Category
page 1Continuum mechanics
tensor
right|thumb|300px|The second-order Cauchy stress tensor \mathbf{T} describes the stress experienced by a material at a given point. For any unit vector \mathbf{v}, the product \mathbf{T} \cdot \mathbf{v} is a vector, denoted \mathbf{T}(\mathbf{v}), that quantifies the force per area along the plane perpendicular to \mathbf{v}. This image shows, for cube faces perpendicular to \mathbf{e}_1, \mathbf{e}_2, \mathbf{e}_3, the corresponding stress vectors \mathbf{T}(\mathbf{e}_1), \mathbf{T}(\mathbf{e}_2), \mathbf{T}(\mathbf{e}_3) along those faces. Because the stress tensor takes one vector as inpu
deformation
transformation of a body from a reference configuration to a current configuration
continuum mechanics
branch of physics which studies the behavior of materials modeled as continuous media
ductility
thumb|Tensile test of an Aluminium–magnesium–silicon alloys|Al-Mg-Si alloy. The local necking and the cup and cone fracture surfaces are typical for ductile metals.
thumb|This tensile test of a Ductile iron|nodular cast iron demonstrates low ductility.
fluid dynamics
subdiscipline of fluid mechanics that deals with fluid flow—the natural science of fluids (liquids and gases) in motion

stiffness
thumb|right|Extension of a coil spring, \delta, caused by an axial force, F.
finite element method
numerical method for solving physical or engineering problems
shear stress
component of stress coplanar with a material cross section
solid mechanics
branch of science that studies the behavior of solid materials

brittleness
thumb|Brittle fracture in glass
thumb|Brittle fracture in cast iron tensile testpieces
A material is brittle if, when subjected to stress, it fractures with little elastic deformation and without significant plastic deformation. Brittle materials absorb relatively little energy prior to fracture, even those of high strength. Breaking is often accompanied by a sharp snapping sound.
non-Newtonian fluid
fluid that does not follow Newton's Law of Viscosity, viscosity (the measure of a fluid's ability to resist gradual deformation by shear or tensile stresses) of non-Newtonian fluids is dependent on shear rate or shear rate history
state function
measurable characteristic of the current state of a thermodynamic system, independent of the history of the system
toughness
thumb|Toughness as defined by the area under the stress–strain curve for one unit volume of the material.
In materials science and metallurgy, toughness is the ability of a material to absorb energy and plastically deform without fracturing. Toughness is the strength with which the material opposes rupture. One definition of material toughness is the amount of energy per unit volume that a material can absorb before rupturing. This measure of toughness is different from that used for fracture toughness, which describes the capacity of materials to resist fracture.
Toughness requires a balance

thixotropy
thumb|Mānuka honey is an example of a thixotropic material.
Thixotropy is a time-dependent shear thinning property. Certain gels or fluids that are thick or viscous under static conditions will flow (become thinner, less viscous) over time when shaken, agitated, shear-stressed, or otherwise stressed (time-dependent viscosity). They then take a fixed time to return to a more viscous state.
Some non-Newtonian pseudoplastic fluids show a time-dependent change in viscosity; the longer the fluid undergoes shear stress, the lower its viscosity. A thixotropic fluid is a fluid which takes a finite tim
viscoelasticity
Viscoelasticity is a material property that combines both viscous and elastic characteristics. Many materials have such viscoelastic properties, especially materials that consist of large molecules. Polymers are viscoelastic because their macromolecules can make temporary entanglements with neighbouring molecules which causes elastic properties. After some time these entanglements will disappear again and the macromolecules will flow into other positions where new entanglements will be made (viscous properties).

