Corvus wrote:There is one force that herrflick does not have appeared to have considered. Why was the paralever introduced in the first place? Unless my memory deceives me (wouldn't be the first time) it was as an answer to shaft jacking (insert jokes using myleene klaas here). Is that true or not?
So, does the shaft jacking counter force place the link bar under compression or tension when accelerating? As far as I can fathom, it will place it under compression. Is that the reason it was subsequently moved on top? Or am I well and truly barking up the wrong tree?
Anybody actually seen what happens, say on a rolling road?
Et tu Corvè?
Well, ahem koff koff, I have considered compression loading and written about it at length, since compression loads are what cause column buckling.
That's what all the calculations were about: to determine ultimate failure loads and the margin of safety I had with my bits of 'ally'.
A 10x margin as it happens, without including the effects of big isolating rubber bushes. These take the sharp edge off sharp impact loads to the tune of 5x and more.
Now - back to jacking, and other stuff:
R1200 and position of torque arm: I wrote about this too. It was moved up to increase ground clearance and so avoid failure by rock. Seemples.
Why was paralever introduced?
- because with the old swinging shaft (did I just say that?) system, the pinion climbed on the ring gear, which in turn forced the drive shaft to rise and so lift the chassis. The reverse on throttle over-run. Bike rocked like a rocking horse.
- with the second drive joint at the rear wheel (paralever), that rise/fall now takes place around the second joint, without affecting the swing arm position (and the bike attitude).
Back to the R1200: with the overhead torque arm there is now compression under braking and tension under acceleration.
As for shock loading over rough surfaces, intuitively I think it's much of a muchness: ABS off and rear wheel locked as it hits the other edge of that big pothole (and we're not off road yet), will produce severe impact loading on the torque arm: compression for the R1200 and tension for the R11x0.
As I think about this situation, two points come to mind:
- the peak kinetic energy available from an engine to produce wheel spin (over potholes say) is limited to the maximum momentary energy available from that engine.
- by contrast, that same engine, applying that energy input over a longer time, can cumulitively raise the total kinetic energy (high road speed) of the bike/rider system to well beyond the energy available for momentary wheel spin.
Point being that once travelling at high road speed, any braking or brake lock through potholes will produce huge shock loads, and will far exceed the loads produced under acceleration over the same potholes.
In the case of the R1200 these will become compression forces in the stay arm and tensile forcess in the R11x0 stay arm.
As for a rolling road view: well a funny thing happened on my way to the forum: I got his brilliant idea of mounting (ohhh do be quiet) my action cam such that I can record the behaviour of my Heath Robinson creation as I ride. (Won't be long Dear - just dashing out to the garidge for a moment - have you seen my duct tape?

)
('Garidge' is how you Poms pronounce the French 'gar-arrrge'). Love it.
With any luck, those in the Coliseum corporate boxes won't be disappointed.
Did I mention I'm 6'5" tall and my initials are 'JC'. No. Probably not. But they ARE.
Cheers
John C.
PS: once replaced with a GS arm I'm planning a load test (to destruction) of my Heath Robinson torque arm.
I'm quite looking forward to what it will tell Us and of what everyone can learn from it, but unless we experiment and analyse we learn nothing of use for the everyday man. Enough said there.
Real torque curves don't have a first derivative. :-^)