We define
![](images/image010.gif) |
(5.34) |
We make a note that and we can write
Using the above definitions, Equation (5.32) and Equation (5.33) can be written together as
![](images/image013.gif) |
(5.35) |
The above equation is called as partially inverted constitutive equation for laminate. From the second of the above equation we write
![](images/image014.gif) |
(5.36) |
Putting this in Equation (5.35) we can get for as
![](images/image016.gif) |
(5.37) |
Let us define
![](images/image017.gif) |
(5.38) |
Combining Equations (5.37) and (5.36) and using the definitions in Equation (5.38), we can write
![](images/image018.gif) |
(5.39) |
This equation is the fully inverted form of laminate constitutive equation. Using Equation (5.34) in Equation (5.38) we can write the above equation in terms of A, B and D matrices as
![](images/image019.gif) |
(5.40) |
From this equation it is easy to deduce that
![](images/image020.gif) |
(5.41) |
The full matrix is symmetric. This also follows from the fact that this is an inverse of a symmetric matrix, that is , and the inverse of a symmetric matrix is also a symmetric matrix.
Equation (5.28) and Equation (5.39) are very important equations in laminate analysis. These equations relate the mid-plane strains and curvatures with resultant in-plane forces and moments and vice versa. |