2012 | OriginalPaper | Chapter
Some Basic Principles of Continuum Mechanics
Author : Tarek I. Zohdi
Published in: Electromagnetic Properties of Multiphase Dielectrics
Publisher: Springer Berlin Heidelberg
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In order to properly consider multifield coupling effects, we will need to draw on some of the tools of classical continuum mechanics.
The term deformation refers to a change in the shape of the continuum between a reference configuration and current configuration. In the reference configuration, a representative particle of the continuum occupies a point
p
in space and has the position vector
$$ {\bf X}=X_1{\bf e}_1+X_2{\bf e}_2+X_3{\bf e}_3\,$$
where
e
1
,
e
2
,
e
3
is a Cartesian reference triad, and
X
1
,
X
2
,
X
3
(with center
O
) can be thought of as labels for a point. Sometimes, the coordinates or labels (
X
1
,
X
2
,
X
3
,
t
) are called the referential coordinates. In the current configuration, the particle originally located at point
P
is located at point
P
′, and can also be expressed in terms of another position vector
x
, with the coordinates (
x
1
,
x
2
,
x
3
,
t
). These are called the current coordinates. It is obvious with this arrangement that the displacement is
u
=
x
–
${\emph \bf X}$
for a point originally at
${\emph \bf X}$
and with final coordinates
x
.