referential coordinates, called material description or Lagrangian description.
Lagrangian description
In the Lagrangian description the position and physical properties of the particles are described in terms of the material or referential coordinates and time. In this case the reference configuration is the configuration at . An observer standing in the referential frame of reference observes the changes in the position and physical properties as the material body moves in space as time progresses. The results obtained are independent of the choice of initial time and reference configuration, . This description is normally used in solid mechanics.
In the Lagrangian description, the motion of a continuum body is expressed by the mapping function (Figure 2),
which is a mapping of the initial configuration onto the current configuration , giving a geometrical correspondence between them, i.e. giving the position vector that a particle , with a position vector in the undeformed or reference configuration , will occupy in the current or deformed configuration at time . The components are called the spatial coordinates.
Physical and kinematic properties , i.e. thermodynamic properties and flow velocity, which describe or characterize features of the material body, are expressed as continuous functions of position and time, i.e. .
The material derivative of any property of a continuum, which may be a scalar, vector, or tensor, is the time rate of change of that property for a specific group of particles of the moving continuum body. The material derivative is also known as the substantial derivative, or comoving derivative, or convective derivative. It can be thought as the rate at which the property changes when measured by an observer traveling with that group of particles.
In the Lagrangian description, the material derivative of is simply the partial derivative with respect to time, and the position vector is held constant as it does not change with time. Thus, we have
The instantaneous position is a property of a particle, and its material derivative is the instantaneous flow velocity of the particle. Therefore, the flow velocity field of the continuum is given by
Similarly, the acceleration field is given by
Continuity in the Lagrangian description is expressed by the spatial and temporal continuity of the mapping from the reference configuration to the current configuration of the material points. All physical quantities characterizing the continuum are described this way. In this sense, the function and are singlevalued and continuous, with continuous derivatives with respect to space and time to whatever order is required, usually to the second or third.
Eulerian description
Continuity allows for the inverse of to trace backwards where the particle currently located at was located in the initial or referenced configuration . In this case the description of motion is made in terms of the spatial coordinates, in which case is called the spatial description or Eulerian description, i.e. the current configuration is taken as the reference configuration.
The Eulerian description, introduced by d'Alembert, focuses on the current configuration , giving attention to what is occurring at a fixed point in space as time progresses, instead of giving attention to individual particles as they move through space and time. This approach is conveniently applied in the study of fluid flow where the kinematic property of greatest interest is the rate at which change is taking place rather than the shape of the body of fluid at a reference time.^{[16]}
Mathematically, the motion of a continuum using the Eulerian description is expressed by the mapping function
which provides a tracing of the particle which now occupies the position in the current configuration to its original position in the initial configuration .
A necessary and sufficient condition for this inverse function to exist is that the determinant of the Jacobian Matrix, often referred to simply as the Jacobian, should be different from zero. Thus,
In the Eulerian description, the physical properties are expressed as
where the functional form of in the Lagrangian description is not the same as the form of in the Eulerian description.
The material derivative of , using the chain rule, is then
The first term on the righthand side of this equation gives the local rate of change of the property occurring at position . The second term of the righthand side is the convective rate of change and expresses the contribution of the particle changing position in space (motion).
Continuity in the Eulerian description is expressed by the spatial and temporal continuity and continuous differentiability of the flow velocity field. All physical quantities are defined this way at each instant of time, in the current configuration, as a function of the vector position .
Displacement field
The vector joining the positions of a particle in the undeformed configuration and deformed configuration is called the displacement vector , in the Lagrangian description, or , in the Eulerian description.
A displacement field is a vector field of all displacement vectors for all particles in the body, which relates the deformed configuration with the undeformed configuration. It is convenient to do the analysis of deformation or motion of a continuum body in terms of the displacement field, In general, the displacement field is expressed in terms of the material coordinates as
or in terms of the spatial coordinates as
where are the direction cosines between the material and spatial coordinate systems with unit vectors and , respectively. Thus
and the relationship between and is then given by
Knowing that
then
It is common to superimpose the coordinate systems for the undeformed and deformed configurations, which results in , and the direction cosines become Kronecker deltas, i.e.
Thus, we have
or in terms of the spatial coordinates as
Governing equations
Continuum mechanics deals with the behavior of materials that can be approximated as continuous for certain length and time scales. The equations that govern the mechanics of such materials include the balance laws for mass, momentum, and energy. Kinematic relations and constitutive equations are needed to complete the system of governing equations. Physical restrictions on the form of the constitutive relations can be applied by requiring that the second law of thermodynamics be satisfied under all conditions. In the continuum mechanics of solids, the second law of thermodynamics is satisfied if the Clausius–Duhem form of the entropy inequality is satisfied.
