]> https://gitweb.dealii.org/ - dealii.git/commitdiff
Fix equation 9557/head
authorDaniel Garcia-Sanchez <daniel.garcia-sanchez@insp.upmc.fr>
Fri, 21 Feb 2020 17:36:50 +0000 (18:36 +0100)
committerDaniel Garcia-Sanchez <daniel.garcia-sanchez@insp.upmc.fr>
Fri, 21 Feb 2020 17:36:50 +0000 (18:36 +0100)
The equation \partial_j (c_{ijkl} \partial_k u_l) is only valid if c_{ijkl} = c_{ijlk}

examples/step-8/doc/intro.dox

index 5e538797e25c7622aa1afc2b21a15cc0e755ef5f..a982951eea68c0b3d69a04e7d49255b28eb318fa 100644 (file)
@@ -20,15 +20,21 @@ vector-valued, meaning that in each point it has a direction and an
 absolute value. The elastic equations are the following:
 @f[
   -
-  \partial_j (c_{ijkl} \partial_k u_l)
+  \partial_j (c_{ijkl} \varepsilon_{kl})
   =
   f_i,
   \qquad
   i=1\ldots d,
 @f]
-where the values $c_{ijkl}$ are the stiffness coefficients and
-will usually depend on the space coordinates. In
-many cases, one knows that the material under consideration is
+where the values $c_{ijkl}$ are the stiffness coefficients that
+usually depend on the space coordinates and the strain $\varepsilon_{kl}$ is
+the symmetrized gradient of the displacement,
+given by
+@f[
+\varepsilon_{kl} =\frac{1}{2}(\partial_k u_l + \partial_l u_k)
+@f]
+
+In many cases, one knows that the material under consideration is
 isotropic, in which case by introduction of the two coefficients
 $\lambda$ and $\mu$ the coefficient tensor reduces to
 @f[

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