Stress and strain are both tensor quantities 59
e = Sa
21 independent
c:E:ts
where E = anda = and S =
It can be shown from energy considerations that the S matrix is symmet-
rical, leading to 21 independent elastic constants.
This number of constants can be reduced if we assume that some of
the strain-stress linkages are not significant. For example, omitting all
shear linkages not on the leading diagonal - which means assuming
that any contributions made by shearing stress components in a given
direction to normal or shear strain components in other directions are
negligible - causes all off-diagonal shear linkages to become zero. The
compliance matrix then reduces to one with nine material properties,
which is the case for an orthotropic material.
]/Ex -v,~/E~ -%Ez^0 0 0
. -... .-..... l/Ey -vyz/&^0 0 0
.... .....
......... ._ ...... ...... 1 /Gxz 0 0
.....
'....- -.., l/Gyz 0
'..,
'...
---......
... 1 /E,
symmetric
where E is a Young's modulus, u is a Poisson's ratio, and G is a shear
modulus.