The balance laws express the idea that the rate of change of a quantity (mass, momentum, energy) in a volume must arise from three causes:
 the physical quantity itself flows through the surface that bounds the volume,
 there is a source of the physical quantity on the surface of the volume, or/and,
 there is a source of the physical quantity inside the volume.
Let be the body (an open subset of Euclidean space) and let be its surface (the boundary of ).
Let the motion of material points in the body be described by the map
where is the position of a point in the initial configuration and is the location of the same point in the deformed configuration.
The deformation gradient is given by
Balance laws
Let be a physical quantity that is flowing through the body. Let be sources on the surface of the body and let be sources inside the body. Let be the outward unit normal to the surface . Let be the flow velocity of the physical particles that carry the physical quantity that is flowing. Also, let the speed at which the bounding surface is moving be (in the direction ).
Then, balance laws can be expressed in the general form
Note that the functions , , and can be scalar valued, vector valued, or tensor valued  depending on the physical quantity that the balance equation deals with. If there are internal boundaries in the body, jump discontinuities also need to be specified in the balance laws.
If we take the Eulerian point of view, it can be shown that the balance laws of mass, momentum, and energy for a solid can be written as (assuming the source term is zero for the mass and angular momentum equations)
In the above equations is the mass density (current), is the material time derivative of , is the particle velocity, is the material time derivative of , is the Cauchy stress tensor, is the body force density, is the internal energy per unit mass, is the material time derivative of , is the heat flux vector, and is an energy source per unit mass.
With respect to the reference configuration (the Lagrangian point of view), the balance laws can be written as
In the above, is the first PiolaKirchhoff stress tensor, and is the mass density in the reference configuration. The first PiolaKirchhoff stress tensor is related to the Cauchy stress tensor by
We can alternatively define the nominal stress tensor which is the transpose of the first PiolaKirchhoff stress tensor such that
Then the balance laws become
The operators in the above equations are defined as such that
where is a vector field, is a secondorder tensor field, and are the components of an orthonormal basis in the current configuration. Also,
where is a vector field, is a secondorder tensor field, and are the components of an orthonormal basis in the reference configuration.
The inner product is defined as
Clausius–Duhem inequality
The Clausius–Duhem inequality can be used to express the second law of thermodynamics for elasticplastic materials. This inequality is a statement concerning the irreversibility of natural processes, especially when energy dissipation is involved.
Just like in the balance laws in the previous section, we assume that there is a flux of a quantity, a source of the quantity, and an internal density of the quantity per unit mass. The quantity of interest in this case is the entropy. Thus, we assume that there is an entropy flux, an entropy source, and an internal entropy density per unit mass () in the region of interest.
Let be such a region and let be its boundary. Then the second law of thermodynamics states that the rate of increase of in this region is greater than or equal to the sum of that supplied to (as a flux or from internal sources) and the change of the internal entropy density due to material flowing in and out of the region.
Let move with a flow velocity and let particles inside have velocities . Let be the unit outward normal to the surface . Let be the density of matter in the region, be the entropy flux at the surface, and be the entropy source per unit mass. Then the entropy inequality may be written as
The scalar entropy flux can be related to the vector flux at the surface by the relation . Under the assumption of incrementally isothermal conditions, we have
where is the heat flux vector, is an energy source per unit mass, and is the absolute temperature of a material point at at time .
