What you call a split ring is what I call a clamp collar. I have used them many times where I need strong holding force or torque. They work especially well in applications with reversing torque, where a key would hammer loose.
A thick ring with a single screw, such as shown in your figure, must be a snug fit when you slide it on the shaft. If it goes on loose, the screw force is used up bending the ring around the shaft.
The analysis procedure is easier to understand if you start with a two piece clamp collar. Here is an example:
https://www.mcmaster.com/#6436k18/=19n4anv. Imagine that the two ring halves flex enough to mold to the shaft. Then you adapt the equation for a thin wall pressure vessel: 2 * Fscrew = 2 * r * P, where
Fscrew = force from screw
r = radius of shaft
P = pressure between clamp collar and shaft
This simplifies to P = Fscrew / r.
Then the total contact force between the clamp collar (total for both pieces) is: Fcontact = Fscrew / r * 2 * r * pi = Fscrew * 2 * pi, where
Fcontact = total contact force (not pressure) between the clamp collar and shaft
Then the slip force is the contact force times friction coefficient: Fslip = Fcontact * mu, where
Fslip is the force to slide the clamp collar on the shaft.
The slip torque is then Fslip times the shaft radius.
The total contact force is exactly the same for your single piece clamp collar with one screw because tensile stress in the collar opposite the single screw provides the same tension as would a second screw.
The analysis gets tricky if the collar is thick and fits loose. In that case, part of the screw force is used to bend the collar to fit the shaft. That part of the screw force that bends the collar is not used for clamping.