Constitutive equations describe how materials behave under different conditions. They're crucial for understanding how stuff reacts to forces and deformations. This topic covers various material types, from simple elastic to complex fluids.
We'll look at models for elastic, hyperelastic, viscoelastic, and plastic materials. We'll also dive into fluid mechanics , exploring key equations and applications. This knowledge is essential for tackling real-world engineering problems.
Elastic and Hyperelastic Materials
Characteristics and Behavior of Elastic Materials
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Elastic materials return to original shape after deformation when stress is removed
Exhibit linear relationship between stress and strain up to elastic limit
Obey Hooke's law σ = E ϵ \sigma = E\epsilon σ = E ϵ where σ \sigma σ represents stress, E E E represents Young's modulus , and ϵ \epsilon ϵ represents strain
Young's modulus measures material stiffness, varies for different materials (steel, rubber, wood)
Poisson's ratio ν \nu ν describes lateral contraction when material is stretched longitudinally
Common elastic materials include metals, ceramics, and some polymers
Hyperelastic Material Models and Applications
Hyperelastic materials exhibit nonlinear stress-strain relationship
Can undergo large deformations without permanent changes
Neo-Hookean model describes incompressible, isotropic hyperelastic materials
Strain energy density function: W = μ 2 ( I 1 − 3 ) W = \frac{\mu}{2}(I_1 - 3) W = 2 μ ( I 1 − 3 )
μ \mu μ represents shear modulus, I 1 I_1 I 1 is first invariant of left Cauchy-Green deformation tensor
Mooney-Rivlin model extends Neo-Hookean model for better accuracy
Strain energy density function: W = C 1 ( I 1 − 3 ) + C 2 ( I 2 − 3 ) W = C_1(I_1 - 3) + C_2(I_2 - 3) W = C 1 ( I 1 − 3 ) + C 2 ( I 2 − 3 )
C 1 C_1 C 1 and C 2 C_2 C 2 are material constants, I 2 I_2 I 2 is second invariant of left Cauchy-Green deformation tensor
Applications include modeling rubber, soft tissues, and elastomers
Viscoelastic and Plastic Materials
Viscoelastic Material Behavior and Models
Viscoelastic materials exhibit both viscous and elastic characteristics
Time-dependent response to applied stress or strain
Creep occurs under constant stress, stress relaxation under constant strain
Maxwell model represents viscoelastic fluids using spring and dashpot in series
Kelvin-Voigt model represents viscoelastic solids using spring and dashpot in parallel
Standard Linear Solid model combines Maxwell and Kelvin-Voigt models for improved accuracy
Applications include polymers, biological tissues, and some metals at high temperatures
Plastic materials undergo permanent deformation when stress exceeds yield strength
Elastic-plastic behavior includes both elastic and plastic regions
Yield criteria determine when plastic deformation begins
Von Mises yield criterion based on distortion energy theory
Tresca yield criterion based on maximum shear stress theory
Strain hardening occurs as material becomes stronger during plastic deformation
Bauschinger effect describes changes in yield strength during cyclic loading
Applications include metal forming processes, structural analysis, and material selection for engineering design
Fluid Mechanics
Fundamental Concepts and Governing Equations
Fluid mechanics studies behavior of liquids and gases under various conditions
Fluids classified as Newtonian (linear stress-strain rate relationship) or non-Newtonian
Continuity equation expresses conservation of mass in fluid flow
Momentum equation derived from Newton's second law applied to fluid element
Energy equation based on first law of thermodynamics for fluid systems
Navier-Stokes equations describe motion of viscous fluid substances
Consist of continuity equation and momentum equations
For incompressible Newtonian fluids: ρ ( ∂ u ∂ t + u ⋅ ∇ u ) = − ∇ p + μ ∇ 2 u + f \rho(\frac{\partial \mathbf{u}}{\partial t} + \mathbf{u} \cdot \nabla\mathbf{u}) = -\nabla p + \mu\nabla^2\mathbf{u} + \mathbf{f} ρ ( ∂ t ∂ u + u ⋅ ∇ u ) = − ∇ p + μ ∇ 2 u + f
ρ \rho ρ represents fluid density, u \mathbf{u} u velocity vector, p p p pressure, μ \mu μ dynamic viscosity, f \mathbf{f} f body forces
Applications and Specialized Areas in Fluid Mechanics
Aerodynamics studies air flow around objects (aircraft, vehicles)
Hydrodynamics focuses on liquid flow (ship design, hydraulic systems)
Computational Fluid Dynamics (CFD) uses numerical methods to solve fluid flow problems
Microfluidics deals with behavior of fluids at microscale (lab-on-a-chip devices)
Multiphase flow involves simultaneous flow of materials with different phases or chemical properties
Rheology studies flow of complex fluids with both solid and liquid characteristics (blood, polymers)