It's quite easy to work out .. Circumference distance in meters = 2 x Pi x radius .. Fc = Cf = Cp = m x a = m x v^2 / r in m/s^2 .. set a radius (in meters) and rpm. Divide rpm by 60 and divide into circumference at a certain radius to find tangential velocity (assuming constant speed). Now you know the acceleration component of the Fc which has a vertical component (using Trig to adjust when not vertical) - offset gravity's acceleration -9,806 m/s^2 by adding the vertical component of the tangential acceleration.eccentrically1 wrote:I think someone did the calculations on this problem in the past. The weights only transitioned under gravity’s influence in the first few turns before they would be merely along for the ride, then at terminal velocity we have to assume gravity had no role. Cf’s would be a problem at terminal velocity. Weights at those speeds would want to be next to the rim, and, ..f wrote: If we take an extreme case of a wheel doing 100 rpm then not only will CF's be effecting the lag but also little time available for a gravity induced transition to occur.
Since B's. one-way wheels did have a good clip then I speculate the transition distances were relatively small, so that the drive could be engaged quicker, and act for longer, time wise.
Sensitivity : increase the radius and rpm until the 2 are zeroed out (using vertical components).
N.B. choose a radius that you think the weights are at. When at 12 o'cl they cancel, when at 6 o'cl they reinforce etc etc.
The noise was heard on the down-going side at all times and was constant. W. proposed that they might be noise makers which B. strenuously denied saying they were an integral part of the motive force and motive power (paraphrased).eccentrically1 wrote:.. Here’s the other problem: at terminal velocity, the weights were still making impacts. IOW, they were still thought to be “ hammering “ the wheel , albeit one at at a time, then “ riding” until their turn came around again. Confusing.
Applying the 'sniff the wind test' I would say that the weights alternating position and changing radius were most likely very close to the axle and therefore much less effected by Cf's, and why the sounds were regular because they were largely unaffected. Unfortunately the witnesses don't say where the noises were thought to be located. We have tended to make assumptions, like, the noises were out by the rim and that "weights" were making an impact noise.
What is known is that something was making an impact noise, but it is not a given in my books that that was transitioning weights, nor that the noise was out in the outer reaches, tho it could well be, imo.