Navier–Cauchy equations

E702911

The Navier–Cauchy equations are the fundamental partial differential equations in linear elasticity that describe how stresses and displacements are related within deformable solid materials.

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Navier–Cauchy equations canonical 1

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Predicate Object
instanceOf elasticity equation
equations of motion
system of partial differential equations
appliesTo homogeneous elastic materials
isotropic elastic materials
linearly elastic materials
assumes continuum hypothesis
linear stress–strain relationship
small deformations
basedOn Cauchy momentum equation NERFINISHED
Hooke's law for linear elasticity NERFINISHED
canBeExpressedIn Cartesian coordinates NERFINISHED
cylindrical coordinates
spherical coordinates
describes equilibrium and motion of elastic bodies
relationship between stresses and displacements in deformable solids
field continuum mechanics
linear elasticity
solid mechanics
governs dynamic elasticity problems
static elasticity problems
hasAlternativeName Cauchy–Navier equations NERFINISHED
Navier equations of elasticity NERFINISHED
hasForm vector partial differential equation
implies stress distribution in the body when combined with constitutive relations
mathematicalNature second-order linear partial differential equations
namedAfter Augustin-Louis Cauchy NERFINISHED
Claude-Louis Navier NERFINISHED
relatedTo Navier–Stokes equations NERFINISHED
wave equation in elastic media
relates displacement gradients to internal stresses
requires boundary conditions
initial conditions for dynamic problems
solutionRepresents displacement field in an elastic body
specialCaseOf general equations of motion in continuum mechanics
usedIn civil engineering
geophysics
materials science
mechanical engineering
seismology
structural analysis
usesConcept Lamé parameters NERFINISHED
Poisson's ratio NERFINISHED
Young's modulus NERFINISHED
body force density
displacement field
strain tensor
stress tensor

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Claude-Louis notableConcept Navier–Cauchy equations
subject surface form: Claude-Louis Navier