Generally, the stresses are uniform in the fibre and matrix. Thus above equation reduces to
|
(7.37) |
Further, for equilibrium in transverse direction, we have
|
(7.38) |
The axial and transverse strains in fibre and matrix are
|
(7.39) |
Using Equations (7.34) and (7.39) in (7.37), we get
|
(7.40) |
Further, using Equation (7.34) in Equation (7.38), we get
|
(7.41) |
We solve Equations (7.40) and (7.41) for , and . The transverse composite strain then is obtained as
|
(7.42) |
Finally, putting the values of and in the above equation, we get an expression for as
|
(7.43) |
where,
|
(7.44) |
Equation (7.43) is an alternate equation for effective transverse modulus . This is also a rule of mixtures equations. It should be noted that the factors and are the nondimensional factors. |