First of all, you have to define the parameters of your problem. Let's use cylindrical coordinates, using the base $(\mathbf{e}_z, \mathbf{e}_r, \mathbf{e}_\theta)$, where $\mathbf{e}_z$ is the axis of rotation.There is an inertial frame of reference $\mathcal{R}_0$, and another one $\mathcal{R}$ which rotates with and angular velocity $\mathbf{\omega} = \omega \mathbf{e}_z$ around $\mathcal{R}_0$, where $\omega = 5\,\textrm{rpm}$. Now, we are studying an object moving with a velocity $\mathbf{v} = -v\mathbf{e}_r$ where $v =10\,\textrm{m/s}$.
Now, you have to use the formula giving the Coriolis acceleration: $\mathbf{a}_c = -2\mathbf{\omega}\times\mathbf{v}$. To find the acceleration, you must find the cross product of two vectors. First of all, you can use the bilinearity of the cross product, ie. the fact that it behaves like a normal multiplication, except that it is not symmetric:
$$(\omega \mathbf{e}_z) \times (-v\mathbf{e}_r) = -\omega v (\mathbf{e}_z \times\mathbf{e}_r)$$
Finally, the cross product of two base vectors can be found easily: use the right-hand rule. Here, $\mathbf{e}_z$ is represented by your middle finger, $\mathbf{e}_z$ by your thumb, so their cross product (in this order) gives your forefinger, that is $\mathbf{e}_\theta$.