I'm asked to prove this relation: $$\left [\textbf{A},\textbf{L} \cdot \textbf{B} \right]=-i \hbar \textbf{A} \times \textbf{B} + L_i \left [\textbf{A},B_i \right].$$ Where $\textbf{A}$ and $\textbf{B}$ are vector operators that satisfy $$\left[L_i,A_j \right]=i \hbar A_k\varepsilon_{ijk},$$ and $\textbf{L}$ is the angular momentum operator.
This is easy using $\left[A_k,L_j B_j \right]=L_j \left[A_k, B_j \right]+ \left[A_k, L_j \right]B_j=L_j \left[A_k, B_j \right]-i \hbar A_l\varepsilon_{jkl}Bj$. Then I'm asked to use this relation to show that $$\textbf{r}(\textbf{L} \cdot\textbf{p})-\textbf{p}(\textbf{L} \cdot\textbf{r})=0.$$ Here is where I'm stuck. Setting $\textbf{A}=\textbf{r}$ and $\textbf{B}=\textbf{p}$ I am able to show that $\textbf{r}(\textbf{L} \cdot\textbf{p})-(\textbf{L} \cdot\textbf{p})\textbf{r}=0.$ With $\textbf{B}=\textbf{r}$ and $\textbf{A}=\textbf{p}$ I get $\textbf{p}(\textbf{L} \cdot\textbf{r})-(\textbf{L} \cdot\textbf{r})\textbf{p}=0.$ But this gets me nowhere.
Am I missing something? The formula is similar to an identity involving $\textbf{L} \times (\textbf{r} \times \textbf{p})$. But I think that the result has to be more or less immediate as it is stated as a corollary to the first relation.