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Depending on the constitutive relation, some components of the
fields and stays continuous everywhere in a laminate while the
other component are only piece-wise continuous.
Example
For example, consider conducting materials. The normal component of the
current and the tangent component(s) of the electrical field are
continuous, the remaining components are discontinuous.
- Generally, the vector field
is subject to some differential constraints (the vectors may be
divergencefree, curlfree, etc.) These constraints imply that some linear
combinations of its components are continuous on
the boundary between layers,
|
(3) |
Here is a matrix projector on the subspace of continuous
components.
The components of are constant in the
laminate and
the the supplementary orthogonal components of
jump on the boundary between layers.
|
(4) |
Projections and are mutually orthogonal:
- The dual vector has the properties similar to the vector
, but its discontinuous components are supplementary to those of
the prime vector ; in other words, the continuous and
discontinuous components
of and switch their places:
|
(5) |
The next Table shows discontinuous components of the fields in
the equations of interest.
These component are completely defined by the normal to the laminate.
The matrix projects vector onto as follows:
Table 1:
Space of discontinuous components of the fields in various
equilibria
Process |
Properties tensor |
Field vector |
Subspace
of discontinuous
components |
Conductivity |
Conductivity tensor |
Curlfree field |
normal |
Conductivity |
Resistivity tensor |
Divergencefree current
|
tangent(s)
|
2D Elasticity |
Stiffness tensor |
Strain
|
the tensorial component
|
2D Elasticity |
Compliance tensor |
Stress |
two tensorial
components
|
3D Elasticity |
Stiffness tensor |
Strain |
Three tensorial
components
|
3D Elasticity |
Compliance tensor |
Stress |
Three tensorial
components
|
Maxwell equations |
|
. |
|
|
|
|
|
|
Next: Effective properties and local
Up: Simple laminates
Previous: Equilibrium
Andre Cherkaev
2001-07-31