Here is my feeble attempt:
$$ \begin{equation}\begin{aligned} \nabla .({\bf T}^T {\bf v}) & = \frac{\partial {\bf T}_{ji}}{\partial x_j} {\bf v}_i + {\bf T}_{ji} \frac{\partial {\bf v}_{i}}{\partial x_j} \\ & = (\nabla . {\bf T}^T) \cdot {\bf v} + {\bf T}^T \, \nabla {\bf v} \end{aligned}\end{equation} \\ $$
Source: page 2 of these lecture notes.
It's a matter of unwrapping the definitions very carefully. Even if you are already familiar with the objects, it is always convenient to go back to the definitions because different authors have conflicting conventions and this often results in different formulas.
From module 1 lecture 4, we have $R:S=R_{ij}S_{ij}$.
Also $Te_j=T_{ij}e_i$, so $$Tv={\textstyle\sum}Te_jv_j={\textstyle\sum}T_{ij}e_iv_j,$$ This means the components of $Tv$ are given by $(Tv)_i=T_{ij}v_j$. Thus we have $(T^tv)_i=T_{ji}v_j$.
From module 2 lecture 2, we have
Puting all of this together, we have $$\begin{aligned} \nabla \cdot (T^tv) &= \partial_i(T^tv)_i \\ &=\partial_i(T_{ji}v_j) \\ &=\partial_iT_{ji}v_j+T_{ji}\partial_iv_j \\ &=(\nabla\cdot T)_jv_j+T_{ji}(\nabla v)_{ji} \\ &=(\nabla\cdot T)\cdot v+T :\nabla v \end{aligned}$$
as you wanted. Hope this helps.