I was idly considering knife edges when it occured to me that a cylinder on two parallel knives would represent a circle rolling on a plane – almost the perfect description of a cycloid. I imagine this has been looked into before. Any suggestions where to look? The pic is just the general idea, but with the knives under the "pivots" to reduce rolling.(please view with bob at the bottom)
This has been analysed by Philip Woodward but alas doesn't result in isochronism. I could dig out the reference if interested.
Thanks for the offer John, but I can now see that the correction should be a proportion of the pendulum length. In my idea, the correction would be in proportion to the roller radius, thus incorrect.
Well for completeness it was in HJ August and September 1994.
Intriguingly, he shows that if the roller rolled below a flat rolling surface it could work. Very strong magnets might do the trick, but then the rest of the pendulum would have to be non-magnetic to avoid magnetic forces interfering with gravitational.
The actual locus of the bob is a "prolate trochoid", not a cycloid. Woodward shows that the radius of curvature of this for small angles is greater than the circular path of the bob with no roller. This means that the "lift" of the bob for a given deflection is less than for a circle, whereas for a true cycloidal path it would be greater. In fact the circular deviation of a pendulum with roller suspension is greater rather than less than normal. Others have confirmed this numerically. Unless one could hang the roller on a magnet this means that there's no point in roller suspensions in an attempt to reduce circular deviation.
Another point is that for compound pendulums (which all real pendulums are to a greater or lesser extent), it can be shown that there is no path the bob could follow that will be isochronous. There are some schemes to correct for circular deviation over a small range of angles, of which the most successful was probably the Fedchenko suspension spring. Or one can try to control CD to gain other benefits which is what Harrison's circular cheeks do.
John, yes I can see that. I was viewing it as a "negative cycloid" But I was questioning Michaels assertion that the roller size mattered. I am experimenting with magnets.
Hopefully, this will help with visuslising the problem with mounting the roller above the support plate. The two cycloids (inverted for clarity) represent a point on the underside of the roller and therefore the pendulum bob With the rod above the plate we get "A" With it below, we get "B"
dave8
p.s. can our helpful moderator turn the image olease?
A first quick and dirty try. The rod is 840mm by 3mm. The magnets and coins are as shown earlier. There is a good rolling action, but the rod is much to thin and long, allowing too much error in the bob (figure of eight) The amplitude falls from 90mm to 45mm in about two minutes. Such a terrible Q is not surprising, considering the work the pendulum has to do, and the rolling surfaces are so far unmachined. The magnets are very strong, and would hold a much heavier bob.
I'm having trouble conceiving how it works. Presumably low Q is caused by friction between coins and top-plate resulting from the magnetic force. I wonder if Q could be improved by increasing bob weight until gravitational force almost balances the magnetic force.
I'm guessing friction follows the same rules whatever type of force brings two moving objects into contact. Does anyone know?
Dave, don't let the coins fool you. They are the modern 2p coins that contaiin iron. As it is a rolling action, it doesn't feel frictiony. It should improve when the coins are replaced by chamfered discs to mimic knife-edges. Bear in mind the rolling action means the effort to physically lift the bob must come from the pendulum. I have ordered some differen sized magnets to hopefully tune the attraction. Also, a half second-sized rod might be better.
To be clear, there is only one cycloidal path that makes the pendulum isochronous and that's one where the roller radius (or diameter?) equals the pendulum length. Anything else just approximates the cycloid for small angles in a way that can correct the isochronism. Anyway the path of the bob for this setup is epi-trochoidal. As far as I know everyone who has looked at this (mainly Woodward) just assumed that the magnetic version would be impracticable and the calculations of the required roller diameter haven't been done, you're pioneering here Dave! Also one would have to factor in that real pendulums are compound just to make it more interesting.
To be clear, there is only one cycloidal path that makes the pendulum isochronous and that's one where the roller radius (or diameter?) equals the pendulum length. […]