vorticity
In continuum mechanics, vorticity is a pseudovector (or axial vector) field that describes the local spinning motion of a continuum near some point (the tendency of something to rotate), as would be seen by an observer located at that point and traveling along with the flow. It is an important quantity in the dynamical theory of fluids and provides a convenient framework for understanding a variety of complex flow phenomena, such as the generation of lift on wings.
compression
application of inward ("pushing") forces to a material or structure
streamline
field lines in a fluid flow
soft tissue
the tissues that connect, support, or surround other structures and organs of the body, not being hard tissue; tendons, ligaments, fascia, skin, fibrous tissues, fat, and synovial membranes (connective tissue), and muscles, nerves and blood vessels
residual stress
remaining stress in a solid material after removal of the original cause
Cauchy stress tensor
tensor that describes the state of stress at a point inside a material
linear strain
relative change of length with respect the original length
bending moment of force
moment that results in the bending of a structural element

OpenFOAM
OpenFOAM (Open Field Operation And Manipulation) is a C++ toolbox for the development of customized numerical solvers, and pre-/post-processing utilities for the solution of continuum mechanics problems, most prominently including computational fluid dynamics (CFD).
shearing
term in mechanics
Eckert number
characteristic number of a fluid for the relation between kinetic energy and enthalpy change

dilatant
thumb|350x350px|Plot of shear rate as a function of the shear stress. Dilatants in green.
A dilatant (, ) (also termed shear thickening) material is one in which viscosity increases with the rate of shear strain. Such a shear thickening fluid, also known by the initialism STF, is an example of a non-Newtonian fluid. This behaviour is usually not observed in pure materials, but can occur in suspensions.
Theorem of corresponding states
assertion that all fluids, when compared at the same reduced temperature and reduced pressure, have approximately the same compressibility factor and all deviate from ideal gas behavior to about the same degree
plasticity theory
solid mechanics theory that is used to describe the plastic behavior of materials
Brinkman number
characteristic number of a fluid for the relation between heat produced by viscosity and heat received from outside by conduction
fluid parcel
very small amount of fluid, identifiable throughout its dynamic history while moving with the fluid flow
Reynolds transport theorem
3D generalization of the Leibniz integral rule
Rankine–Hugoniot conditions
concept in physics
stream function
The stream function is constant along a streamline
constitutive equation
relation between two physical quantities that is specific to a material or substance
Cauchy momentum equation
equation
Cauchy number
characteristic number in continuum mechanics used in the study of compressible flows
control volume
Shear thinning
non-Newtonian fluid behavior
second polar moment of area
moment
Timoshenko beam theory
Model of shear deformation and bending effects
theory of tides
aspect of history
plate theory
mathematical descriptions of the mechanics of flat plates
yield surface
Geometric representation of material yield
shear rate
time derivative of shear strain
shear and moment diagram
structural design tool
finite strain theory
theory
orthotropic material
type of anisotropic material
Mesophase
In chemistry and chemical physics, a mesophase or mesomorphic phase is a phase of matter intermediate between solid and liquid. Gelatin is a common example of a partially ordered structure in a mesophase. Further, biological structures such as the lipid bilayers of cell membranes are examples of mesophases. Mobile ions in mesophases are either orientationally or rotationally disordered while their centers are located at the ordered sites in the crystal structure. Mesophases with long-range positional order but no orientational order are plastic crystals, whereas those with long-range orientati
flexural strength
material property
enstrophy
In fluid dynamics, the enstrophy \mathcal{E} can be interpreted as another type of potential density; or, more concretely, the quantity directly related to the kinetic energy in the flow model that corresponds to dissipation effects in the fluid. It is particularly useful in the study of turbulent flows, and is often identified in the study of thrusters as well as in combustion theory and meteorology.
digital image correlation
Mathematical image techniques
velocity potential
scalar potential used in fluid dynamics
hyperelastic material
material for which the stress–strain relationship derives from a strain energy density function
Betti's theorem
Reciprocal work theorem in engineering
Izod impact strength test
equipment and procedure to measure materials' impact resistance
viscoplasticity
thumb|upright=1.1|Figure 1. Elements used in one-dimensional models of viscoplastic materials.
Damage mechanics
damage to materials due to cyclic mechanical loads

strain rate tensor
physical quantity that describes the rate of change of the deformation of a material
bimoment
Bimoment (aka warping moment) is a term used in the analysis of beams (continuum mechanics) that relates to torsion and warping. Its symbol is Mω.