Civil Engineering Reference
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For a proof, see Duvaut and Lions [1976], Nitsche [1981], or the end of this §.
Its structure is similar to the proof that the divergence satisfies an inf-sup condition
as a mapping of H 1 () d into L 2 () ; cf. Ch. III, §6. A special case in which the
inequality can be easily verified is dealt with in Remark 3.5 below.
3.2 Remark. If the strain tensor E of a deformation is trivial, then by Remark 1.1
the deformation is an affine distance-preserving transformation. An analogous as-
sertion holds for the linearized strain tensor ε : Let ⊂ R
3 be open and connected.
Then for v H 1 (),
ε(v)
=
0 ,
if and only if
3 .
v(x) = a x + b
with a, b ∈ R
( 3 . 16 )
For the proof, we note that
2
∂x i ∂x j v k =
∂x i ε jk +
∂x j ε ik
∂x k ε ij =
0
( 3 . 17 )
in H 1 () if ε(v) =
0. From this we conclude that every component v k must be
a linear function. But then a simple computation shows that a displacement of the
form v(x) = Ax + b can only be compatible with ε(v) =
0if A is skew-symmetric.
This leads to (3.16).
On the other hand, it is easy to verify that the linear strains for the displace-
ments of the form (3.16) vanish.
Korn's inequality is simplified for functions which satisfy a zero boundary
condition. In the sense of Remark II.1.6, it is only necessary that v vanishes on
a part 0 of the boundary, and that 0 possesses a positive (n
1 ) -dimensional
measure.
3 be an open bounded
set with piecewise smooth boundary. In addition, suppose 0 ∂ has positive
two-dimensional measure. Then there exists a positive number c = c (, 0 ) such
that
3.3 Korn's Inequality (Korn's second inequality). Let ⊂ R
ε(v) : ε(v)dx c v
2
1
for all v H 1 ().
( 3 . 18 )
Here H 1 () is the closure of
{ v C () 3
; v(x) =
0 for x 0 }
w.r.t. the
· 1 -norm.
Proof. Suppose that the inequality is false. Then there exists a sequence (v n )
H 1 () with
ε(v n ) : ε(v n )dx
1
n
2
ε(v n )
0 :
=
and
| v n | 1 =
1 .
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