We can use the back-cab rule as following$$\mathbf{F}_{centrifugal} = -m \boldsymbol{\omega} \times [\boldsymbol{\omega} \times \mathbf{r}]=-m((\boldsymbol{\omega}\cdot\boldsymbol{r})\boldsymbol{\omega}-|\boldsymbol{\omega}|^2\boldsymbol{r})=m|\boldsymbol{\omega}|^2r-m(\boldsymbol{r}\cdot \boldsymbol{\omega})\boldsymbol{\omega}$$