What you want is essentially the Biot-Savart Law.
For a point charge that is moving slowly compared to the speed of light (which is also a condition for the Couloumb law that you give to be true, by the way), Biot-Savart says that a point charge makes a magnetic field like:
$\vec{B}=\frac{\mu_0}{4\pi}q_{1}\vec{v_1}\times\frac{\hat{r}}{r^2}$,
where $\vec{v_1}$ is the velocity of particle 1 and $q_{1}$ is its charge.
Then, the force particle two feels from it is the Lorentz force,
$\vec{F_2}=q_{2}\vec{v_2}\times\vec{B}$,
where $\vec{v_2}$ is its own velocity and $q_{2}$ its charge.
Put them together and you get the magnetic force one particle feels from the other,
$\vec{F_{1 \rightarrow 2}}=\frac{\mu_0 q_{1}q_{2}}{4\pi r^2}\vec{v_2}\times\{\vec{v_1}\times\hat{r}\}$
So it is a force that is very direction-dependent, unlike the other two formula you give: it depends on the velocities of each particle, both directions and magnitudes, as well as how these directions compare to the direction of the line that separates the two particles. For a given combination of these directions and speeds, it falls off as r^2 just like the other two forces.