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Always interested in offers/projects/new ideas. Eclectic experience in fields like: numerical computing; Python web; Java enterprise; functional languages; GPGPU; SQL databases; etc. Based in Santiago, Chile; telecommute worldwide. CV; email.

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Modelling Bicycle Wheels

From: andrew cooke <andrew@...>

Date: Thu, 13 Oct 2016 10:50:46 -0300

I'm trying to do some simple (2D, simplified physics) modelling of
bicycle wheels.  Unfortunately, it's turning out to be harder than I

The immediate problem is that I am not able to find (efficiently and
reliably) the stable solution.  It seems that my equations for forces
and energy are correct, because occasionally a solution converges.
The difficulty is "numerical" in some sense.

I can think of three problems:

- Local forces

  I calculate the force at each "spoke hole" as the sum of three
  components - the spoke (in tension, connected to the fixed hub), and
  the two rim segments (in compression, spanning to adjacent holes).
  The simplified physics assumes a "hinge" at each hole.

  This sounds fairly reasonable (in particular, I have a Jobst quote
  somewhere supporting the hinge model), except that it assumes that
  the rim segment endpoints are in equilibrium.  In fact there may be
  net forces there (when not at equilibrium) which are "passed along"
  and also affect the hole under examination.

  I don't see any way to avoid this.  It's the ugly compromise one
  gets when finding a static solution to a system that would go
  through some dynamic evolution.  Ideally you would model the entire
  dynamics.  Instead, you iterate the static minimisation.  But some
  of the (GSL) minimisation routines I am using seem to handle this

- Local movement

  I describe the system as a collection of (x,y) coordinates of the
  holes (spoke end points).  So a simple physical action like
  contracting the rim inwards in response to spoke tension involves
  altering all the variables.

  I am not sure this is a problem for methods that use a matrix-based
  solution (since the solution can move multiple points), but it seems
  like it could seriously affect simplex minimisation.

  Instead, I could use some kind of Fourier scheme where zeroth order
  is a constant radial shift, etc etc.  The problem here is that it
  seems to make calculating derivatives much more expensive (although
  derivatives are not needed for simplex).

- Unstable collapse

  The hinge model assumes that the rim segments always have an
  internal (hub facing) angle less than 180 degrees.  If this is
  exceeded then the wheel becomes unstable and collapses.

  This may be a source of instabilities in the solution when an
  additional force is applied.  It would be useful to have some kind
  of minimisation that could easily detect this condition.

Given that I am currently stalled it seems like I have two options.  I
can implement the Fourier based approach (second above) or try to do
some kind of customized solution "by hand".

A hand-rolled approach could deal with item 1 above by using an
iterative alorithm (quasi-dynamic).  It could also handle the third
point if it used calculations tailored exactly to the configuration

So I could calculate the approximate solution for each hole in
isolation as a pair of 1D roots (zero force perpendicular and parallel
to the chord from neighbouring holes).  This would be quick and allow
detection of the instability.  By moving the hole only a fraction of
the distance to the solution and then iterating the entire wheel I
would move towards a consistent solution.


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