Similarly, we define the following the Poisson’s ratios and as
|
(7.153) |
Thus, using Equation (7.149), we get
|
(7.154) |
The other engineering constants that can be directly related to the effective stiffness coefficients are
|
(7.155) |
Equations (7.152), (7.154) and (7.155) are four equations with five effective stiffness constants. We need one more equation in effective stiffness constants that relates an effective engineering constant. Then we can solve for and in terms of effective engineering constants.
We develop this equation as follows. Let us define the plane strain bulk modulus, corresponding to the state of strain
|
(7.156) |
For this state of strain, from the constitutive equation in Equation (7.148) the normal stresses are given as
|
(7.157) |
Let us define where
|
(7.158) |
is defined as effective plane strain bulk modulus.
Now, Equations (7.152), (7.154), (7.155) and (7.158) can be inverted to give
|
(7.159) |
In the above exercise, the measurable properties are and . However, one can measure the other engineering properties and express the effective stiffness coefficients. Let us consider that a uniaxial tension normal to the fibre direction is applied such that and . Putting this in Equation (7.148) we can solve for the normal strains. The normal strains in terms of and are given as
|
(7.160) |
From the second of the above equation, we can write
|
(7.161) |
|