We then have the Clausius–Duhem inequality in integral form:
We can show that the entropy inequality may be written in differential form as
In terms of the Cauchy stress and the internal energy, the Clausius–Duhem inequality may be written as
Applications
See also
 Bernoulli's principle
 Cauchy elastic material
 Configurational mechanics
 Curvilinear coordinates
 Equation of state
 Finite deformation tensors
 Finite strain theory
 Hyperelastic material
 Lagrangian and Eulerian specification of the flow field
 Movable cellular automaton
 Peridynamics (a nonlocal continuum theory leading to integral equations)
 Stress (physics)
 Stress measures
 Tensor calculus
 Tensor derivative (continuum mechanics)
 Theory of elasticity
Notes
 ↑ OstojaStarzewski, M. (2008). "710". Microstructural randomness and scaling in mechanics of materials. CRC Press. ISBN 1584884177.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 ↑ A. J. Roberts, A onedimensional introduction to continuum mechanics, World Scientific, 1994
 ↑ Dienes, J. K.; Solem, Johndale C. (1999). "Nonlinear behavior of some hydrostatically stressed isotropic elastomeric foams". Acta Mechanica. 138: 155–162.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 ↑ ^{4.0} ^{4.1} Smith & Truesdell p.97
 ↑ Slaughter
 ↑ Lubliner
 ↑ ^{7.0} ^{7.1} Liu
 ↑ ^{8.0} ^{8.1} Wu
 ↑ ^{9.0} ^{9.1} ^{9.2} Fung
 ↑ ^{10.0} ^{10.1} Mase
 ↑ Atanackovic
 ↑ ^{12.0} ^{12.1} ^{12.2} Irgens
 ↑ ^{13.0} ^{13.1} ^{13.2} Chadwick
 ↑ Maxwell pointed out that nonvanishing body moments exist in a magnet in a magnetic field and in a dielectric material in an electric field with different planes of polarization. Fung p.76.
 ↑ Couple stresses and body couples were first explored by Voigt and Cosserat, and later reintroduced by Mindlin in 1960 on his work for Bell Labs on pure quartz crystals. Richards p.55.
 ↑ Spencer, A.J.M. (1980). Continuum Mechanics. Longman Group Limited (London). p. 83. ISBN 0582442826.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
References
 Batra, R. C. (2006). Elements of Continuum Mechanics. Reston, VA: AIAA.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Chandramouli, P.N (2014). Continuum Mechanics. Yes Dee Publishing Pvt Ltd. ISBN 9789380381398.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Eringen, A. Cemal (1980). Mechanics of Continua (2nd ed.). Krieger Pub Co. ISBN 088275663X.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Chen, Youping; James D. Lee; Azim Eskandarian (2009). Meshless Methods in Solid Mechanics (First ed.). Springer New York. ISBN 1441921486.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Dill, Ellis Harold (2006). Continuum Mechanics: Elasticity, Plasticity, Viscoelasticity. Germany: CRC Press. ISBN 0849397790.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Dimitrienko, Yuriy (2011). Nonlinear Continuum Mechanics and Large Inelastic Deformations. Germany: Springer. ISBN 9789400700338.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Hutter, Kolumban; Klaus Jöhnk (2004). Continuum Methods of Physical Modeling. Germany: Springer. ISBN 3540206191.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Fung, Y. C. (1977). A First Course in Continuum Mechanics (2nd ed.). PrenticeHall, Inc. ISBN 0133183114.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Gurtin, M. E. (1981). An Introduction to Continuum Mechanics. New York: Academic Press.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Lai, W. Michael; David Rubin; Erhard Krempl (1996). Introduction to Continuum Mechanics (3rd ed.). Elsevier, Inc. ISBN 9780750628945.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>^{[dead link]}
 Lubarda, Vlado A. (2001). Elastoplasticity Theory. CRC Press. ISBN 0849311381.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Lubliner, Jacob (2008). Plasticity Theory (Revised Edition) (PDF). Dover Publications. ISBN 0486462900.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Malvern, Lawrence E. (1969). Introduction to the mechanics of a continuous medium. New Jersey: PrenticeHall, Inc.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Mase, George E. (1970). Continuum Mechanics. McGrawHill Professional. ISBN 0070406634.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Mase, G. Thomas; George E. Mase (1999). Continuum Mechanics for Engineers (Second ed.). CRC Press. ISBN 0849318556.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Maugin, G. A. (1999). The Thermomechanics of Nonlinear Irreversible Behaviors: An Introduction. Singapore: World Scientific.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 NematNasser, Sia (2006). Plasticity: A Treatise on Finite Deformation of Heterogeneous Inelastic Materials. Cambridge: Cambridge University Press. ISBN 0521839793.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 OstojaStarzewski, Martin (2008). Microstructural Randomness and Scaling in Mechanics of Materials. Boca Raton, FL: Chapman & Hall/CRC Press. ISBN 9781584884170.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Rees, David (2006). Basic Engineering Plasticity  An Introduction with Engineering and Manufacturing Applications. ButterworthHeinemann. ISBN 0750680253.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>
 Wright, T. W. (2002). The Physics and Mathematics of Adiabatic Shear Bands. Cambridge, UK: Cambridge University Press.<templatestyles src="Module:Citation/CS1/styles.css"></templatestyles>