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It’s worth looking into this ‘loop factor’ in a little more depth. It’s a bit of a sidetrack but it does affect steering to some degree (under power).
The natural tendency of a vehicle under acceleration is to ‘squat down’ on the rear suspension due partly to the change in weight distribution since the vehicle’s C of G is considerably above the horizontal driving force. Thus it creates that ‘squat’.
We might assume that the drive force acts where the rubber hits the road, but it actually acts on a bike horizontally through the rear axle. And since the pull of the chain also has an effect, depending on the geometry of the swingarm & chain-sprocket set-up, the drive force can (& often does) produce a torque that extends the rear suspension. Since this is counter to the squat effect, it is understandably called anti-squat (or more correctly, anti-squat torque).
Apart from engine HP & grip on the road (eg sticky tyre, grippy surface, or otherwise) there are numerous variables that affect it: ie front & rear sprocket diameter, swingarm pivot position, swingarm angle & front sprocket position. The diag below ‘reveals all’.
When it all boils down in the geometry, it all depends on the dimensions 'a' and 'b'. They are the most critical. (In a sense the length and angle of the swingarm are irrelevant. What counts is the distance 'b'.)

- Chain Torque JPG.JPG (14.08 KiB) Viewed 7839 times
You can see that the chain pull force ‘F1’ acting at a distance ‘a’ from the pivot produces an anti-clockwise torque (F1 a) compressing the suspension (ie squat torque) & will be greatest on full compression when ‘a’ is maximum. But the thrust force ‘F’ (ie drive force) acting at a distance ‘b’ from the pivot produces a clockwise torque (F b) extending the rear suspension (ie anti-squat torque) & will be greatest at full extension when ‘b’ is maximum.
Now
it’s the overall resultant that is important. When F b > F1 a, the overall nett effect is anti-squat torque (Fb – F1a), but when F1 a > F b the overall nett effect is squat.
It is effectively an over-centre mechanism. At some point of suspension compression on most bikes the anti-squat torque (Fb) is going to be zero. That happens when b=0, ie when the swingarm is horizontal. But what happens to it on further compression? It becomes an additional squat torque added to that of the chain-pull squat torque.
Apart from ‘a’ & ‘b’ changing as the suspension is compressed, they are also dependant on the sprocket diameters & the height of the swingarm pivot relative to the front sprocket & rear axle. That’s why the pivot location is critical to squat/anti-squat (& why some factory GP bikes have adjustable pivot locations for diff gearing combinations, track/tyre/stickiness, suspension settings etc).
If you get the pivot too high you get too much anti-squat, thereby worsening the ‘loop factor’ by raising the C of G as the suspension extends under power, & also stiffening the rear suspension under power. But if you get it too low you get excessive squat & soften the rear suspension under power. (In fact on high powered bikes you tend to pull the tyre off the track & cause excessive wheelspin.)
Now as long as ‘b’ > 0 (ie the rear axle is below the swingarm pivot) there is going to be some anti-squat torque produced under power even though it reduces towards zero as the swingarm approaches horizontal.
Going back to the RL, it seems that its swingarm is not horizontal until the rear suspension is almost bottomed!

- RL250_Jap_front 75.jpg (70.56 KiB) Viewed 7839 times
Add to that the RL’s ‘frisky’ engine & you can see why the high swingarm pivot potentially has such importance/effect. (You can also see that running longer shocks is likely to make the loop factor doubly worse, by both raising the C of G directly & increasing the anti-squat effect.).
While having some anti-squat torque still produced at/near full compression is not necessarily a problem in itself (since it’s the nett effect that matters), it probably does indicate that the RL has excessive anti-squat at laden ride height, raising the C of G & tendency to loop under power.
Apart from lowering the swingarm pivot, one could overcome it somewhat with shorter/softer shocks (which unfortunately also lowers ground clearance & slows the steering) or with a roller under the top chain-run to raise it a little further above the swingarm pivot, thus increasing ‘a’ (in Fig 5.15 above) & hence also the pro-squat torque, to overcome more of that anti-squat.
By contrast to the RL, look at this pic of a Greeves Pathfinder. The Puch engine has a very low countershaft sprocket, meaning the swingarm is almost horizontal, even unladen.

- Greeves Pathfinder 2.jpg (187.29 KiB) Viewed 7839 times
That’s going to produce very little anti-squat even unladen at full extension of the suspension. In fact I wouldn’t be surprised if there was noticeable squat under power even with only a very light rider on board (ie with minimal laden sag).