For a beam made of two or more materials with different moduli of elasticity, show that Eq. (6.6)
\[
\tau_{\mathrm{ave}}=\frac{V Q}{I t}
\]
remains valid provided that both $Q$ and $I$ are computed by using the transformed section of the beam (see Sec. 4.4 ) and provided further that $t$ is the actual width of the beam where $\tau_{\text {ave }}$ is computed.