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Using summation convention notation, this may be written as
1 f i
1
+ E σ ij E δ ij σ kk
=
j
ij =
with
δ ij =
0 f i
=
j
and
σ
= σ
+ σ
+ σ
= σ
+ σ
+ σ
(1.33a)
kk
xx
yy
zz
x
y
z
More generally, this is often placed in the form
=
F ijkl σ kl
(1.33b)
ij
6 matrix E 1 .
From Eq. (1.32) [or Eq. (1.33)], the stresses can be found by inversion as functions of
strains
where F ijkl is the index notation form of the 6
×
σ
νν ν.
x
x
1
νν.
σ
y
y
ν
1
0
.
σ
z
z
ν
ν
1
ν
E
...
=
...
...
...
. ...
...
...
...
(1.34a)
(
1
+ ν)(
1
2
ν)
.
1
2
ν
τ xy
00
γ xy
2
.
1
2
ν
0
0
0
τ xz
γ xz
2
.
00 1 2 ν
2
τ yz
γ yz
σ
=
E
(1.34b)
In index notation, this can be written as
E
ν
E
σ ij =
ν) δ ij kk +
+ ν) ij = λδ ij kk +
2
µ ij
(1.35a)
(
1
+ ν)(
1
2
(
1
or
σ ij =
E ijkl kl
(1.35b)
where
λ =
E
ν/
[
(
1
+ ν)(
1
2
ν)
] and
µ =
G
=
E
/
[2
(
1
+ ν)
] are the Lame's 12
constants, and
kk = xx + yy + zz = x + y + z .
It is sometimes convenient, for example, in soil mechanics, to express the material
law in terms of the bulk modulus K . To do so, define the deviatoric stress and strain
components
1
3 σ kk δ ij
σ ij = σ ij
(1.36)
1
3 kk δ ij
ij = ij
12 Gabriel Lame (1795-1870) was a French engineer who, after graduation from the Ecole Polytechnique, worked
at a Russian railroad institute and helped establish a new engineering school in St. Petersburg. He introduced and
applied curvilinear coordinates, and contributed to number theory, applied mechanics, and thermodynamics. In
1852, he co-authored (with Clapeyron) the first topic on the theory of elasticity.
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