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Lecture 21Energy principles and stability
Instructor: Prof. Marcial Gonzalez
Spring, 2015ME 612 – Continuum Mechanics
September 21, 2021
Lecture 21 – Energy principles and stability
Experimental mechanics and
thermodynamics
Tensor algebra Tensor analysis
reference configuration
thermo-mechanical loads
KINEMATICS OF DEFORMATIONS deformed configuration
CONTINUOUSMEDIA
atomic/micro/meso
structureis revealed
16 unknown fields + 5 equations
laws of nature .CONSERVATION OF MASS
BALANCE OF LINEAR MOMENTUMBALANCE OF ANGULAR MOMENTUM
LAWS OF THERMODYNAMICS CONSTITUTIVE EQUATIONS11 equations
Empirical observation
Multi-scaleapproaches
continuously varying fields(time and space averages over the underlying structure)
2
3
Static equilibrium – Boundary value problem- Conservation of linear momentum
reference configuration
deformed configuration
CONTINUOUSMEDIA
Note: conservative body forces and dead loads.
DIY
Lecture 21 – Energy principles and stability
4
Static equilibrium – Boundary value problem- Conservation of linear momentum
- Airy stress function: plain stress, Cartesian coordinate system
reference configuration
deformed configuration
CONTINUOUSMEDIA
Lecture 21 – Energy principles and stability
5
Static equilibrium – Boundary value problem- Airy stress function: plain stress, polar coordinate system
General solution:
Lecture 21 – Energy principles and stability
6
Static equilibrium – Variational formulation- Total potential energy (conservative body forces and dead loads)
- An admissible deformation mapping is such that
- Principle of stationary potential energy:Given the set of admissible displacement fields for a conservative
system, an equilibrium state will correspond to one for which the potential energy is stationary (or to a minimum for stable solutions).
reference configuration
deformed configuration
CONTINUOUSMEDIA
Lecture 21 – Energy principles and stability
7
Static equilibrium – Variational formulation- Total potential energy (conservative body forces and dead loads)
- An admissible deformation mapping is such that
- Principle of minimum potential energy – Variational principle
reference configuration
deformed configuration
CONTINUOUSMEDIA
Lecture 21 – Energy principles and stability
8
Static equilibrium – Variational formulation- Total potential energy (conservative body forces and dead loads)
- An admissible deformation mapping is such that
- Principle of stationary potential energy – Variational principle
reference configuration
deformed configuration
CONTINUOUSMEDIA
Lecture 21 – Energy principles and stability
9
Static equilibrium – Variational formulation- Principle of stationary potential energy – Variational principle
Proof
reference configuration
deformed configuration
CONTINUOUSMEDIA
Lecture 21 – Energy principles and stability
10
Static equilibrium – Variational formulation- Principle of stationary potential energy – Variational principle
Veinberg’s theorem:
A BVP is variational iff and iff
reference configuration
deformed configuration
CONTINUOUSMEDIA
Lecture 21 – Energy principles and stability
11
Static equilibrium – Stability- Principle of stationary potential energy:
Given the set of admissible displacement fields for a conservative system, an equilibrium state will correspond to one for which the potential energy is stationary
- Stable solution? A stationary point could be a minimum, a maximum or a saddle point.
- Theory of stability of infinite-dimensional spaces is not trivial …
reference configuration
deformed configuration
CONTINUOUSMEDIA
Lecture 21 – Energy principles and stability
12
Static equilibrium – Stability- Stable solution?
A stationary point could be a minimum, a maximum or a saddle point.
- Under the assumptions presented before, stability of an equilibrium configuration can be determined from the stability of the linearized problem about the equilibrium configuration.
- Ultimately, stability can be inferred from the strain energy density!
reference configuration
deformed configuration
CONTINUOUSMEDIA
Lecture 21 – Energy principles and stability
13
Static equilibrium – Stability- Stable solution?
A stationary point could be a minimum, a maximum or a saddle point.- Stability can be inferred from the strain energy density:
+ Necessary condition (but not sufficient) The mixed elastic tensor has to be a rank-one convex tensor, that is the strain energy density has to be rank-one convex.
+ Sufficient conditions come from nonlinear terms and from boundarycondition.
reference configuration
deformed configuration
CONTINUOUSMEDIA
Lecture 21 – Energy principles and stability
14
Static equilibrium – Stability- Examples of rank-one convexity
neo-Hookean material
Saint Venant-Kirchhoff material
Counterexample
reference configuration
deformed configuration
CONTINUOUSMEDIA
DIYcompression
Lecture 21 – Energy principles and stability
15
Load-controlled vs. displacement-controlled experiments
Saint Venant-Kirchhoff material
Blatz-Ko material
DIY
Lecture 21 – Energy principles and stability
Any questions?
16
Lecture 21 – Energy principles and stability